2.20.67 INTRODUCTORY DIFFERENTIAL EQUATIONS. Martha L. Abell, James P. Braselton. Fourth edition 2014. ElScAe. 2014

Column notations: A is ODE degree. B is Program Number of solutions generated. C is CAS Number of solutions generated.

Table 2.512: INTRODUCTORY DIFFERENTIAL EQUATIONS. Martha L. Abell, James P. Braselton. Fourth edition 2014. ElScAe. 2014










#

ODE

A

B

C

Program classification

CAS classification

Solved?

Verified?

time (sec)











14044

\[ {}y^{\prime \prime }+y^{\prime }-2 y = x^{3} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.791











14045

\[ {}y y^{\prime }+y^{4} = \sin \left (x \right ) \]

1

0

2

unknown

[‘y=_G(x,y’)‘]

N/A

2.337











14046

\[ {}y^{\prime \prime \prime }-2 y^{\prime \prime }+5 y^{\prime }+y = {\mathrm e}^{x} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _with_linear_symmetries]]

68.348











14047

\[ {}{y^{\prime }}^{2}+y = 0 \]

2

2

2

quadrature

[_quadrature]

1.197











14048

\[ {}t^{2} y^{\prime \prime }+t y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.947











14049

\[ {}x {y^{\prime \prime }}^{2}+2 y = 2 x \]

2

0

2

unknown

[[_2nd_order, _with_linear_symmetries]]

N/A

0.493











14050

\[ {}x^{\prime \prime }+2 \sin \left (x\right ) = \sin \left (2 t \right ) \]

1

0

0

unknown

[NONE]

N/A

1.274











14051

\[ {}2 x -1-y^{\prime } = 0 \]

1

1

1

quadrature

[_quadrature]

0.236











14052

\[ {}2 x -y-y y^{\prime } = 0 \]

1

1

9

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

4.731











14053

\[ {}y^{\prime }+2 y = 0 \]

1

1

1

quadrature

[_quadrature]

0.618











14054

\[ {}y^{\prime }+x y = 0 \]

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.553











14055

\[ {}y^{\prime }+y = \sin \left (x \right ) \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.62











14056

\[ {}y^{\prime \prime }-y^{\prime }-12 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.431











14057

\[ {}y^{\prime \prime }+9 y^{\prime } = 0 \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.816











14058

\[ {}x^{\prime \prime }+2 x^{\prime }-10 x = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.527











14059

\[ {}x^{\prime \prime }+x = t \cos \left (t \right )-\cos \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.711











14060

\[ {}y^{\prime \prime }-12 y^{\prime }+40 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.954











14061

\[ {}y^{\prime \prime \prime }-4 y^{\prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.353











14062

\[ {}y^{\prime \prime \prime }-2 y^{\prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.351











14063

\[ {}x^{2} y^{\prime \prime }-12 x y^{\prime }+42 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_1, second_order_change_of_variable_on_y_method_2, linear_second_order_ode_solved_by_an_integrating_factor

[[_Emden, _Fowler]]

2.977











14064

\[ {}t^{2} y^{\prime \prime }+3 t y^{\prime }+5 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.825











14065

\[ {}y^{\prime } = -\frac {x}{y} \]

1

1

2

exact, separable, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

2.871











14066

\[ {}3 y \left (t^{2}+y\right )+t \left (t^{2}+6 y\right ) y^{\prime } = 0 \]

1

1

2

exact, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class G‘], _exact, _rational, [_Abel, ‘2nd type‘, ‘class B‘]]

4.441











14067

\[ {}y^{\prime } = -\frac {2 y}{x}-3 \]

1

1

1

linear, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

2.029











14068

\[ {}y \cos \left (t \right )+\left (2 y+\sin \left (t \right )\right ) y^{\prime } = 0 \]

1

1

2

exact

[_exact, [_1st_order, ‘_with_symmetry_[F(x),G(y)]‘], [_Abel, ‘2nd type‘, ‘class A‘]]

3.627











14069

\[ {}\frac {y}{x}+\cos \left (y\right )+\left (\ln \left (x \right )-x \sin \left (y\right )\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact]

5.138











14070

\[ {}y^{\prime } = \left (x^{2}-1\right ) \left (x^{3}-3 x \right )^{3} \]

1

1

1

quadrature

[_quadrature]

0.47











14071

\[ {}y^{\prime } = x \sin \left (x^{2}\right ) \]

1

1

1

quadrature

[_quadrature]

1.158











14072

\[ {}y^{\prime } = \frac {x}{\sqrt {x^{2}-16}} \]

1

1

1

quadrature

[_quadrature]

0.473











14073

\[ {}y^{\prime } = \frac {1}{x \ln \left (x \right )} \]

1

1

1

quadrature

[_quadrature]

0.248











14074

\[ {}y^{\prime } = x \ln \left (x \right ) \]

1

1

1

quadrature

[_quadrature]

0.255











14075

\[ {}y^{\prime } = x \,{\mathrm e}^{-x} \]

1

1

1

quadrature

[_quadrature]

0.314











14076

\[ {}y^{\prime } = \frac {-2 x -10}{\left (2+x \right ) \left (x -4\right )} \]

1

1

1

quadrature

[_quadrature]

0.416











14077

\[ {}y^{\prime } = \frac {-x^{2}+x}{\left (1+x \right ) \left (x^{2}+1\right )} \]

1

1

1

quadrature

[_quadrature]

0.508











14078

\[ {}y^{\prime } = \frac {\sqrt {x^{2}-16}}{x} \]

1

1

1

quadrature

[_quadrature]

0.862











14079

\[ {}y^{\prime } = \left (-x^{2}+4\right )^{\frac {3}{2}} \]

1

1

1

quadrature

[_quadrature]

1.289











14080

\[ {}y^{\prime } = \frac {1}{x^{2}-16} \]

1

1

1

quadrature

[_quadrature]

0.33











14081

\[ {}y^{\prime } = \cos \left (x \right ) \cot \left (x \right ) \]

1

1

1

quadrature

[_quadrature]

1.217











14082

\[ {}y^{\prime } = \sin \left (x \right )^{3} \tan \left (x \right ) \]

1

1

1

quadrature

[_quadrature]

2.884











14083

\[ {}y^{\prime }+2 y = 0 \]

i.c.

1

1

1

quadrature

[_quadrature]

0.752











14084

\[ {}y^{\prime }+y = \sin \left (t \right ) \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

2.041











14085

\[ {}y^{\prime \prime }-y^{\prime }-12 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.905











14086

\[ {}y^{\prime \prime }+9 y^{\prime } = 0 \]

i.c.

1

0

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

2.472











14087

\[ {}y^{\prime \prime \prime }-2 y^{\prime \prime } = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.709











14088

\[ {}y^{\prime \prime \prime }-4 y^{\prime } = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.779











14089

\[ {}t^{2} y^{\prime \prime }-12 t y^{\prime }+42 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_1, second_order_change_of_variable_on_y_method_2, linear_second_order_ode_solved_by_an_integrating_factor

[[_Emden, _Fowler]]

4.648











14090

\[ {}x^{2} y^{\prime \prime }+3 x y^{\prime }+5 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

5.391











14091

\[ {}y^{\prime } = 4 x^{3}-x +2 \]

i.c.

1

1

1

quadrature

[_quadrature]

0.502











14092

\[ {}y^{\prime } = \sin \left (2 t \right )-\cos \left (2 t \right ) \]

i.c.

1

1

1

quadrature

[_quadrature]

1.24











14093

\[ {}y^{\prime } = \frac {\cos \left (\frac {1}{x}\right )}{x^{2}} \]

i.c.

1

1

1

quadrature

[_quadrature]

1.26











14094

\[ {}y^{\prime } = \frac {\ln \left (x \right )}{x} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.608











14095

\[ {}y^{\prime } = \frac {\left (x -4\right ) y^{3}}{x^{3} \left (y-2\right )} \]

1

1

2

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.083











14096

\[ {}y^{\prime } = \frac {y^{2}+2 x y}{x^{2}} \]

1

1

1

riccati, bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _rational, _Bernoulli]

1.803











14097

\[ {}x y^{\prime }+y = \cos \left (x \right ) \]

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

1.547











14098

\[ {}16 y^{\prime \prime }+24 y^{\prime }+153 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.883











14099

\[ {}\left [\begin {array}{c} x^{\prime }=4 y \\ y^{\prime }=-x-2 y \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

1.799











14100

\[ {}4 x \left (x^{2}+y^{2}\right )-5 y+4 y \left (x^{2}+y^{2}-5 x \right ) y^{\prime } = 0 \]

1

0

0

unknown

[_rational]

N/A

31.028











14101

\[ {}y^{\prime } = \sin \left (x \right )^{4} \]

i.c.

1

1

1

quadrature

[_quadrature]

2.008











14102

\[ {}y^{\prime \prime \prime \prime }+\frac {25 y^{\prime \prime }}{2}-5 y^{\prime }+\frac {629 y}{16} = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

2.489











14103

\[ {}\left [\begin {array}{c} x^{\prime }=4 y \\ y^{\prime }=-4 x \end {array}\right ] \]

i.c.

1

1

2

system of linear ODEs

system of linear ODEs

0.619











14104

\[ {}\left [\begin {array}{c} x^{\prime }=-5 x+4 y \\ y^{\prime }=2 x+2 y \end {array}\right ] \]

i.c.

1

1

2

system of linear ODEs

system of linear ODEs

0.734











14105

\[ {}y^{\prime }+y \cos \left (x \right ) = 0 \]

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.975











14106

\[ {}y^{\prime }-y = \sin \left (x \right ) \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.642











14107

\[ {}y^{\prime \prime }+4 y^{\prime }-5 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.43











14108

\[ {}y^{\prime \prime }-6 y^{\prime }+45 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.921











14109

\[ {}x^{2} y^{\prime \prime }-x y^{\prime }-16 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

5.091











14110

\[ {}x^{2} y^{\prime \prime }+3 x y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.804











14111

\[ {}y^{\prime \prime }+2 y^{\prime }+2 y = x \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

1.148











14112

\[ {}y^{\prime \prime }-7 y^{\prime }+12 y = 2 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.668











14113

\[ {}2 x -3 y+\left (2 y-3 x \right ) y^{\prime } = 0 \]

1

1

2

exact, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _exact, _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

3.77











14114

\[ {}y \cos \left (x y\right )+\sin \left (x \right )+x \cos \left (x y\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact, [_1st_order, ‘_with_symmetry_[F(x),G(x)*y+H(x)]‘]]

9.581











14115

\[ {}y^{\prime } = x \,{\mathrm e}^{-x^{2}} \]

1

1

1

quadrature

[_quadrature]

0.276











14116

\[ {}y^{\prime } = x^{2} \sin \left (x \right ) \]

1

1

1

quadrature

[_quadrature]

0.842











14117

\[ {}y^{\prime } = \frac {2 x^{2}-x +1}{\left (-1+x \right ) \left (x^{2}+1\right )} \]

1

1

1

quadrature

[_quadrature]

0.423











14118

\[ {}y^{\prime } = \frac {x^{2}}{\sqrt {x^{2}-1}} \]

1

1

1

quadrature

[_quadrature]

0.605











14119

\[ {}y^{\prime }+2 y = x^{2} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.708











14120

\[ {}y^{\prime \prime }+4 y = t \]

i.c.

1

0

0

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

N/A

1.134











14121

\[ {}x^{2} y^{\prime \prime }+5 x y^{\prime }+4 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

3.826











14122

\[ {}y^{\prime } = \cos \left (x \right )^{2} \sin \left (x \right ) \]

i.c.

1

1

1

quadrature

[_quadrature]

1.403











14123

\[ {}y^{\prime } = \frac {4 x -9}{3 \left (x -3\right )^{\frac {2}{3}}} \]

i.c.

1

1

1

quadrature

[_quadrature]

1.024











14124

\[ {}y^{\prime }+t^{2} = y^{2} \]

i.c.

1

0

1

riccati

[_Riccati]

N/A

3.217











14125

\[ {}y^{\prime }+t^{2} = \frac {1}{y^{2}} \]

i.c.

1

0

0

unknown

[_rational]

N/A

1.046











14126

\[ {}y^{\prime } = y+\frac {1}{1-t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.396











14127

\[ {}y^{\prime } = y^{\frac {1}{5}} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.817











14128

\[ {}\frac {y^{\prime }}{t} = \sqrt {y} \]

i.c.

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.411











14129

\[ {}y^{\prime } = 4 t^{2}-t y^{2} \]

i.c.

1

1

1

riccati

[_Riccati]

9.375











14130

\[ {}y^{\prime } = y \sqrt {t} \]

i.c.

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

2.45











14131

\[ {}y^{\prime } = 6 y^{\frac {2}{3}} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.816











14132

\[ {}y^{\prime } = \sin \left (y\right )-\cos \left (t \right ) \]

i.c.

1

0

0

unknown

[‘y=_G(x,y’)‘]

N/A

2.324











14133

\[ {}t y^{\prime } = y \]

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.45











14134

\[ {}y^{\prime } = y \tan \left (t \right ) \]

i.c.

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

3.138











14135

\[ {}y^{\prime } = \frac {1}{t^{2}+1} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.68











14136

\[ {}y^{\prime } = \sqrt {y^{2}-1} \]

i.c.

1

1

1

quadrature

[_quadrature]

2.811











14137

\[ {}y^{\prime } = \sqrt {y^{2}-1} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.481











14138

\[ {}y^{\prime } = \sqrt {y^{2}-1} \]

i.c.

1

1

1

quadrature

[_quadrature]

4.001











14139

\[ {}y^{\prime } = \sqrt {y^{2}-1} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.434











14140

\[ {}y^{\prime } = \sqrt {25-y^{2}} \]

i.c.

1

1

1

quadrature

[_quadrature]

2.458











14141

\[ {}y^{\prime } = \sqrt {25-y^{2}} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.438











14142

\[ {}y^{\prime } = \sqrt {25-y^{2}} \]

i.c.

1

1

1

quadrature

[_quadrature]

3.124











14143

\[ {}y^{\prime } = \sqrt {25-y^{2}} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.451











14144

\[ {}t y^{\prime }+y = t^{3} \]

i.c.

1

1

1

exact, linear, differentialType, first_order_ode_lie_symmetry_lookup

[_linear]

2.257











14145

\[ {}t^{3} y^{\prime }+t^{4} y = 2 t^{3} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

2.265











14146

\[ {}2 y^{\prime }+t y = \ln \left (t \right ) \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

5.365











14147

\[ {}y^{\prime }+y \sec \left (t \right ) = t \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

5.944











14148

\[ {}y^{\prime }+\frac {y}{t -3} = \frac {1}{-1+t} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.927











14149

\[ {}\left (t -2\right ) y^{\prime }+\left (t^{2}-4\right ) y = \frac {1}{2+t} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

8.855











14150

\[ {}y^{\prime }+\frac {y}{\sqrt {-t^{2}+4}} = t \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

5.844











14151

\[ {}y^{\prime }+\frac {y}{\sqrt {-t^{2}+4}} = t \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

7.891











14152

\[ {}t y^{\prime }+y = t \sin \left (t \right ) \]

i.c.

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

2.056











14153

\[ {}y^{\prime }+y \tan \left (t \right ) = \sin \left (t \right ) \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

2.844











14154

\[ {}y^{\prime } = y^{2} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.44











14155

\[ {}y^{\prime } = t y^{2} \]

i.c.

1

1

1

exact, riccati, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.537











14156

\[ {}y^{\prime } = -\frac {t}{y} \]

i.c.

1

1

1

exact, separable, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

20.007











14157

\[ {}y^{\prime } = -y^{3} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.509











14158

\[ {}y^{\prime } = \frac {x}{y^{2}} \]

1

1

3

exact, separable, differentialType, first_order_ode_lie_symmetry_lookup

[_separable]

6.905











14159

\[ {}\frac {1}{2 \sqrt {t}}+y^{2} y^{\prime } = 0 \]

1

1

3

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.367











14160

\[ {}y^{\prime } = \frac {\sqrt {y}}{x^{2}} \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.974











14161

\[ {}y^{\prime } = \frac {1+y^{2}}{y} \]

1

2

2

quadrature

[_quadrature]

0.663











14162

\[ {}6+4 t^{3}+\left (5+\frac {9}{y^{8}}\right ) y^{\prime } = 0 \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.216











14163

\[ {}\frac {6}{t^{9}}-\frac {6}{t^{3}}+t^{7}+\left (9+\frac {1}{s^{2}}-4 s^{8}\right ) s^{\prime } = 0 \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.842











14164

\[ {}4 \sinh \left (4 y\right ) y^{\prime } = 6 \cosh \left (3 x \right ) \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

7.496











14165

\[ {}y^{\prime } = \frac {y+1}{t +1} \]

1

1

1

exact, linear, separable, homogeneousTypeD2, homogeneousTypeMapleC, first_order_ode_lie_symmetry_lookup

[_separable]

1.514











14166

\[ {}y^{\prime } = \frac {y+2}{1+2 t} \]

1

1

1

exact, linear, separable, homogeneousTypeMapleC, first_order_ode_lie_symmetry_lookup

[_separable]

2.882











14167

\[ {}\frac {3}{t^{2}} = \left (\frac {1}{\sqrt {y}}+\sqrt {y}\right ) y^{\prime } \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.525











14168

\[ {}3 \sin \left (x \right )-4 \cos \left (y\right ) y^{\prime } = 0 \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.569











14169

\[ {}\cos \left (y\right ) y^{\prime } = 8 \sin \left (8 t \right ) \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.514











14170

\[ {}y^{\prime }+k y = 0 \]

1

1

1

quadrature

[_quadrature]

0.725











14171

\[ {}\left (5 x^{5}-4 \cos \left (x\right )\right ) x^{\prime }+2 \cos \left (9 t \right )+2 \sin \left (7 t \right ) = 0 \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

38.446











14172

\[ {}\cosh \left (6 t \right )+5 \sinh \left (4 t \right )+20 \sinh \left (y\right ) y^{\prime } = 0 \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

10.86











14173

\[ {}y^{\prime } = {\mathrm e}^{2 y+10 t} \]

1

1

1

exact, separable, first order special form ID 1, first_order_ode_lie_symmetry_lookup

[_separable]

0.952











14174

\[ {}y^{\prime } = {\mathrm e}^{3 y+2 t} \]

1

1

1

exact, separable, first order special form ID 1, first_order_ode_lie_symmetry_lookup

[_separable]

0.931











14175

\[ {}\sin \left (t \right )^{2} = \cos \left (y\right )^{2} y^{\prime } \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.695











14176

\[ {}3 \sin \left (t \right )-\sin \left (3 t \right ) = \left (\cos \left (4 y\right )-4 \cos \left (y\right )\right ) y^{\prime } \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

36.885











14177

\[ {}x^{\prime } = \frac {\sec \left (t \right )^{2}}{\sec \left (x\right ) \tan \left (x\right )} \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

35.875











14178

\[ {}\left (2-\frac {5}{y^{2}}\right ) y^{\prime }+4 \cos \left (x \right )^{2} = 0 \]

1

1

2

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

3.216











14179

\[ {}y^{\prime } = \frac {t^{3}}{y \sqrt {\left (1-y^{2}\right ) \left (t^{4}+9\right )}} \]

1

1

1

exactWithIntegrationFactor

[[_1st_order, ‘_with_symmetry_[F(x),G(x)*y+H(x)]‘]]

3.423











14180

\[ {}\tan \left (y\right ) \sec \left (y\right )^{2} y^{\prime }+\cos \left (2 x \right )^{3} \sin \left (2 x \right ) = 0 \]

1

1

2

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

37.102











14181

\[ {}y^{\prime } = \frac {\left (1+2 \,{\mathrm e}^{y}\right ) {\mathrm e}^{-y}}{t \ln \left (t \right )} \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

3.635











14182

\[ {}x \sin \left (x^{2}\right ) = \frac {\cos \left (\sqrt {y}\right ) y^{\prime }}{\sqrt {y}} \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

37.088











14183

\[ {}\frac {-2+x}{x^{2}-4 x +3} = \frac {\left (1-\frac {1}{y}\right )^{2} y^{\prime }}{y^{2}} \]

1

1

3

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

10.648











14184

\[ {}\frac {\cos \left (y\right ) y^{\prime }}{\left (1-\sin \left (y\right )\right )^{2}} = \sin \left (x \right )^{3} \cos \left (x \right ) \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

37.259











14185

\[ {}y^{\prime } = \frac {\left (5-2 \cos \left (x \right )\right )^{3} \sin \left (x \right ) \cos \left (y\right )^{4}}{\sin \left (y\right )} \]

1

1

3

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

36.439











14186

\[ {}\frac {\sqrt {\ln \left (x \right )}}{x} = \frac {{\mathrm e}^{\frac {3}{y}} y^{\prime }}{y} \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.431











14187

\[ {}y^{\prime } = \frac {5^{-t}}{y^{2}} \]

1

1

3

exact, separable, differentialType, first_order_ode_lie_symmetry_lookup

[_separable]

50.23











14188

\[ {}y^{\prime } = t^{2} y^{2}+y^{2}-t^{2}-1 \]

1

1

1

exact, riccati, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.637











14189

\[ {}y^{\prime } = y^{2}-3 y+2 \]

1

1

1

quadrature

[_quadrature]

0.855











14190

\[ {}4 \left (-1+x \right )^{2} y^{\prime }-3 \left (3+y\right )^{2} = 0 \]

1

1

1

exact, riccati, separable, homogeneousTypeMapleC, first_order_ode_lie_symmetry_lookup

[_separable]

1.885











14191

\[ {}y^{\prime } = \sin \left (t -y\right )+\sin \left (t +y\right ) \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

3.093











14192

\[ {}y^{\prime } = y^{3}+1 \]

1

1

1

quadrature

[_quadrature]

4.538











14193

\[ {}y^{\prime } = y^{3}-1 \]

1

1

1

quadrature

[_quadrature]

4.643











14194

\[ {}y^{\prime } = y^{3}+y \]

1

2

2

quadrature

[_quadrature]

2.178











14195

\[ {}y^{\prime } = y^{3}-y^{2} \]

1

1

1

quadrature

[_quadrature]

0.717











14196

\[ {}y^{\prime } = y^{3}-y \]

1

2

2

quadrature

[_quadrature]

1.527











14197

\[ {}y^{\prime } = y^{3}+y \]

1

2

2

quadrature

[_quadrature]

0.966











14198

\[ {}y^{\prime } = x^{3} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.317











14199

\[ {}y^{\prime } = \cos \left (t \right ) \]

i.c.

1

1

1

quadrature

[_quadrature]

0.51











14200

\[ {}1 = \cos \left (y\right ) y^{\prime } \]

i.c.

1

1

1

quadrature

[_quadrature]

0.472











14201

\[ {}\sin \left (y \right )^{2} = x^{\prime } \]

i.c.

1

1

1

quadrature

[_quadrature]

0.655











14202

\[ {}y^{\prime } = \frac {\sqrt {t}}{y} \]

i.c.

1

1

1

exact, separable, differentialType, first_order_ode_lie_symmetry_lookup

[_separable]

5.73











14203

\[ {}y^{\prime } = \sqrt {\frac {y}{t}} \]

i.c.

1

1

4

homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

123.202











14204

\[ {}y^{\prime } = \frac {{\mathrm e}^{t}}{y+1} \]

i.c.

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.654











14205

\[ {}y^{\prime } = {\mathrm e}^{t -y} \]

i.c.

1

1

1

exact, separable, first order special form ID 1, first_order_ode_lie_symmetry_lookup

[_separable]

1.177











14206

\[ {}y^{\prime } = \frac {y}{\ln \left (y\right )} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.535











14207

\[ {}y^{\prime } = t \sin \left (t^{2}\right ) \]

i.c.

1

1

1

quadrature

[_quadrature]

0.757











14208

\[ {}y^{\prime } = \frac {1}{x^{2}+1} \]

i.c.

1

1

1

quadrature

[_quadrature]

0.374











14209

\[ {}y^{\prime } = \frac {\sin \left (x \right )}{\cos \left (y\right )+1} \]

i.c.

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.88











14210

\[ {}y^{\prime } = \frac {3+y}{1+3 x} \]

i.c.

1

1

1

exact, linear, separable, homogeneousTypeMapleC, first_order_ode_lie_symmetry_lookup

[_separable]

2.444











14211

\[ {}y^{\prime } = {\mathrm e}^{x -y} \]

i.c.

1

1

1

exact, separable, first order special form ID 1, first_order_ode_lie_symmetry_lookup

[_separable]

1.232











14212

\[ {}y^{\prime } = {\mathrm e}^{2 x -y} \]

i.c.

1

1

1

exact, separable, first order special form ID 1, first_order_ode_lie_symmetry_lookup

[_separable]

1.476











14213

\[ {}y^{\prime } = \frac {3 y+1}{x +3} \]

i.c.

1

1

1

exact, linear, separable, homogeneousTypeMapleC, first_order_ode_lie_symmetry_lookup

[_separable]

2.701











14214

\[ {}y^{\prime } = y \cos \left (t \right ) \]

i.c.

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.632











14215

\[ {}y^{\prime } = y^{2} \cos \left (t \right ) \]

i.c.

1

1

1

exact, riccati, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.333











14216

\[ {}y^{\prime } = \sqrt {y}\, \cos \left (t \right ) \]

i.c.

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

3.479











14217

\[ {}y^{\prime }+y f \left (t \right ) = 0 \]

i.c.

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.801











14218

\[ {}y^{\prime } = -\frac {y-2}{-2+x} \]

i.c.

1

1

1

exact, linear, separable, differentialType, homogeneousTypeMapleC, first_order_ode_lie_symmetry_lookup

[_separable]

2.186











14219

\[ {}y^{\prime } = \frac {x +y+3}{3 x +3 y+1} \]

1

1

1

first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

1.496











14220

\[ {}y^{\prime } = \frac {x -y+2}{2 x -2 y-1} \]

1

1

1

first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

1.58











14221

\[ {}y^{\prime } = \left (x +y-4\right )^{2} \]

1

1

1

riccati, homogeneousTypeC, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class C‘], _Riccati]

1.074











14222

\[ {}y^{\prime } = \left (3 y+1\right )^{4} \]

1

3

3

quadrature

[_quadrature]

1.407











14223

\[ {}y^{\prime } = 3 y \]

1

1

1

quadrature

[_quadrature]

0.467











14224

\[ {}y^{\prime } = -y \]

1

1

1

quadrature

[_quadrature]

0.468











14225

\[ {}y^{\prime } = y^{2}-y \]

1

1

1

quadrature

[_quadrature]

0.835











14226

\[ {}y^{\prime } = 16 y-8 y^{2} \]

1

1

1

quadrature

[_quadrature]

0.836











14227

\[ {}y^{\prime } = 12+4 y-y^{2} \]

1

1

1

quadrature

[_quadrature]

0.947











14228

\[ {}y^{\prime } = y f \left (t \right ) \]

i.c.

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.638











14229

\[ {}y^{\prime }-y = 10 \]

1

1

1

quadrature

[_quadrature]

0.375











14230

\[ {}y^{\prime }-y = 2 \,{\mathrm e}^{-t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.894











14231

\[ {}y^{\prime }-y = 2 \cos \left (t \right ) \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.11











14232

\[ {}y^{\prime }-y = t^{2}-2 t \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.833











14233

\[ {}y^{\prime }-y = 4 t \,{\mathrm e}^{-t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.948











14234

\[ {}t y^{\prime }+y = t^{2} \]

1

1

1

exact, linear, differentialType, first_order_ode_lie_symmetry_lookup

[_linear]

1.039











14235

\[ {}t y^{\prime }+y = t \]

1

1

1

exact, linear, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_linear]

1.537











14236

\[ {}x y^{\prime }+y = x \,{\mathrm e}^{x} \]

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

0.965











14237

\[ {}x y^{\prime }+y = {\mathrm e}^{-x} \]

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

0.992











14238

\[ {}y^{\prime }-\frac {2 t y}{t^{2}+1} = 2 \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.048











14239

\[ {}y^{\prime }-\frac {4 t y}{4 t^{2}+1} = 4 t \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.078











14240

\[ {}y^{\prime } = 2 x +\frac {x y}{x^{2}-1} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.14











14241

\[ {}y^{\prime }+y \cot \left (t \right ) = \cos \left (t \right ) \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.421











14242

\[ {}y^{\prime }-\frac {3 t y}{t^{2}-4} = t \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.097











14243

\[ {}y^{\prime }-\frac {4 t y}{4 t^{2}-9} = t \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.108











14244

\[ {}y^{\prime }-\frac {9 x y}{9 x^{2}+49} = x \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.084











14245

\[ {}y^{\prime }+2 y \cot \left (x \right ) = \cos \left (x \right ) \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.288











14246

\[ {}y^{\prime }+x y = x^{3} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

0.894











14247

\[ {}y^{\prime }-x y = x \]

1

1

1

exact, linear, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.14











14248

\[ {}y^{\prime } = \frac {1}{x +y^{2}} \]

1

1

1

exactWithIntegrationFactor, first_order_ode_lie_symmetry_calculated

[[_1st_order, _with_exponential_symmetries]]

0.976











14249

\[ {}y^{\prime }-x = y \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.776











14250

\[ {}y-\left (x +3 y^{2}\right ) y^{\prime } = 0 \]

1

1

2

exactWithIntegrationFactor, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class G‘], _rational]

1.014











14251

\[ {}x^{\prime } = \frac {3 x t^{2}}{-t^{3}+1} \]

1

1

1

exact, linear, separable, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.479











14252

\[ {}p^{\prime } = t^{3}+\frac {p}{t} \]

1

1

1

linear, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

0.995











14253

\[ {}v^{\prime }+v = {\mathrm e}^{-s} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.904











14254

\[ {}y^{\prime }-y = 4 \,{\mathrm e}^{t} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.171











14255

\[ {}y^{\prime }+y = {\mathrm e}^{-t} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.116











14256

\[ {}y^{\prime }+3 t^{2} y = {\mathrm e}^{-t^{3}} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.23











14257

\[ {}y^{\prime }+2 t y = 2 t \]

i.c.

1

1

1

exact, linear, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.138











14258

\[ {}t y^{\prime }+y = \cos \left (t \right ) \]

i.c.

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

1.395











14259

\[ {}t y^{\prime }+y = 2 \,{\mathrm e}^{t} t \]

i.c.

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

1.293











14260

\[ {}\left (1+{\mathrm e}^{t}\right ) y^{\prime }+{\mathrm e}^{t} y = t \]

i.c.

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

1.49











14261

\[ {}\left (t^{2}+4\right ) y^{\prime }+2 t y = 2 t \]

i.c.

1

1

1

exact, linear, separable, differentialType, first_order_ode_lie_symmetry_lookup

[_separable]

2.252











14262

\[ {}x^{\prime } = x+t +1 \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.076











14263

\[ {}y^{\prime } = {\mathrm e}^{2 t}+2 y \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.102











14264

\[ {}y^{\prime }-\frac {y}{t} = \ln \left (t \right ) \]

1

1

1

linear, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.043











14265

\[ {}y^{\prime \prime }-\frac {y^{\prime }}{t}+\frac {y}{t^{2}} = \frac {1}{t} \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _exact, _linear, _nonhomogeneous]]

2.964











14266

\[ {}y^{\prime }+y = \left \{\begin {array}{cc} 4 & 0\le t <2 \\ 0 & 2\le t \end {array}\right . \]

i.c.

1

0

1

linear, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

4.965











14267

\[ {}y^{\prime }+y = \left \{\begin {array}{cc} t & 0\le t <1 \\ 0 & 1\le t \end {array}\right . \]

i.c.

1

0

1

linear, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

4.58











14268

\[ {}y^{\prime }-y = \sin \left (2 t \right ) \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.211











14269

\[ {}y^{\prime }+y = 5 \,{\mathrm e}^{2 t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.919











14270

\[ {}y^{\prime }+y = {\mathrm e}^{-t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.858











14271

\[ {}y^{\prime }+y = 2-{\mathrm e}^{2 t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.918











14272

\[ {}y^{\prime }-5 y = t \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.876











14273

\[ {}y^{\prime }+3 y = 27 t^{2}+9 \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.898











14274

\[ {}y^{\prime }-\frac {y}{2} = 5 \cos \left (t \right )+2 \,{\mathrm e}^{t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.453











14275

\[ {}y^{\prime }+4 y = 8 \cos \left (4 t \right ) \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.347











14276

\[ {}y^{\prime }+10 y = 2 \,{\mathrm e}^{t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.939











14277

\[ {}y^{\prime }-3 y = 27 t^{2} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.893











14278

\[ {}y^{\prime }-y = 2 \,{\mathrm e}^{t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.849











14279

\[ {}y^{\prime }+y = 4+3 \,{\mathrm e}^{t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.959











14280

\[ {}y^{\prime }+y = 2 \cos \left (t \right )+t \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.183











14281

\[ {}y^{\prime }+\frac {y}{2} = \sin \left (t \right ) \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.462











14282

\[ {}y^{\prime }-\frac {y}{2} = \sin \left (t \right ) \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.385











14283

\[ {}t y^{\prime }+y = t \cos \left (t \right ) \]

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

1.155











14284

\[ {}y^{\prime }+y = t \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.079











14285

\[ {}y^{\prime }+y = \sin \left (t \right ) \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.336











14286

\[ {}y^{\prime }+y = \cos \left (t \right ) \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.329











14287

\[ {}y^{\prime }+y = {\mathrm e}^{t} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.079











14288

\[ {}y^{2}-\frac {y}{2 \sqrt {t}}+\left (2 t y-\sqrt {t}+1\right ) y^{\prime } = 0 \]

1

1

2

exact, first_order_ode_lie_symmetry_calculated

[_exact, _rational, [_Abel, ‘2nd type‘, ‘class B‘]]

13.151











14289

\[ {}\frac {t}{\sqrt {t^{2}+y^{2}}}+\frac {y y^{\prime }}{\sqrt {t^{2}+y^{2}}} = 0 \]

1

1

2

exact, separable, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

2.712











14290

\[ {}y \cos \left (t y\right )+t \cos \left (t y\right ) y^{\prime } = 0 \]

1

1

2

exact, linear, separable, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.697











14291

\[ {}y \sec \left (t \right )^{2}+2 t +\tan \left (t \right ) y^{\prime } = 0 \]

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

11.383











14292

\[ {}3 t y^{2}+y^{3} y^{\prime } = 0 \]

1

1

3

exact, separable, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.883











14293

\[ {}t -y \sin \left (t \right )+\left (y^{6}+\cos \left (t \right )\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact]

3.112











14294

\[ {}y \sin \left (2 t \right )+\left (\sqrt {y}+\cos \left (2 t \right )\right ) y^{\prime } = 0 \]

1

1

1

exactWithIntegrationFactor

[[_1st_order, ‘_with_symmetry_[F(x)*G(y),0]‘]]

11.048











14295

\[ {}{\mathrm e}^{2 t}-y-\left ({\mathrm e}^{y}-t \right ) y^{\prime } = 0 \]

1

0

0

unknown

[‘y=_G(x,y’)‘]

N/A

1.326











14296

\[ {}\ln \left (t y\right )+\frac {t y^{\prime }}{y} = 0 \]

1

1

1

exact, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class G‘], _exact]

3.692











14297

\[ {}{\mathrm e}^{t y}+\frac {t \,{\mathrm e}^{t y} y^{\prime }}{y} = 0 \]

1

1

1

exact, linear, separable, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.963











14298

\[ {}3 t^{2}-y^{\prime } = 0 \]

1

1

1

quadrature

[_quadrature]

0.203











14299

\[ {}-1+3 y^{2} y^{\prime } = 0 \]

1

3

3

quadrature

[_quadrature]

0.709











14300

\[ {}y^{2}+2 t y y^{\prime } = 0 \]

1

1

3

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.162











14301

\[ {}\frac {3 t^{2}}{y}-\frac {t^{3} y^{\prime }}{y^{2}} = 0 \]

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.835











14302

\[ {}2 t +y^{3}+\left (3 t y^{2}+4\right ) y^{\prime } = 0 \]

1

1

3

exact

[_exact, _rational]

1.446











14303

\[ {}-\frac {1}{y}+\left (\frac {t}{y^{2}}+3 y^{2}\right ) y^{\prime } = 0 \]

1

1

1

exact, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class G‘], _exact, _rational]

1.446











14304

\[ {}2 t y+\left (t^{2}+y^{2}\right ) y^{\prime } = 0 \]

1

1

3

exact, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _exact, _rational, _dAlembert]

10.187











14305

\[ {}2 t y^{3}+\left (1+3 t^{2} y^{2}\right ) y^{\prime } = 0 \]

1

1

3

exact, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class G‘], _exact, _rational]

3.243











14306

\[ {}\sin \left (y\right )^{2}+t \sin \left (2 y\right ) y^{\prime } = 0 \]

1

1

2

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

6.826











14307

\[ {}3 t^{2}+3 y^{2}+6 t y y^{\prime } = 0 \]

1

1

2

exact, bernoulli, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _exact, _rational, _Bernoulli]

2.386











14308

\[ {}{\mathrm e}^{t} \sin \left (y\right )+\left (1+{\mathrm e}^{t} \cos \left (y\right )\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact, [_1st_order, ‘_with_symmetry_[F(x)*G(y),0]‘]]

2.067











14309

\[ {}3 t^{2} y+3 y^{2}-1+\left (t^{3}+6 t y\right ) y^{\prime } = 0 \]

1

1

2

exact

[_exact, _rational, [_Abel, ‘2nd type‘, ‘class B‘]]

1.608











14310

\[ {}-2 t y^{2} \sin \left (t^{2}\right )+2 y \cos \left (t^{2}\right ) y^{\prime } = 0 \]

1

1

3

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

3.513











14311

\[ {}2 t -y^{2} \sin \left (t y\right )+\left (\cos \left (t y\right )-t y \sin \left (t y\right )\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact]

11.457











14312

\[ {}1-y^{2} \cos \left (t y\right )+\left (t y \cos \left (t y\right )+\sin \left (t y\right )\right ) y^{\prime } = 0 \]

1

0

0

unknown

[‘y=_G(x,y’)‘]

N/A

8.605











14313

\[ {}2 t \sin \left (y\right )-2 t y \sin \left (t^{2}\right )+\left (t^{2} \cos \left (y\right )+\cos \left (t^{2}\right )\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact]

35.254











14314

\[ {}\left (3+t \right ) \cos \left (t +y\right )+\sin \left (t +y\right )+\left (3+t \right ) \cos \left (t +y\right ) y^{\prime } = 0 \]

1

1

1

exact, first_order_ode_lie_symmetry_calculated

[[_1st_order, _with_linear_symmetries], _exact]

10.316











14315

\[ {}\frac {2 t^{2} y \cos \left (t^{2}\right )-y \sin \left (t^{2}\right )}{t^{2}}+\frac {\left (2 t y+\sin \left (t^{2}\right )\right ) y^{\prime }}{t} = 0 \]

1

1

2

exact

[_exact, [_1st_order, ‘_with_symmetry_[F(x)*G(y),0]‘], [_Abel, ‘2nd type‘, ‘class B‘]]

9.75











14316

\[ {}-\frac {y^{2} {\mathrm e}^{\frac {y}{t}}}{t^{2}}+1+{\mathrm e}^{\frac {y}{t}} \left (1+\frac {y}{t}\right ) y^{\prime } = 0 \]

1

1

1

exact, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _exact, _dAlembert]

3.293











14317

\[ {}2 t \sin \left (\frac {y}{t}\right )-y \cos \left (\frac {y}{t}\right )+t \cos \left (\frac {y}{t}\right ) y^{\prime } = 0 \]

1

1

1

exact, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _exact, _dAlembert]

3.123











14318

\[ {}2 t y^{2}+2 t^{2} y y^{\prime } = 0 \]

i.c.

1

1

1

exact, linear, separable, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.845











14319

\[ {}1+\frac {y}{t^{2}}-\frac {y^{\prime }}{t} = 0 \]

i.c.

1

1

1

exact, linear, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_linear]

1.148











14320

\[ {}2 t y+3 t^{2}+\left (t^{2}-1\right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact, linear, differentialType, first_order_ode_lie_symmetry_lookup

[_linear]

1.512











14321

\[ {}1+5 t -y-\left (t +2 y\right ) y^{\prime } = 0 \]

i.c.

1

1

2

exact, differentialType, homogeneousTypeMapleC, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _exact, _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

5.456











14322

\[ {}{\mathrm e}^{y}-2 t y+\left (t \,{\mathrm e}^{y}-t^{2}\right ) y^{\prime } = 0 \]

i.c.

1

0

0

exact

[_exact]

N/A

4.658











14323

\[ {}2 t y \,{\mathrm e}^{t^{2}}+2 t \,{\mathrm e}^{-y}+\left ({\mathrm e}^{t^{2}}-t^{2} {\mathrm e}^{-y}+1\right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact

[_exact]

36.807











14324

\[ {}y^{2}-2 \sin \left (2 t \right )+\left (1+2 t y\right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact

[_exact, [_Abel, ‘2nd type‘, ‘class B‘]]

8.174











14325

\[ {}\cos \left (t \right )^{2}-\sin \left (t \right )^{2}+y+\left (\sec \left (y\right ) \tan \left (y\right )+t \right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact

[_exact]

39.358











14326

\[ {}\frac {1}{t^{2}+1}-y^{2}-2 t y y^{\prime } = 0 \]

i.c.

1

1

0

exact, bernoulli, first_order_ode_lie_symmetry_lookup

[_exact, _rational, _Bernoulli]

1.777











14327

\[ {}\frac {2 t}{t^{2}+1}+y+\left ({\mathrm e}^{y}+t \right ) y^{\prime } = 0 \]

i.c.

1

0

0

exact

[_exact]

N/A

9.528











14328

\[ {}-2 x -y \cos \left (x y\right )+\left (2 y-x \cos \left (x y\right )\right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact

[_exact]

35.291











14329

\[ {}-4 x^{3}+6 y \sin \left (6 x y\right )+\left (4 y^{3}+6 x \sin \left (6 x y\right )\right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact

[_exact]

44.442











14330

\[ {}t^{2} y+t^{3} y^{\prime } = 0 \]

1

1

1

exact, linear, separable, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.45











14331

\[ {}y \left (2 \,{\mathrm e}^{t}+4 t \right )+3 \left ({\mathrm e}^{t}+t^{2}\right ) y^{\prime } = 0 \]

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.579











14332

\[ {}y+\left (2 t -y \,{\mathrm e}^{y}\right ) y^{\prime } = 0 \]

1

1

1

exactWithIntegrationFactor

[[_1st_order, ‘_with_symmetry_[F(x)*G(y),0]‘]]

1.392











14333

\[ {}2 t y+y^{2}-t^{2} y^{\prime } = 0 \]

1

1

1

riccati, bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _rational, _Bernoulli]

1.324











14334

\[ {}y+2 t^{2}+\left (t^{2} y-t \right ) y^{\prime } = 0 \]

1

1

2

exactWithIntegrationFactor

[_rational, [_1st_order, ‘_with_symmetry_[F(x),G(x)]‘], [_Abel, ‘2nd type‘, ‘class B‘]]

1.399











14335

\[ {}5 t y+4 y^{2}+1+\left (t^{2}+2 t y\right ) y^{\prime } = 0 \]

1

1

2

exactWithIntegrationFactor

[_rational, [_Abel, ‘2nd type‘, ‘class B‘]]

1.58











14336

\[ {}5 t y^{2}+y+\left (2 t^{3}-t \right ) y^{\prime } = 0 \]

1

1

1

riccati, bernoulli, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class D‘], _rational, _Bernoulli]

1.608











14337

\[ {}2 t +\tan \left (y\right )+\left (t -t^{2} \tan \left (y\right )\right ) y^{\prime } = 0 \]

1

1

2

exactWithIntegrationFactor

[[_1st_order, ‘_with_symmetry_[F(x),G(x)]‘]]

2.592











14338

\[ {}2 t -y^{2} \sin \left (t y\right )+\left (\cos \left (t y\right )-t y \sin \left (t y\right )\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact]

11.434











14339

\[ {}-1+{\mathrm e}^{t y} y+y \cos \left (t y\right )+\left (1+{\mathrm e}^{t y} t +t \cos \left (t y\right )\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact]

41.909











14340

\[ {}2 t +2 y+\left (2 t +2 y\right ) y^{\prime } = 0 \]

1

1

3

quadrature

[_quadrature]

0.211











14341

\[ {}\frac {9 t}{5}+2 y+\left (2 t +2 y\right ) y^{\prime } = 0 \]

1

1

2

exact, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _exact, _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

3.082











14342

\[ {}2 t +\frac {19 y}{10}+\left (\frac {19 t}{10}+2 y\right ) y^{\prime } = 0 \]

1

1

2

exact, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _exact, _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

3.076











14343

\[ {}y^{\prime }-\frac {y}{2} = \frac {t}{y} \]

1

1

2

bernoulli, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_rational, _Bernoulli]

1.296











14344

\[ {}y^{\prime }+y = t y^{2} \]

1

1

1

riccati, bernoulli, first_order_ode_lie_symmetry_lookup

[_Bernoulli]

0.944











14345

\[ {}2 t y^{\prime }-y = 2 t y^{3} \cos \left (t \right ) \]

1

1

2

bernoulli, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_Bernoulli]

35.666











14346

\[ {}t y^{\prime }-y = t y^{3} \sin \left (t \right ) \]

1

2

2

bernoulli, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class D‘], _Bernoulli]

32.289











14347

\[ {}y^{\prime }-2 y = \frac {\cos \left (t \right )}{\sqrt {y}} \]

1

1

1

bernoulli, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_Bernoulli]

10.556











14348

\[ {}y^{\prime }+3 y = \sqrt {y}\, \sin \left (t \right ) \]

1

1

1

bernoulli, first_order_ode_lie_symmetry_lookup

[_Bernoulli]

41.946











14349

\[ {}y^{\prime }-\frac {y}{t} = t y^{2} \]

1

1

1

riccati, bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class D‘], _rational, _Bernoulli]

1.211











14350

\[ {}y^{\prime }-\frac {y}{t} = \frac {y^{2}}{t^{2}} \]

1

1

1

riccati, bernoulli, exactByInspection, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _rational, _Bernoulli]

1.177











14351

\[ {}y^{\prime }-\frac {y}{t} = \frac {y^{2}}{t} \]

1

1

1

exact, riccati, bernoulli, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

2.685











14352

\[ {}y^{\prime }-\frac {y}{t} = t^{2} y^{\frac {3}{2}} \]

1

1

1

bernoulli, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class G‘], _rational, _Bernoulli]

2.291











14353

\[ {}\cos \left (\frac {t}{t +y}\right )+{\mathrm e}^{\frac {2 y}{t}} y^{\prime } = 0 \]

1

1

1

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

3.639











14354

\[ {}y \ln \left (\frac {t}{y}\right )+\frac {t^{2} y^{\prime }}{t +y} = 0 \]

1

1

1

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

15.695











14355

\[ {}2 \ln \left (t \right )-\ln \left (4 y^{2}\right ) y^{\prime } = 0 \]

1

1

2

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

5.747











14356

\[ {}\frac {2}{t}+\frac {1}{y}+\frac {t y^{\prime }}{y^{2}} = 0 \]

1

1

1

riccati, bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _rational, _Bernoulli]

1.791











14357

\[ {}\frac {\sin \left (2 t \right )}{\cos \left (2 y\right )}+\frac {\ln \left (y\right ) y^{\prime }}{\ln \left (t \right )} = 0 \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

30.221











14358

\[ {}\sqrt {t^{2}+1}+y y^{\prime } = 0 \]

1

1

2

exact, separable, differentialType, first_order_ode_lie_symmetry_lookup

[_separable]

3.096











14359

\[ {}2 t +\left (y-3 t \right ) y^{\prime } = 0 \]

1

1

2

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class C‘], _dAlembert]

3.185











14360

\[ {}2 y-3 t +t y^{\prime } = 0 \]

1

1

1

linear, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.466











14361

\[ {}t y-y^{2}+t \left (t -3 y\right ) y^{\prime } = 0 \]

1

1

3

homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class B‘]]

3.457











14362

\[ {}t^{2}+t y+y^{2}-t y y^{\prime } = 0 \]

1

1

1

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class B‘]]

1.678











14363

\[ {}t^{3}+y^{3}-t y^{2} y^{\prime } = 0 \]

1

1

3

bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _rational, _Bernoulli]

2.089











14364

\[ {}y^{\prime } = \frac {t +4 y}{4 t +y} \]

1

1

1

exactByInspection, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

3.911











14365

\[ {}t -y+t y^{\prime } = 0 \]

1

1

1

linear, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

0.949











14366

\[ {}y+\left (t +y\right ) y^{\prime } = 0 \]

1

1

2

exact, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _exact, _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

3.825











14367

\[ {}2 t^{2}-7 t y+5 y^{2}+t y y^{\prime } = 0 \]

1

1

1

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class B‘]]

15.009











14368

\[ {}y+2 \sqrt {t^{2}+y^{2}}-t y^{\prime } = 0 \]

1

1

1

first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

5.359











14369

\[ {}y^{2} = \left (t y-4 t^{2}\right ) y^{\prime } \]

1

1

1

exactByInspection, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class B‘]]

1.947











14370

\[ {}y-\left (3 \sqrt {t y}+t \right ) y^{\prime } = 0 \]

1

1

1

first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

3.876











14371

\[ {}\left (t^{2}-y^{2}\right ) y^{\prime }+y^{2}+t y = 0 \]

1

1

3

exact, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

3.86











14372

\[ {}t y y^{\prime }-t^{2} {\mathrm e}^{-\frac {y}{t}}-y^{2} = 0 \]

1

1

1

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

1.488











14373

\[ {}y^{\prime } = \frac {1}{\frac {2 y \,{\mathrm e}^{-\frac {t}{y}}}{t}+\frac {t}{y}} \]

1

1

1

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

3.719











14374

\[ {}t \left (\ln \left (t \right )-\ln \left (y\right )\right ) y^{\prime } = y \]

1

1

1

exactByInspection, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

3.945











14375

\[ {}y^{\prime }+2 y = t^{2} \sqrt {y} \]

i.c.

1

1

1

bernoulli, first_order_ode_lie_symmetry_lookup

[_Bernoulli]

2.97











14376

\[ {}y^{\prime }-2 y = t^{2} \sqrt {y} \]

i.c.

1

1

1

bernoulli, first_order_ode_lie_symmetry_lookup

[_Bernoulli]

3.215











14377

\[ {}y^{\prime } = \frac {4 y^{2}-t^{2}}{2 t y} \]

i.c.

1

1

1

bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _rational, _Bernoulli]

2.464











14378

\[ {}t +y-t y^{\prime } = 0 \]

i.c.

1

1

1

linear, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.295











14379

\[ {}t y^{\prime }-y-\sqrt {t^{2}+y^{2}} = 0 \]

i.c.

1

1

2

first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, _dAlembert]

3.808











14380

\[ {}t^{3}+y^{2} \sqrt {t^{2}+y^{2}}-t y \sqrt {t^{2}+y^{2}}\, y^{\prime } = 0 \]

i.c.

1

1

1

exactWithIntegrationFactor, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

5.021











14381

\[ {}y^{3}-t^{3}-t y^{2} y^{\prime } = 0 \]

i.c.

1

1

1

bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _rational, _Bernoulli]

1.701











14382

\[ {}t y^{3}-\left (t^{4}+y^{4}\right ) y^{\prime } = 0 \]

i.c.

1

1

1

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, _dAlembert]

6.012











14383

\[ {}y^{4}+\left (t^{4}-t y^{3}\right ) y^{\prime } = 0 \]

i.c.

1

1

1

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, _dAlembert]

8.887











14384

\[ {}t -2 y+1+\left (4 t -3 y-6\right ) y^{\prime } = 0 \]

1

1

1

homogeneousTypeMapleC, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

4.077











14385

\[ {}5 t +2 y+1+\left (2 t +y+1\right ) y^{\prime } = 0 \]

1

1

1

exact, differentialType, homogeneousTypeMapleC, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _exact, _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

4.359











14386

\[ {}3 t -y+1-\left (6 t -2 y-3\right ) y^{\prime } = 0 \]

1

1

1

first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

1.536











14387

\[ {}2 t +3 y+1+\left (4 t +6 y+1\right ) y^{\prime } = 0 \]

1

1

1

first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

1.532











14388

\[ {}y^{\prime }-\frac {2 y}{x} = -x^{2} y \]

1

1

1

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.704











14389

\[ {}y^{\prime }+y \cot \left (x \right ) = y^{4} \]

i.c.

1

1

1

bernoulli, first_order_ode_lie_symmetry_lookup

[_Bernoulli]

37.984











14390

\[ {}t y^{\prime }-{y^{\prime }}^{3} = y \]

3

3

3

clairaut

[[_1st_order, _with_linear_symmetries], _Clairaut]

0.749











14391

\[ {}t y^{\prime }-y-2 \left (t y^{\prime }-y\right )^{2} = y^{\prime }+1 \]

2

4

3

clairaut

[[_1st_order, _with_linear_symmetries], _rational, _Clairaut]

1.021











14392

\[ {}t y^{\prime }-y-1 = {y^{\prime }}^{2}-y^{\prime } \]

2

2

2

clairaut

[[_1st_order, _with_linear_symmetries], _Clairaut]

0.456











14393

\[ {}1+y-t y^{\prime } = \ln \left (y^{\prime }\right ) \]

0

2

2

clairaut

[[_1st_order, _with_linear_symmetries], _Clairaut]

1.332











14394

\[ {}1-2 t y^{\prime }+2 y = \frac {1}{{y^{\prime }}^{2}} \]

3

4

4

clairaut

[[_1st_order, _with_linear_symmetries], _Clairaut]

1.589











14395

\[ {}y = -t y^{\prime }+\frac {{y^{\prime }}^{5}}{5} \]

5

2

1

dAlembert

[_dAlembert]

0.66











14396

\[ {}y = t {y^{\prime }}^{2}+3 {y^{\prime }}^{2}-2 {y^{\prime }}^{3} \]

3

5

4

dAlembert

[_dAlembert]

59.272











14397

\[ {}y = t \left (y^{\prime }+1\right )+2 y^{\prime }+1 \]

1

1

1

linear, homogeneousTypeMapleC, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.308











14398

\[ {}y = t \left (2-y^{\prime }\right )+2 {y^{\prime }}^{2}+1 \]

2

3

3

dAlembert

[[_1st_order, _with_linear_symmetries], _dAlembert]

0.661











14399

\[ {}t^{\frac {1}{3}} y^{\frac {2}{3}}+t +\left (t^{\frac {2}{3}} y^{\frac {1}{3}}+y\right ) y^{\prime } = 0 \]

1

1

1

first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class G‘], _rational]

5.841











14400

\[ {}y^{\prime } = \frac {y^{2}-t^{2}}{t y} \]

i.c.

1

1

2

bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _rational, _Bernoulli]

1.677











14401

\[ {}y \sin \left (\frac {t}{y}\right )-\left (t +t \sin \left (\frac {t}{y}\right )\right ) y^{\prime } = 0 \]

i.c.

1

1

1

homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _dAlembert]

4.586











14402

\[ {}y^{\prime } = \frac {2 t^{5}}{5 y^{2}} \]

1

1

3

exact, separable, differentialType, first_order_ode_lie_symmetry_lookup

[_separable]

7.595











14403

\[ {}\cos \left (4 x \right )-8 \sin \left (y\right ) y^{\prime } = 0 \]

1

1

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.574











14404

\[ {}y^{\prime }-\frac {y}{t} = \frac {y^{2}}{t} \]

1

1

1

exact, riccati, bernoulli, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

2.98











14405

\[ {}y^{\prime } = \frac {{\mathrm e}^{8 y}}{t} \]

1

1

1

exact, separable, first order special form ID 1, first_order_ode_lie_symmetry_lookup

[_separable]

1.113











14406

\[ {}y^{\prime } = \frac {{\mathrm e}^{5 t}}{y^{4}} \]

1

1

5

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

0.912











14407

\[ {}-\frac {1}{x^{5}}+\frac {1}{x^{3}} = \left (2 y^{4}-6 y^{9}\right ) y^{\prime } \]

1

1

10

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.445











14408

\[ {}y^{\prime } = \frac {y \,{\mathrm e}^{-2 t}}{\ln \left (y\right )} \]

1

1

2

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.911











14409

\[ {}y^{\prime } = \frac {\left (4-7 x \right ) \left (2 y-3\right )}{\left (-1+x \right ) \left (2 x -5\right )} \]

1

1

1

exact, linear, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.785











14410

\[ {}y^{\prime }+3 y = -10 \sin \left (t \right ) \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.303











14411

\[ {}3 t +\left (t -4 y\right ) y^{\prime } = 0 \]

1

1

1

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class C‘], _dAlembert]

3.595











14412

\[ {}y-t +\left (t +y\right ) y^{\prime } = 0 \]

1

1

2

exact, differentialType, homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _exact, _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

2.921











14413

\[ {}y-x +y^{\prime } = 0 \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.888











14414

\[ {}y^{2}+\left (t y+t^{2}\right ) y^{\prime } = 0 \]

1

1

2

homogeneousTypeD2, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, [_Abel, ‘2nd type‘, ‘class B‘]]

3.637











14415

\[ {}r^{\prime } = \frac {r^{2}+t^{2}}{r t} \]

1

1

2

bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class A‘], _rational, _Bernoulli]

1.603











14416

\[ {}x^{\prime } = \frac {5 t x}{t^{2}+x^{2}} \]

1

1

1

homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class A‘], _rational, _dAlembert]

5.543











14417

\[ {}t^{2}-y+\left (-t +y\right ) y^{\prime } = 0 \]

1

1

2

exact, differentialType

[_exact, _rational, [_1st_order, ‘_with_symmetry_[F(x),G(x)]‘], [_Abel, ‘2nd type‘, ‘class A‘]]

1.964











14418

\[ {}t^{2} y+\sin \left (t \right )+\left (\frac {t^{3}}{3}-\cos \left (y\right )\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact]

9.555











14419

\[ {}\tan \left (y\right )-t +\left (t \sec \left (y\right )^{2}+1\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact]

4.931











14420

\[ {}t \ln \left (y\right )+\left (\frac {t^{2}}{2 y}+1\right ) y^{\prime } = 0 \]

1

1

1

exact

[_exact, [_1st_order, ‘_with_symmetry_[F(x)*G(y),0]‘]]

1.882











14421

\[ {}y^{\prime }+y = 5 \]

1

1

1

quadrature

[_quadrature]

0.445











14422

\[ {}y^{\prime }+t y = t \]

1

1

1

exact, linear, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.487











14423

\[ {}x^{\prime }+\frac {x}{y} = y^{2} \]

1

1

1

exact, linear, differentialType, first_order_ode_lie_symmetry_lookup

[_linear]

1.267











14424

\[ {}t r^{\prime }+r = t \cos \left (t \right ) \]

1

1

1

exact, linear, first_order_ode_lie_symmetry_lookup

[_linear]

1.18











14425

\[ {}y^{\prime }-y = t y^{3} \]

1

2

2

bernoulli, first_order_ode_lie_symmetry_lookup

[_Bernoulli]

1.333











14426

\[ {}y^{\prime }+y = \frac {{\mathrm e}^{t}}{y^{2}} \]

1

1

3

bernoulli, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_1st_order, _with_linear_symmetries], _Bernoulli]

1.687











14427

\[ {}y = t y^{\prime }+3 {y^{\prime }}^{4} \]

4

4

4

clairaut

[[_1st_order, _with_linear_symmetries], _Clairaut]

2.53











14428

\[ {}-t y^{\prime }+y = 2 y^{2} \ln \left (t \right ) \]

1

1

1

riccati, bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class D‘], _Bernoulli]

1.624











14429

\[ {}-t y^{\prime }+y = -2 {y^{\prime }}^{3} \]

3

3

3

clairaut

[[_1st_order, _with_linear_symmetries], _Clairaut]

0.726











14430

\[ {}-t y^{\prime }+y = -4 {y^{\prime }}^{2} \]

2

2

2

clairaut

[[_1st_order, _with_linear_symmetries], _Clairaut]

0.48











14431

\[ {}2 x -y-2+\left (2 y-x \right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact, differentialType, homogeneousTypeMapleC, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _exact, _rational, [_Abel, ‘2nd type‘, ‘class A‘]]

7.896











14432

\[ {}\cos \left (t -y\right )+\left (1-\cos \left (t -y\right )\right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _exact, _dAlembert]

9.635











14433

\[ {}{\mathrm e}^{t y} y-2 t +t \,{\mathrm e}^{t y} y^{\prime } = 0 \]

i.c.

1

1

1

exact

[_exact, [_1st_order, ‘_with_symmetry_[F(x),G(x)*y+H(x)]‘]]

2.181











14434

\[ {}\sin \left (y\right )-y \cos \left (t \right )+\left (t \cos \left (y\right )-\sin \left (t \right )\right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact

[_exact]

11.48











14435

\[ {}y^{2}+\left (2 t y-2 \cos \left (y\right ) \sin \left (y\right )\right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact

[_exact, [_1st_order, ‘_with_symmetry_[F(x)*G(y),0]‘]]

2.804











14436

\[ {}\frac {y}{t}+\ln \left (y\right )+\left (\frac {t}{y}+\ln \left (t \right )\right ) y^{\prime } = 0 \]

i.c.

1

1

1

exact

[_exact]

3.188











14437

\[ {}y^{\prime } = -x +y^{2} \]

i.c.

1

1

1

riccati

[[_Riccati, _special]]

3.14











14438

\[ {}y^{\prime } = \sqrt {x -y} \]

i.c.

1

1

1

first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _dAlembert]

7.889











14439

\[ {}y^{\prime } = x +y^{\frac {1}{3}} \]

i.c.

1

0

0

unknown

[_Chini]

N/A

0.863











14440

\[ {}y^{\prime } = \sin \left (x^{2} y\right ) \]

i.c.

1

0

0

unknown

[‘y=_G(x,y’)‘]

N/A

1.079











14441

\[ {}y^{\prime } = t y^{3} \]

i.c.

1

0

1

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.024











14442

\[ {}y^{\prime } = \frac {t}{y^{3}} \]

i.c.

1

1

4

exact, separable, differentialType, first_order_ode_lie_symmetry_lookup

[_separable]

2.13











14443

\[ {}y^{\prime } = -\frac {y}{t -2} \]

i.c.

1

1

1

exact, linear, separable, differentialType, homogeneousTypeD2, homogeneousTypeMapleC, first_order_ode_lie_symmetry_lookup

[_separable]

2.637











14444

\[ {}y^{\prime \prime }-y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

1.292











14445

\[ {}y^{\prime \prime }+2 y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.381











14446

\[ {}2 t^{2} y^{\prime \prime }-3 t y^{\prime }-3 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

1.671











14447

\[ {}y^{\prime \prime }+9 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

1.941











14448

\[ {}y^{\prime \prime }-y^{\prime }-2 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.608











14449

\[ {}y^{\prime \prime }+9 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

5.305











14450

\[ {}3 t^{2} y^{\prime \prime }-5 t y^{\prime }-3 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.791











14451

\[ {}t^{2} y^{\prime \prime }+7 t y^{\prime }-7 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_Emden, _Fowler]]

4.243











14452

\[ {}y^{\prime \prime }+y = 2 \cos \left (t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.036











14453

\[ {}y^{\prime \prime }+10 y^{\prime }+24 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.322











14454

\[ {}y^{\prime \prime }+16 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

1.914











14455

\[ {}y^{\prime \prime }+6 y^{\prime }+18 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.708











14456

\[ {}t^{2} y^{\prime \prime }+t y^{\prime }-y = 0 \]

1

1

1

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _exact, _linear, _homogeneous]]

3.97











14457

\[ {}y^{\prime \prime }-5 y^{\prime }+6 y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _missing_x]]

0.283











14458

\[ {}y^{\prime \prime }+6 y^{\prime }+8 y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _missing_x]]

0.286











14459

\[ {}y^{\prime \prime }-4 y^{\prime }+4 y = 0 \]

i.c.

1

1

1

reduction_of_order

[[_2nd_order, _missing_x]]

0.441











14460

\[ {}y^{\prime \prime }+10 y^{\prime }+25 y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _missing_x]]

0.287











14461

\[ {}y^{\prime \prime }+9 y = 0 \]

i.c.

1

1

1

reduction_of_order

[[_2nd_order, _missing_x]]

0.563











14462

\[ {}y^{\prime \prime }+49 y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _missing_x]]

0.544











14463

\[ {}t^{2} y^{\prime \prime }+4 t y^{\prime }-4 y = 0 \]

1

1

1

reduction_of_order

[[_Emden, _Fowler]]

0.521











14464

\[ {}t^{2} y^{\prime \prime }+6 t y^{\prime }+6 y = 0 \]

1

1

1

reduction_of_order

[[_Emden, _Fowler]]

0.578











14465

\[ {}t^{2} y^{\prime \prime }+t y^{\prime }+\left (t^{2}-\frac {1}{4}\right ) y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.758











14466

\[ {}t^{2} y^{\prime \prime }+3 t y^{\prime }+y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _exact, _linear, _homogeneous]]

0.548











14467

\[ {}a y^{\prime \prime }+b y^{\prime }+c y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.607











14468

\[ {}t^{2} y^{\prime \prime }+a t y^{\prime }+b y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

3.349











14469

\[ {}4 t^{2} y^{\prime \prime }+4 t y^{\prime }+\left (36 t^{2}-1\right ) y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

1.005











14470

\[ {}t y^{\prime \prime }+2 y^{\prime }+16 t y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.822











14471

\[ {}y^{\prime \prime }+b \left (t \right ) y^{\prime }+c \left (t \right ) y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

1.766











14472

\[ {}y^{\prime \prime }+b \left (t \right ) y^{\prime }+c \left (t \right ) y = 0 \]

i.c.

1

0

0

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

N/A

0.922











14473

\[ {}y^{\prime \prime } = 0 \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_ode_quadrature, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _quadrature]]

0.84











14474

\[ {}y^{\prime \prime }-4 y^{\prime }-12 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.328











14475

\[ {}y^{\prime \prime }+y^{\prime } = 0 \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.27











14476

\[ {}y^{\prime \prime }+3 y^{\prime }-4 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.325











14477

\[ {}y^{\prime \prime }+8 y^{\prime }+12 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.325











14478

\[ {}y^{\prime \prime }+5 y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.386











14479

\[ {}8 y^{\prime \prime }+6 y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.342











14480

\[ {}4 y^{\prime \prime }+9 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

1.474











14481

\[ {}y^{\prime \prime }+16 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

1.194











14482

\[ {}y^{\prime \prime }+8 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

2.447











14483

\[ {}y^{\prime \prime }+7 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

2.267











14484

\[ {}4 y^{\prime \prime }+21 y^{\prime }+5 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.344











14485

\[ {}7 y^{\prime \prime }+4 y^{\prime }-3 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.339











14486

\[ {}4 y^{\prime \prime }+4 y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.391











14487

\[ {}y^{\prime \prime }-6 y^{\prime }+9 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.372











14488

\[ {}y^{\prime \prime }-y^{\prime } = 0 \]

i.c.

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.337











14489

\[ {}3 y^{\prime \prime }-y^{\prime } = 0 \]

i.c.

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.742











14490

\[ {}y^{\prime \prime }+y^{\prime }-12 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.582











14491

\[ {}y^{\prime \prime }-7 y^{\prime }+12 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.576











14492

\[ {}2 y^{\prime \prime }-7 y^{\prime }-4 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.596











14493

\[ {}y^{\prime \prime }-7 y^{\prime }+10 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.545











14494

\[ {}y^{\prime \prime }+36 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

8.265











14495

\[ {}y^{\prime \prime }+100 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

14.04











14496

\[ {}y^{\prime \prime }-2 y^{\prime }+y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.674











14497

\[ {}y^{\prime \prime }+4 y^{\prime }+4 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.761











14498

\[ {}y^{\prime \prime }+2 y^{\prime }+5 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.944











14499

\[ {}y^{\prime \prime }+4 y^{\prime }+20 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.9











14500

\[ {}y^{\prime \prime }+y^{\prime }-y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.975











14501

\[ {}y^{\prime \prime }+y^{\prime }+y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.251











14502

\[ {}y^{\prime \prime }-y^{\prime }+y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.296











14503

\[ {}y^{\prime \prime }-y^{\prime }-y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.0











14504

\[ {}6 y^{\prime \prime }+5 y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.339











14505

\[ {}9 y^{\prime \prime }+6 y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.399











14506

\[ {}y^{\prime \prime }+4 y^{\prime }+20 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.379











14507

\[ {}3 t^{2} y^{\prime \prime }-2 t y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_Emden, _Fowler]]

2.668











14508

\[ {}t^{2} y^{\prime \prime }-t y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_Emden, _Fowler]]

2.598











14509

\[ {}a y^{\prime \prime }+2 b y^{\prime }+c y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.615











14510

\[ {}y^{\prime \prime }+6 y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.372











14511

\[ {}y^{\prime \prime }-5 y^{\prime }+6 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.318











14512

\[ {}y^{\prime \prime }-6 y^{\prime }-16 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.329











14513

\[ {}y^{\prime \prime }-16 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

1.61











14514

\[ {}y^{\prime \prime }+2 y^{\prime }+5 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.584











14515

\[ {}{y^{\prime \prime }}^{2}-5 y^{\prime \prime } y^{\prime }+4 y^{2} = 0 \]

2

0

3

unknown

[[_2nd_order, _missing_x]]

N/A

0.355











14516

\[ {}{y^{\prime \prime }}^{2}-2 y^{\prime \prime } y^{\prime }+y^{2} = 0 \]

2

0

4

unknown

[[_2nd_order, _missing_x]]

N/A

0.314











14517

\[ {}y^{\prime \prime }+4 y^{\prime }+3 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.539











14518

\[ {}y^{\prime \prime }+y = 8 \,{\mathrm e}^{2 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.694











14519

\[ {}y^{\prime \prime }-4 y^{\prime }+3 y = -{\mathrm e}^{-9 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.508











14520

\[ {}y^{\prime \prime }-4 y^{\prime }+3 y = 2 \,{\mathrm e}^{3 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.553











14521

\[ {}y^{\prime \prime }-y = 2 t -4 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.496











14522

\[ {}y^{\prime \prime }-2 y^{\prime }+y = t^{2} \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _with_linear_symmetries]]

0.592











14523

\[ {}y^{\prime \prime }+2 y^{\prime } = 3-4 t \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

2.054











14524

\[ {}y^{\prime \prime }+y = \cos \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.089











14525

\[ {}y^{\prime \prime }+4 y = 4 \cos \left (t \right )-\sin \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.691











14526

\[ {}y^{\prime \prime }+4 y = \cos \left (2 t \right )+t \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.235











14527

\[ {}y^{\prime \prime }+4 y = 3 t \,{\mathrm e}^{-t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.744











14528

\[ {}y^{\prime \prime } = 3 t^{4}-2 t \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_ode_quadrature, second_order_linear_constant_coeff

[[_2nd_order, _quadrature]]

0.902











14529

\[ {}y^{\prime \prime }-4 y^{\prime }+13 y = 2 t \,{\mathrm e}^{-2 t} \sin \left (3 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.512











14530

\[ {}y^{\prime \prime }+y^{\prime }-2 y = -1 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.485











14531

\[ {}5 y^{\prime \prime }+y^{\prime }-4 y = -3 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.508











14532

\[ {}y^{\prime \prime }-2 y^{\prime }-8 y = 32 t \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.509











14533

\[ {}16 y^{\prime \prime }-8 y^{\prime }-15 y = 75 t \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.541











14534

\[ {}y^{\prime \prime }+2 y^{\prime }+26 y = -338 t \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

1.02











14535

\[ {}y^{\prime \prime }+3 y^{\prime }-4 y = -32 t^{2} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.566











14536

\[ {}8 y^{\prime \prime }+6 y^{\prime }+y = 5 t^{2} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.559











14537

\[ {}y^{\prime \prime }-6 y^{\prime }+8 y = -256 t^{3} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.552











14538

\[ {}y^{\prime \prime }-2 y^{\prime } = 52 \sin \left (3 t \right ) \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

3.997











14539

\[ {}y^{\prime \prime }-6 y^{\prime }+13 y = 25 \sin \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.119











14540

\[ {}y^{\prime \prime }-9 y = 54 \sin \left (2 t \right ) t \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.024











14541

\[ {}y^{\prime \prime }-5 y^{\prime }+6 y = -78 \cos \left (3 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.682











14542

\[ {}y^{\prime \prime }+4 y^{\prime }+4 y = -32 t^{2} \cos \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

1.672











14543

\[ {}y^{\prime \prime }-y^{\prime }-20 y = -2 \,{\mathrm e}^{t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.52











14544

\[ {}y^{\prime \prime }-4 y^{\prime }-5 y = -648 t^{2} {\mathrm e}^{5 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.655











14545

\[ {}y^{\prime \prime }-7 y^{\prime }+12 y = -2 t^{3} {\mathrm e}^{4 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.604











14546

\[ {}y^{\prime \prime }+4 y^{\prime } = 8 \,{\mathrm e}^{4 t}-4 \,{\mathrm e}^{-4 t} \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

2.337











14547

\[ {}y^{\prime \prime }-3 y^{\prime } = t^{2}-{\mathrm e}^{3 t} \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

2.58











14548

\[ {}y^{\prime \prime }+4 y^{\prime } = -24 t -6-4 t \,{\mathrm e}^{-4 t}+{\mathrm e}^{-4 t} \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

2.517











14549

\[ {}y^{\prime \prime }-3 y^{\prime } = t^{2}-{\mathrm e}^{3 t} \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

2.22











14550

\[ {}y^{\prime \prime } = t^{2}+{\mathrm e}^{t}+\sin \left (t \right ) \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_ode_quadrature, second_order_linear_constant_coeff

[[_2nd_order, _quadrature]]

3.571











14551

\[ {}y^{\prime \prime }+3 y^{\prime } = 18 \]

i.c.

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

2.643











14552

\[ {}y^{\prime \prime }-y = 4 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

5.685











14553

\[ {}y^{\prime \prime }-4 y = 32 t \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.755











14554

\[ {}y^{\prime \prime }+2 y^{\prime }-3 y = -2 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.733











14555

\[ {}y^{\prime \prime }+y^{\prime }-6 y = 3 t \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.772











14556

\[ {}y^{\prime \prime }+8 y^{\prime }+16 y = 4 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.926











14557

\[ {}y^{\prime \prime }+7 y^{\prime }+10 y = t \,{\mathrm e}^{-t} \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.832











14558

\[ {}y^{\prime \prime }+6 y^{\prime }+25 y = -1 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.244











14559

\[ {}y^{\prime \prime }-3 y^{\prime } = -{\mathrm e}^{3 t}-2 t \]

i.c.

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

3.026











14560

\[ {}y^{\prime \prime }-y^{\prime } = -3 t -4 t^{2} {\mathrm e}^{2 t} \]

i.c.

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

3.357











14561

\[ {}y^{\prime \prime }-2 y^{\prime } = 2 t^{2} \]

i.c.

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

2.508











14562

\[ {}y^{\prime \prime }+4 y^{\prime } = -24 t -6-4 t \,{\mathrm e}^{-4 t}+{\mathrm e}^{-4 t} \]

i.c.

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

2.844











14563

\[ {}y^{\prime \prime }-3 y^{\prime } = {\mathrm e}^{-3 t}-{\mathrm e}^{3 t} \]

i.c.

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

3.079











14564

\[ {}y^{\prime \prime }+9 y = \left \{\begin {array}{cc} 2 t & 0\le t <\pi \\ 0 & \pi \le t \end {array}\right . \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

7.708











14565

\[ {}y^{\prime \prime }+9 \pi ^{2} y = \left \{\begin {array}{cc} 2 t & 0\le t <\pi \\ 2 t -2 \pi & \pi \le t <2 \pi \\ 0 & 2 \pi \le t \end {array}\right . \]

i.c.

1

0

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

29.137











14566

\[ {}y^{\prime \prime }+4 y = \left \{\begin {array}{cc} 0 & 0\le t <\pi \\ 10 & \pi \le t <2 \pi \\ 0 & 2 \pi \le t \end {array}\right . \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

5.716











14567

\[ {}y^{\prime }-4 y = t^{2} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.99











14568

\[ {}y^{\prime }+y = \cos \left (2 t \right ) \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.553











14569

\[ {}y^{\prime }-y = {\mathrm e}^{4 t} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.167











14570

\[ {}y^{\prime }+4 y = {\mathrm e}^{-4 t} \]

i.c.

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.237











14571

\[ {}y^{\prime }+4 y = t \,{\mathrm e}^{-4 t} \]

1

1

1

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.985











14572

\[ {}y^{\prime \prime }+y^{\prime }-2 y = f \left (t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.669











14573

\[ {}x^{\prime \prime }+9 x = \sin \left (3 t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.256











14574

\[ {}4 y^{\prime \prime }+4 y^{\prime }+37 y = \cos \left (3 t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.283











14575

\[ {}y^{\prime \prime }+4 y = 1 \]

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

2.166











14576

\[ {}y^{\prime \prime }+16 y^{\prime } = t \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

2.14











14577

\[ {}y^{\prime \prime }-7 y^{\prime }+10 y = {\mathrm e}^{3 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.507











14578

\[ {}y^{\prime \prime }+16 y = 2 \cos \left (4 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.981











14579

\[ {}y^{\prime \prime }+4 y^{\prime }+20 y = 2 t \,{\mathrm e}^{-2 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.75











14580

\[ {}y^{\prime \prime }+\frac {y}{4} = \sec \left (\frac {t}{2}\right )+\csc \left (\frac {t}{2}\right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.672











14581

\[ {}y^{\prime \prime }+16 y = \csc \left (4 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.001











14582

\[ {}y^{\prime \prime }+16 y = \cot \left (4 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.523











14583

\[ {}y^{\prime \prime }+2 y^{\prime }+50 y = {\mathrm e}^{-t} \csc \left (7 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.307











14584

\[ {}y^{\prime \prime }+6 y^{\prime }+25 y = {\mathrm e}^{-3 t} \left (\sec \left (4 t \right )+\csc \left (4 t \right )\right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.216











14585

\[ {}y^{\prime \prime }-2 y^{\prime }+26 y = {\mathrm e}^{t} \left (\sec \left (5 t \right )+\csc \left (5 t \right )\right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.49











14586

\[ {}y^{\prime \prime }+12 y^{\prime }+37 y = {\mathrm e}^{-6 t} \csc \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.991











14587

\[ {}y^{\prime \prime }-6 y^{\prime }+34 y = {\mathrm e}^{3 t} \tan \left (5 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.489











14588

\[ {}y^{\prime \prime }-10 y^{\prime }+34 y = {\mathrm e}^{5 t} \cot \left (3 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.442











14589

\[ {}y^{\prime \prime }-12 y^{\prime }+37 y = {\mathrm e}^{6 t} \sec \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.914











14590

\[ {}y^{\prime \prime }-8 y^{\prime }+17 y = {\mathrm e}^{4 t} \sec \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.895











14591

\[ {}y^{\prime \prime }-9 y = \frac {1}{1+{\mathrm e}^{3 t}} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.72











14592

\[ {}y^{\prime \prime }-25 y = \frac {1}{1-{\mathrm e}^{5 t}} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.772











14593

\[ {}y^{\prime \prime }-y = 2 \sinh \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.128











14594

\[ {}y^{\prime \prime }-2 y^{\prime }+y = \frac {{\mathrm e}^{t}}{t} \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.651











14595

\[ {}y^{\prime \prime }-4 y^{\prime }+4 y = \frac {{\mathrm e}^{2 t}}{t^{2}} \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.666











14596

\[ {}y^{\prime \prime }+8 y^{\prime }+16 y = \frac {{\mathrm e}^{-4 t}}{t^{4}} \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.67











14597

\[ {}y^{\prime \prime }+6 y^{\prime }+9 y = \frac {{\mathrm e}^{-3 t}}{t} \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.662











14598

\[ {}y^{\prime \prime }+6 y^{\prime }+9 y = {\mathrm e}^{-3 t} \ln \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.705











14599

\[ {}y^{\prime \prime }+3 y^{\prime }+2 y = \cos \left ({\mathrm e}^{t}\right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.827











14600

\[ {}y^{\prime \prime }+4 y^{\prime }+4 y = {\mathrm e}^{-2 t} \sqrt {-t^{2}+1} \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.816











14601

\[ {}y^{\prime \prime }-2 y^{\prime }+y = {\mathrm e}^{t} \sqrt {-t^{2}+1} \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.732











14602

\[ {}y^{\prime \prime }-10 y^{\prime }+25 y = {\mathrm e}^{5 t} \ln \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.81











14603

\[ {}y^{\prime \prime }-4 y^{\prime }+4 y = {\mathrm e}^{2 t} \arctan \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.765











14604

\[ {}y^{\prime \prime }+8 y^{\prime }+16 y = \frac {{\mathrm e}^{-4 t}}{t^{2}+1} \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.68











14605

\[ {}y^{\prime \prime }+y = \sec \left (\frac {t}{2}\right )+\csc \left (\frac {t}{2}\right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.872











14606

\[ {}y^{\prime \prime }+9 y = \tan \left (3 t \right )^{2} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.764











14607

\[ {}y^{\prime \prime }+9 y = \sec \left (3 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.02











14608

\[ {}y^{\prime \prime }+9 y = \tan \left (3 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.251











14609

\[ {}y^{\prime \prime }+4 y = \tan \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.305











14610

\[ {}y^{\prime \prime }+16 y = \tan \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.408











14611

\[ {}y^{\prime \prime }+4 y = \tan \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.132











14612

\[ {}y^{\prime \prime }+9 y = \sec \left (3 t \right ) \tan \left (3 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.364











14613

\[ {}y^{\prime \prime }+4 y = \sec \left (2 t \right ) \tan \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.381











14614

\[ {}y^{\prime \prime }+9 y = \frac {\csc \left (3 t \right )}{2} \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.352











14615

\[ {}y^{\prime \prime }+4 y = \sec \left (2 t \right )^{2} \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.241











14616

\[ {}y^{\prime \prime }-16 y = 16 t \,{\mathrm e}^{-4 t} \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.909











14617

\[ {}y^{\prime \prime }+y = \tan \left (t \right )^{2} \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.585











14618

\[ {}y^{\prime \prime }+4 y = \sec \left (2 t \right )+\tan \left (2 t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.411











14619

\[ {}y^{\prime \prime }+9 y = \csc \left (3 t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.619











14620

\[ {}y^{\prime \prime }+4 y^{\prime }+3 y = 65 \cos \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.66











14621

\[ {}t^{2} y^{\prime \prime }+3 t y^{\prime }+y = \ln \left (t \right ) \]

1

1

1

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _exact, _linear, _nonhomogeneous]]

5.294











14622

\[ {}t^{2} y^{\prime \prime }+t y^{\prime }+4 y = t \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

4.547











14623

\[ {}t^{2} y^{\prime \prime }-4 t y^{\prime }-6 y = 2 \ln \left (t \right ) \]

1

1

1

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _exact, _linear, _nonhomogeneous]]

3.653











14624

\[ {}4 y^{\prime \prime }+4 y^{\prime }+y = {\mathrm e}^{-\frac {t}{2}} \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _with_linear_symmetries]]

0.918











14625

\[ {}{\mathrm e}^{-2 t} \left (y y^{\prime \prime }-{y^{\prime }}^{2}\right )-2 t \left (t +1\right ) y = 0 \]

1

0

0

unknown

[NONE]

N/A

0.199











14626

\[ {}y^{\prime \prime }+4 y = f \left (t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.829











14627

\[ {}t^{2} y^{\prime \prime }-4 t y^{\prime }+\left (t^{2}+6\right ) y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.833











14628

\[ {}t^{2} y^{\prime \prime }-4 t y^{\prime }+\left (t^{2}+6\right ) y = t^{3}+2 t \]

i.c.

1

0

1

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _with_linear_symmetries]]

N/A

1.562











14629

\[ {}t y^{\prime \prime }+2 y^{\prime }+t y = 0 \]

1

1

1

reduction_of_order

[_Lienard]

0.618











14630

\[ {}t y^{\prime \prime }+2 y^{\prime }+t y = -t \]

i.c.

1

1

1

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _with_linear_symmetries]]

2.221











14631

\[ {}4 t^{2} y^{\prime \prime }+4 t y^{\prime }+\left (16 t^{2}-1\right ) y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.963











14632

\[ {}4 t^{2} y^{\prime \prime }+4 t y^{\prime }+\left (16 t^{2}-1\right ) y = 16 t^{\frac {3}{2}} \]

i.c.

1

0

0

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _linear, _nonhomogeneous]]

N/A

1.503











14633

\[ {}4 t^{2} y^{\prime \prime }+4 t y^{\prime }+\left (16 t^{2}-1\right ) y = 16 t^{\frac {3}{2}} \]

i.c.

1

1

1

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _linear, _nonhomogeneous]]

2.326











14634

\[ {}t^{2} \left (-1+\ln \left (t \right )\right ) y^{\prime \prime }-t y^{\prime }+y = -\frac {3 \left (1+\ln \left (t \right )\right )}{4 \sqrt {t}} \]

i.c.

1

1

1

second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _with_linear_symmetries]]

3.713











14635

\[ {}\left (\sin \left (t \right )-t \cos \left (t \right )\right ) y^{\prime \prime }-t \sin \left (t \right ) y^{\prime }+y \sin \left (t \right ) = t \]

i.c.

1

1

1

second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

12.105











14636

\[ {}y^{\prime \prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _quadrature]]

0.247











14637

\[ {}y^{\prime \prime \prime }-10 y^{\prime \prime }+25 y^{\prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.362











14638

\[ {}8 y^{\prime \prime \prime }+y^{\prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.292











14639

\[ {}y^{\prime \prime \prime \prime }+16 y^{\prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.44











14640

\[ {}y^{\prime \prime \prime }-2 y^{\prime \prime }-y^{\prime }+2 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.309











14641

\[ {}3 y^{\prime \prime \prime }-4 y^{\prime \prime }-5 y^{\prime }+2 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.333











14642

\[ {}6 y^{\prime \prime \prime }-5 y^{\prime \prime }-2 y^{\prime }+y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.331











14643

\[ {}y^{\prime \prime \prime }-5 y^{\prime }+2 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.378











14644

\[ {}5 y^{\prime \prime \prime }-15 y^{\prime }+11 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

1.82











14645

\[ {}y^{\prime \prime \prime \prime }+y^{\prime \prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.283











14646

\[ {}y^{\prime \prime \prime \prime }-9 y^{\prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.324











14647

\[ {}y^{\prime \prime \prime \prime }-16 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.445











14648

\[ {}y^{\prime \prime \prime \prime }-6 y^{\prime \prime \prime }-y^{\prime \prime }+54 y^{\prime }-72 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.372











14649

\[ {}y^{\prime \prime \prime \prime }+7 y^{\prime \prime \prime }+6 y^{\prime \prime }-32 y^{\prime }-32 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.408











14650

\[ {}y^{\prime \prime \prime \prime }+2 y^{\prime \prime \prime }-2 y^{\prime \prime }+8 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.552











14651

\[ {}y^{\left (5\right )}+4 y^{\prime \prime \prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.324











14652

\[ {}y^{\left (5\right )}+4 y^{\prime \prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.448











14653

\[ {}y^{\left (5\right )}+3 y^{\prime \prime \prime \prime }+3 y^{\prime \prime \prime }+y^{\prime \prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.214











14654

\[ {}y^{\prime \prime \prime \prime }+2 y^{\prime \prime }+y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.215











14655

\[ {}y^{\prime \prime \prime \prime }+8 y^{\prime \prime }+16 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.22











14656

\[ {}y^{\left (6\right )}+3 y^{\prime \prime \prime \prime }+3 y^{\prime \prime }+y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.235











14657

\[ {}y^{\left (6\right )}+12 y^{\prime \prime \prime \prime }+48 y^{\prime \prime }+64 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.239











14658

\[ {}y^{\prime \prime \prime }-2 y^{\prime \prime } = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.457











14659

\[ {}y^{\prime \prime \prime }-y = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

1.256











14660

\[ {}y^{\prime \prime \prime \prime }+16 y^{\prime \prime \prime } = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.584











14661

\[ {}y^{\prime \prime \prime \prime }-8 y^{\prime \prime }+16 y = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.733











14662

\[ {}24 y^{\prime \prime \prime }-26 y^{\prime \prime }+9 y^{\prime }-y = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.561











14663

\[ {}y^{\prime \prime \prime \prime }-5 y^{\prime \prime }+4 y = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.664











14664

\[ {}y^{\prime \prime \prime \prime }-16 y = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.941











14665

\[ {}8 y^{\left (5\right )}+4 y^{\prime \prime \prime \prime }+66 y^{\prime \prime \prime }-41 y^{\prime \prime }-37 y^{\prime } = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

1.342











14666

\[ {}2 y^{\left (5\right )}+7 y^{\prime \prime \prime \prime }+17 y^{\prime \prime \prime }+17 y^{\prime \prime }+5 y^{\prime } = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

1.315











14667

\[ {}y^{\left (5\right )}+8 y^{\prime \prime \prime \prime } = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.637











14668

\[ {}y^{\left (6\right )}-3 y^{\prime \prime \prime \prime }+3 y^{\prime \prime }-y = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.652











14669

\[ {}y^{\prime \prime \prime }+9 y^{\prime \prime }+16 y^{\prime }-26 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.462











14670

\[ {}y^{\prime \prime \prime \prime }+12 y^{\prime \prime \prime }+60 y^{\prime \prime }+124 y^{\prime }+75 y = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.533











14671

\[ {}y^{\prime \prime \prime }+3 y^{\prime \prime }+2 y^{\prime }+6 y = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.985











14672

\[ {}y^{\prime \prime \prime \prime }-8 y^{\prime \prime \prime }+30 y^{\prime \prime }-56 y^{\prime }+49 y = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.968











14673

\[ {}\frac {31 y^{\prime \prime \prime }}{100}+\frac {56 y^{\prime \prime }}{5}-\frac {49 y^{\prime }}{5}+\frac {53 y}{10} = 0 \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

9.282











14674

\[ {}2 y y^{\prime \prime }+y^{2} = {y^{\prime }}^{2} \]

1

2

2

second_order_ode_missing_x

[[_2nd_order, _missing_x], [_2nd_order, _reducible, _mu_xy]]

8.819











14675

\[ {}y^{\prime \prime \prime }+y^{\prime \prime } = {\mathrm e}^{t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

0.25











14676

\[ {}y^{\prime \prime \prime \prime }-16 y = 1 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

2.335











14677

\[ {}y^{\left (5\right )}-y^{\prime \prime \prime \prime } = 1 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.288











14678

\[ {}y^{\prime \prime \prime \prime }+9 y^{\prime \prime } = 1 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.351











14679

\[ {}y^{\prime \prime \prime \prime }+9 y^{\prime \prime } = 9 \,{\mathrm e}^{3 t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_y]]

0.354











14680

\[ {}y^{\prime \prime \prime }+10 y^{\prime \prime }+34 y^{\prime }+40 y = t \,{\mathrm e}^{-4 t}+2 \,{\mathrm e}^{-3 t} \cos \left (t \right ) \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _linear, _nonhomogeneous]]

4.13











14681

\[ {}y^{\prime \prime \prime }+6 y^{\prime \prime }+11 y^{\prime }+6 y = 2 \,{\mathrm e}^{-3 t}-t \,{\mathrm e}^{-t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _linear, _nonhomogeneous]]

0.907











14682

\[ {}y^{\prime \prime \prime \prime }-6 y^{\prime \prime \prime }+13 y^{\prime \prime }-24 y^{\prime }+36 y = 108 t \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _with_linear_symmetries]]

3.791











14683

\[ {}y^{\prime \prime \prime }+6 y^{\prime \prime }-14 y^{\prime }-104 y = -111 \,{\mathrm e}^{t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _with_linear_symmetries]]

2.122











14684

\[ {}y^{\prime \prime \prime \prime }-10 y^{\prime \prime \prime }+38 y^{\prime \prime }-64 y^{\prime }+40 y = 153 \,{\mathrm e}^{-t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _with_linear_symmetries]]

3.254











14685

\[ {}y^{\prime \prime \prime }+4 y^{\prime } = \tan \left (2 t \right ) \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

36.872











14686

\[ {}y^{\prime \prime \prime }+4 y^{\prime } = \sec \left (2 t \right ) \tan \left (2 t \right ) \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

8.023











14687

\[ {}y^{\prime \prime \prime \prime }+4 y^{\prime \prime } = \sec \left (2 t \right )^{2} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_y]]

1.172











14688

\[ {}y^{\prime \prime \prime \prime }+4 y^{\prime \prime } = \tan \left (2 t \right )^{2} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_y]]

1.327











14689

\[ {}y^{\prime \prime \prime }+9 y^{\prime } = \sec \left (3 t \right ) \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

10.88











14690

\[ {}y^{\prime \prime \prime }+y^{\prime } = -\sec \left (t \right ) \tan \left (t \right ) \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

6.128











14691

\[ {}y^{\prime \prime \prime }+4 y^{\prime } = \sec \left (2 t \right ) \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

6.538











14692

\[ {}y^{\prime \prime \prime }-2 y^{\prime \prime } = -\frac {1}{t^{2}}-\frac {2}{t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

0.48











14693

\[ {}y^{\prime \prime \prime }-3 y^{\prime \prime }+3 y^{\prime }-y = \frac {{\mathrm e}^{t}}{t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _linear, _nonhomogeneous]]

0.383











14694

\[ {}y^{\prime \prime \prime }-4 y^{\prime \prime }-11 y^{\prime }+30 y = {\mathrm e}^{4 t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _with_linear_symmetries]]

0.827











14695

\[ {}y^{\prime \prime \prime }+3 y^{\prime \prime }-10 y^{\prime }-24 y = {\mathrm e}^{-3 t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _with_linear_symmetries]]

0.824











14696

\[ {}y^{\prime \prime \prime }-13 y^{\prime }+12 y = \cos \left (t \right ) \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _linear, _nonhomogeneous]]

1.013











14697

\[ {}y^{\prime \prime \prime }+3 y^{\prime \prime }+2 y^{\prime } = \cos \left (t \right ) \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

0.822











14698

\[ {}y^{\left (6\right )}+y^{\prime \prime \prime \prime } = -24 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.375











14699

\[ {}y^{\prime \prime \prime \prime }+y^{\prime \prime } = \tan \left (t \right )^{2} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_y]]

1.138











14700

\[ {}y^{\prime \prime \prime }-y^{\prime \prime } = 3 t^{2} \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

0.507











14701

\[ {}y^{\prime \prime \prime \prime }+y^{\prime \prime } = \sec \left (t \right )^{2} \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_y]]

2.826











14702

\[ {}y^{\prime \prime \prime }+y^{\prime } = \sec \left (t \right ) \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

4.151











14703

\[ {}y^{\prime \prime \prime \prime }+y^{\prime \prime } = \cos \left (t \right ) \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_y]]

1.326











14704

\[ {}y^{\prime \prime \prime \prime }+y^{\prime \prime } = t \]

i.c.

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_y]]

0.818











14705

\[ {}t^{2} \ln \left (t \right ) y^{\prime \prime \prime }-t y^{\prime \prime }+y^{\prime } = 1 \]

1

1

1

higher_order_missing_y

[[_3rd_order, _missing_y]]

1.441











14706

\[ {}\left (t^{2}+t \right ) y^{\prime \prime \prime }+\left (-t^{2}+2\right ) y^{\prime \prime }-\left (2+t \right ) y^{\prime } = -2-t \]

1

1

1

higher_order_missing_y

[[_3rd_order, _missing_y]]

1.491











14707

\[ {}2 t^{3} y^{\prime \prime \prime }+t^{2} y^{\prime \prime }+t y^{\prime }-y = -3 t^{2} \]

i.c.

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.793











14708

\[ {}t y^{\prime \prime \prime \prime }+2 y^{\prime \prime \prime } = \frac {45}{8 t^{\frac {7}{2}}} \]

i.c.

1

0

1

unknown

[[_high_order, _missing_y]]

N/A

1.443











14709

\[ {}4 x^{2} y^{\prime \prime }-8 x y^{\prime }+5 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.299











14710

\[ {}3 x^{2} y^{\prime \prime }-4 x y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.232











14711

\[ {}2 x^{2} y^{\prime \prime }-8 x y^{\prime }+8 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_Emden, _Fowler]]

2.76











14712

\[ {}2 x^{2} y^{\prime \prime }-7 x y^{\prime }+7 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_Emden, _Fowler]]

2.839











14713

\[ {}4 x^{2} y^{\prime \prime }+17 y = 0 \]

1

1

1

kovacic, second_order_euler_ode

[[_Emden, _Fowler]]

0.803











14714

\[ {}9 x^{2} y^{\prime \prime }-9 x y^{\prime }+10 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.359











14715

\[ {}2 x^{2} y^{\prime \prime }-2 x y^{\prime }+20 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.325











14716

\[ {}x^{2} y^{\prime \prime }-5 x y^{\prime }+10 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.247











14717

\[ {}4 x^{2} y^{\prime \prime }+8 x y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.172











14718

\[ {}4 x^{2} y^{\prime \prime }+y = 0 \]

1

1

1

kovacic, second_order_euler_ode

[[_Emden, _Fowler]]

0.613











14719

\[ {}x^{2} y^{\prime \prime }-5 x y^{\prime }+9 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.172











14720

\[ {}x^{2} y^{\prime \prime }+7 x y^{\prime }+9 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.17











14721

\[ {}x^{3} y^{\prime \prime \prime }+22 x^{2} y^{\prime \prime }+124 x y^{\prime }+140 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.567











14722

\[ {}x^{3} y^{\prime \prime \prime }-4 x^{2} y^{\prime \prime }-46 x y^{\prime }+100 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.564











14723

\[ {}x^{3} y^{\prime \prime \prime }+2 x^{2} y^{\prime \prime }-4 x y^{\prime }+4 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.55











14724

\[ {}x^{3} y^{\prime \prime \prime }+4 x^{2} y^{\prime \prime }+6 x y^{\prime }+4 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _exact, _linear, _homogeneous]]

0.681











14725

\[ {}x^{3} y^{\prime \prime \prime }+2 x y^{\prime }-2 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.665











14726

\[ {}x^{3} y^{\prime \prime \prime }+3 x^{2} y^{\prime \prime }-2 x y^{\prime }-2 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _exact, _linear, _homogeneous]]

0.598











14727

\[ {}x^{3} y^{\prime \prime \prime }+6 x^{2} y^{\prime \prime }+7 x y^{\prime }+y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _exact, _linear, _homogeneous]]

0.341











14728

\[ {}x^{3} y^{\prime \prime \prime \prime }+6 x^{2} y^{\prime \prime \prime }+7 x y^{\prime \prime }+y^{\prime } = 0 \]

1

1

1

higher_order_missing_y

[[_high_order, _missing_y]]

0.823











14729

\[ {}x^{2} y^{\prime \prime }+5 x y^{\prime }+4 y = \frac {1}{x^{5}} \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

2.681











14730

\[ {}x^{2} y^{\prime \prime }-5 x y^{\prime }+9 y = x^{3} \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

3.467











14731

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+y = \frac {1}{x^{2}} \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

9.394











14732

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+4 y = \frac {1}{x^{2}} \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

9.445











14733

\[ {}x^{2} y^{\prime \prime }+2 x y^{\prime }-6 y = 2 x \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

1.912











14734

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }-16 y = \ln \left (x \right ) \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

2.49











14735

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+4 y = 8 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

5.369











14736

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+36 y = x^{2} \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

7.129











14737

\[ {}x^{3} y^{\prime \prime \prime }+3 x^{2} y^{\prime \prime }-11 x y^{\prime }+16 y = \frac {1}{x^{3}} \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.496











14738

\[ {}x^{3} y^{\prime \prime \prime }+16 x^{2} y^{\prime \prime }+70 x y^{\prime }+80 y = \frac {1}{x^{13}} \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.501











14739

\[ {}3 x^{2} y^{\prime \prime }-4 x y^{\prime }+2 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

4.274











14740

\[ {}2 x^{2} y^{\prime \prime }-7 x y^{\prime }+7 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_Emden, _Fowler]]

5.136











14741

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+4 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.483











14742

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+2 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

4.565











14743

\[ {}x^{3} y^{\prime \prime \prime }+10 x^{2} y^{\prime \prime }-20 x y^{\prime }+20 y = 0 \]

i.c.

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.826











14744

\[ {}x^{3} y^{\prime \prime \prime }+15 x^{2} y^{\prime \prime }+54 x y^{\prime }+42 y = 0 \]

i.c.

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.832











14745

\[ {}x^{3} y^{\prime \prime \prime }-2 x^{2} y^{\prime \prime }+5 x y^{\prime }-5 y = 0 \]

i.c.

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

1.302











14746

\[ {}x^{3} y^{\prime \prime \prime }-6 x^{2} y^{\prime \prime }+17 x y^{\prime }-17 y = 0 \]

i.c.

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

1.346











14747

\[ {}2 x^{2} y^{\prime \prime }+3 x y^{\prime }-y = \frac {1}{x^{2}} \]

i.c.

1

1

1

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _exact, _linear, _nonhomogeneous]]

4.778











14748

\[ {}x^{2} y^{\prime \prime }+4 x y^{\prime }+2 y = \ln \left (x \right ) \]

i.c.

1

1

1

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_1, second_order_change_of_variable_on_y_method_2, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _exact, _linear, _nonhomogeneous]]

8.766











14749

\[ {}4 x^{2} y^{\prime \prime }+y = x^{3} \]

i.c.

1

1

1

kovacic, second_order_euler_ode

[[_2nd_order, _with_linear_symmetries]]

1.23











14750

\[ {}9 x^{2} y^{\prime \prime }+27 x y^{\prime }+10 y = \frac {1}{x} \]

i.c.

1

0

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

11.657











14751

\[ {}x^{2} y^{\prime \prime }-x y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.231











14752

\[ {}x^{2} y^{\prime \prime }+4 x y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_1, second_order_change_of_variable_on_y_method_2, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _exact, _linear, _homogeneous]]

4.191











14753

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

1.844











14754

\[ {}x^{3} y^{\prime \prime \prime }+3 x^{2} y^{\prime \prime }+37 x y^{\prime } = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _missing_y]]

0.673











14755

\[ {}x^{3} y^{\prime \prime \prime }+3 x^{2} y^{\prime \prime }-3 x y^{\prime } = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _missing_y]]

0.546











14756

\[ {}x^{3} y^{\prime \prime \prime }+x y^{\prime }-y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.329











14757

\[ {}x^{3} y^{\prime \prime \prime }+3 x^{2} y^{\prime \prime }-3 x y^{\prime } = -8 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _missing_y]]

0.438











14758

\[ {}\left (x^{2}+1\right )^{2} y^{\prime \prime }+2 x \left (x^{2}+1\right ) y^{\prime }+4 y = 0 \]

1

1

1

kovacic, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _with_linear_symmetries], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.355











14759

\[ {}\left (x^{2}+1\right )^{2} y^{\prime \prime }+2 x \left (x^{2}+1\right ) y^{\prime }+4 y = \arctan \left (x \right ) \]

1

1

1

kovacic, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _linear, _nonhomogeneous]]

2.633











14760

\[ {}\left (x^{2}+1\right )^{2} y^{\prime \prime }+2 x \left (x^{2}+1\right ) y^{\prime }+4 y = 0 \]

i.c.

1

1

1

kovacic, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _with_linear_symmetries], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.166











14761

\[ {}\left (x^{2}+1\right )^{2} y^{\prime \prime }+2 x \left (x^{2}+1\right ) y^{\prime }+4 y = \arctan \left (x \right ) \]

i.c.

1

1

1

kovacic, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _linear, _nonhomogeneous]]

3.023











14762

\[ {}\left (x^{4}-1\right ) y^{\prime \prime }+\left (x^{3}-x \right ) y^{\prime }+\left (x^{2}-1\right ) y = 0 \]

1

1

1

kovacic, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _with_linear_symmetries], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

1.791











14763

\[ {}\left (x^{4}-1\right ) y^{\prime \prime }+\left (x^{3}-x \right ) y^{\prime }+\left (4 x^{2}-4\right ) y = 0 \]

1

1

1

kovacic, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _with_linear_symmetries], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

1.724











14764

\[ {}\left (x^{4}-1\right ) y^{\prime \prime }+\left (x^{3}-x \right ) y^{\prime }+\left (x^{2}-1\right ) y = 0 \]

i.c.

1

1

1

kovacic, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _with_linear_symmetries], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

1.668











14765

\[ {}x^{2} y^{\prime \prime }+4 x y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_1, second_order_change_of_variable_on_y_method_2, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _exact, _linear, _homogeneous]]

4.118











14766

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+y = x^{2} \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

4.156











14767

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+4 y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.634











14768

\[ {}x^{2} y^{\prime \prime }-x y^{\prime }+y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_Emden, _Fowler]]

3.135











14769

\[ {}x^{3} y^{\prime \prime \prime }+16 x^{2} y^{\prime \prime }+79 x y^{\prime }+125 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.75











14770

\[ {}x^{4} y^{\prime \prime \prime \prime }+5 x^{3} y^{\prime \prime \prime }-12 x^{2} y^{\prime \prime }-12 x y^{\prime }+48 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_high_order, _with_linear_symmetries]]

0.704











14771

\[ {}x^{4} y^{\prime \prime \prime \prime }+14 x^{3} y^{\prime \prime \prime }+55 x^{2} y^{\prime \prime }+65 x y^{\prime }+15 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_high_order, _exact, _linear, _homogeneous]]

0.903











14772

\[ {}x^{4} y^{\prime \prime \prime \prime }+8 x^{3} y^{\prime \prime \prime }+27 x^{2} y^{\prime \prime }+35 x y^{\prime }+45 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_high_order, _with_linear_symmetries]]

1.339











14773

\[ {}x^{4} y^{\prime \prime \prime \prime }+10 x^{3} y^{\prime \prime \prime }+27 x^{2} y^{\prime \prime }+21 x y^{\prime }+4 y = 0 \]

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_high_order, _with_linear_symmetries]]

0.398











14774

\[ {}x^{3} y^{\prime \prime \prime }+9 x^{2} y^{\prime \prime }+44 x y^{\prime }+58 y = 0 \]

i.c.

1

1

1

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

1.306











14775

\[ {}6 x^{2} y^{\prime \prime }+5 x y^{\prime }-y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.089











14776

\[ {}x^{2} y^{\prime \prime }-2 x y^{\prime }+7 y = 0 \]

1

1

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_Emden, _Fowler]]

1.577











14777

\[ {}\left (-2+x \right ) y^{\prime \prime }+y^{\prime }-y = 0 \]

1

1

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

1.383











14778

\[ {}\left (x^{2}-4\right ) y^{\prime \prime }+16 \left (2+x \right ) y^{\prime }-y = 0 \]

1

1

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

15.529











14779

\[ {}y^{\prime \prime }+3 y^{\prime }-18 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _missing_x]]

1.031











14780

\[ {}y^{\prime \prime }-11 y^{\prime }+30 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _missing_x]]

1.037











14781

\[ {}y^{\prime \prime }+y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _missing_x]]

0.655











14782

\[ {}y^{\prime \prime }-y^{\prime }-2 y = {\mathrm e}^{-x} \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

1.111











14783

\[ {}\left (-2 x -2\right ) y^{\prime \prime }+2 y^{\prime }+4 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

1.113











14784

\[ {}\left (3 x +2\right ) y^{\prime \prime }+3 x y^{\prime } = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _missing_y]]

1.095











14785

\[ {}\left (1+3 x \right ) y^{\prime \prime }-3 y^{\prime }-2 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

1.133











14786

\[ {}\left (-x^{2}+2\right ) y^{\prime \prime }+2 \left (-1+x \right ) y^{\prime }+4 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _exact, _linear, _homogeneous]]

1.313











14787

\[ {}y^{\prime \prime }-x y^{\prime }+4 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[_Hermite]

0.263











14788

\[ {}\left (2 x^{2}+2\right ) y^{\prime \prime }+2 x y^{\prime }-3 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

0.904











14789

\[ {}\left (3-2 x \right ) y^{\prime \prime }+2 y^{\prime }-2 y = 0 \]

i.c.

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

4.09











14790

\[ {}y^{\prime \prime }-4 x^{2} y = 0 \]

i.c.

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_Emden, _Fowler]]

2.684











14791

\[ {}\left (2 x^{2}-1\right ) y^{\prime \prime }+2 x y^{\prime }-3 y = 0 \]

i.c.

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[_Gegenbauer, [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.914











14792

\[ {}y^{\prime \prime }+x y^{\prime } = \sin \left (x \right ) \]

i.c.

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _missing_y]]

3.002











14793

\[ {}y^{\prime \prime }+y^{\prime }+x y = \cos \left (x \right ) \]

i.c.

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _linear, _nonhomogeneous]]

3.41











14794

\[ {}y^{\prime \prime }+\left (y^{2}-1\right ) y^{\prime }+y = 0 \]

i.c.

1

1

1

second order series method. Taylor series method

[[_2nd_order, _missing_x], _Van_der_Pol]

2.422











14795

\[ {}y^{\prime \prime }+\left (\frac {{y^{\prime }}^{2}}{3}-1\right ) y^{\prime }+y = 0 \]

i.c.

1

1

1

second order series method. Taylor series method

[[_2nd_order, _missing_x]]

2.365











14796

\[ {}y^{\prime \prime }-2 x y^{\prime }+2 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

0.977











14797

\[ {}y^{\prime \prime }-2 x y^{\prime }+6 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

0.855











14798

\[ {}\left (-x^{2}+1\right ) y^{\prime \prime }-x y^{\prime }+y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _exact, _linear, _homogeneous]]

0.996











14799

\[ {}\left (-x^{2}+1\right ) y^{\prime \prime }-x y^{\prime }+9 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[_Gegenbauer, [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

0.999











14800

\[ {}y^{\prime \prime }-y \cos \left (x \right ) = \sin \left (x \right ) \]

i.c.

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _linear, _nonhomogeneous]]

4.432











14801

\[ {}x^{2} y^{\prime \prime }+6 y = 0 \]

1

1

1

second order series method. Regular singular point. Complex roots

[[_Emden, _Fowler]]

1.183











14802

\[ {}x \left (1+x \right ) y^{\prime \prime }+\frac {y^{\prime }}{x^{2}}+5 y = 0 \]

1

0

0

second order series method. Irregular singular point

[[_2nd_order, _with_linear_symmetries]]

N/A

5.925











14803

\[ {}\left (x^{2}-3 x -4\right ) y^{\prime \prime }-\left (1+x \right ) y^{\prime }+\left (x^{2}-1\right ) y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

1.627











14804

\[ {}\left (x^{2}-25\right )^{2} y^{\prime \prime }-\left (x +5\right ) y^{\prime }+10 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

9.745











14805

\[ {}2 x y^{\prime \prime }-5 y^{\prime }-3 y = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[[_Emden, _Fowler]]

1.558











14806

\[ {}5 x y^{\prime \prime }+8 y^{\prime }-x y = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[[_2nd_order, _with_linear_symmetries]]

1.401











14807

\[ {}9 x y^{\prime \prime }+14 y^{\prime }+\left (-1+x \right ) y = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[[_2nd_order, _with_linear_symmetries]]

1.966











14808

\[ {}7 x y^{\prime \prime }+10 y^{\prime }+\left (-x^{2}+1\right ) y = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[[_2nd_order, _with_linear_symmetries]]

3.066











14809

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+\left (-1+x \right ) y = 0 \]

1

1

1

second order series method. Regular singular point. Difference is integer

[[_2nd_order, _with_linear_symmetries]]

3.704











14810

\[ {}x y^{\prime \prime }+2 x y^{\prime }+y = 0 \]

1

1

1

second order series method. Regular singular point. Difference is integer

[[_2nd_order, _with_linear_symmetries]]

4.007











14811

\[ {}y^{\prime \prime }+\frac {8 y^{\prime }}{3 x}-\left (\frac {2}{3 x^{2}}-1\right ) y = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[[_2nd_order, _with_linear_symmetries]]

1.533











14812

\[ {}y^{\prime \prime }+\left (\frac {16}{3 x}-1\right ) y^{\prime }-\frac {16 y}{3 x^{2}} = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[[_2nd_order, _exact, _linear, _homogeneous]]

1.69











14813

\[ {}y^{\prime \prime }+\left (\frac {1}{2 x}-2\right ) y^{\prime }-\frac {35 y}{16 x^{2}} = 0 \]

1

1

1

second order series method. Regular singular point. Difference is integer

[[_2nd_order, _with_linear_symmetries]]

4.348











14814

\[ {}y^{\prime \prime }-\left (\frac {1}{x}+2\right ) y^{\prime }+\left (x +\frac {1}{x^{2}}\right ) y = 0 \]

1

1

1

second order series method. Regular singular point. Repeated root

[[_2nd_order, _with_linear_symmetries]]

2.827











14815

\[ {}x^{2} y^{\prime \prime }+7 x y^{\prime }-7 y = 0 \]

1

1

1

second order series method. Regular singular point. Difference is integer

[[_Emden, _Fowler]]

1.222











14816

\[ {}x^{2} y^{\prime \prime }+3 x y^{\prime }+y = 0 \]

1

1

1

second order series method. Regular singular point. Repeated root

[[_2nd_order, _exact, _linear, _homogeneous]]

1.137











14817

\[ {}x^{2} y^{\prime \prime }-3 x y^{\prime }+4 y = 0 \]

1

1

1

second order series method. Regular singular point. Repeated root

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

1.024











14818

\[ {}y^{\prime \prime }+x y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_Emden, _Fowler]]

0.681











14819

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+\left (-k^{2}+x^{2}\right ) y = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[_Bessel]

2.056











14820

\[ {}\left (-x^{2}+1\right ) y^{\prime \prime }-2 x y^{\prime }+k \left (k +1\right ) y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[_Gegenbauer]

1.566











14821

\[ {}x \left (1-x \right ) y^{\prime \prime }+\left (\frac {1}{2}-3 x \right ) y^{\prime }-y = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[[_2nd_order, _exact, _linear, _homogeneous]]

1.63











14822

\[ {}x \left (1-x \right ) y^{\prime \prime }+y^{\prime }+2 y = 0 \]

1

1

1

second order series method. Regular singular point. Repeated root

[[_2nd_order, _exact, _linear, _homogeneous]]

1.405











14823

\[ {}x \left (1-x \right ) y^{\prime \prime }+\left (1-2 x \right ) y^{\prime }+2 y = 0 \]

1

1

1

second order series method. Regular singular point. Repeated root

[_Jacobi]

1.47











14824

\[ {}x y^{\prime \prime }+\left (1-x \right ) y^{\prime }+k y = 0 \]

1

1

1

second order series method. Regular singular point. Repeated root

[_Laguerre]

1.949











14825

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+\left (x^{2}-\frac {1}{4}\right ) y = 0 \]

1

1

1

second order series method. Regular singular point. Difference is integer

[[_2nd_order, _with_linear_symmetries]]

1.449











14826

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+\left (16 x^{2}-25\right ) y = 0 \]

1

1

1

second order series method. Regular singular point. Difference is integer

[[_2nd_order, _with_linear_symmetries]]

3.785











14827

\[ {}y^{\prime \prime }-7 y^{\prime }+10 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.341











14828

\[ {}y^{\prime \prime }-y^{\prime }-2 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.333











14829

\[ {}y^{\prime \prime }-2 y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.562











14830

\[ {}\left (t +1\right )^{2} y^{\prime \prime }-2 \left (t +1\right ) y^{\prime }+2 y = 0 \]

1

1

1

reduction_of_order

[[_2nd_order, _with_linear_symmetries], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

0.749











14831

\[ {}t y^{\prime \prime }+2 y^{\prime }+t y = 0 \]

1

1

1

reduction_of_order

[_Lienard]

0.674











14832

\[ {}y^{\prime \prime }+7 y^{\prime }+10 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.357











14833

\[ {}6 y^{\prime \prime }+5 y^{\prime }-4 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.366











14834

\[ {}y^{\prime \prime }+2 y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.414











14835

\[ {}y^{\prime \prime }+3 y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.345











14836

\[ {}y^{\prime \prime }-10 y^{\prime }+34 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.772











14837

\[ {}2 y^{\prime \prime }-5 y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.362











14838

\[ {}15 y^{\prime \prime }-11 y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.365











14839

\[ {}20 y^{\prime \prime }+y^{\prime }-y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.366











14840

\[ {}12 y^{\prime \prime }+8 y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.359











14841

\[ {}2 y^{\prime \prime \prime }+3 y^{\prime \prime }+y^{\prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.329











14842

\[ {}9 y^{\prime \prime \prime }+36 y^{\prime \prime }+40 y^{\prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.503











14843

\[ {}9 y^{\prime \prime \prime }+12 y^{\prime \prime }+13 y^{\prime } = 0 \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.5











14844

\[ {}y^{\prime \prime }-2 y^{\prime }-8 y = -t \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.536











14845

\[ {}y^{\prime \prime }+5 y^{\prime } = 5 t^{2} \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

2.464











14846

\[ {}y^{\prime \prime }-4 y^{\prime } = -3 \sin \left (t \right ) \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

3.441











14847

\[ {}y^{\prime \prime }+2 y^{\prime }+5 y = 3 \sin \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.237











14848

\[ {}y^{\prime \prime }-9 y = \frac {1}{1+{\mathrm e}^{3 t}} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.692











14849

\[ {}y^{\prime \prime }-2 y^{\prime } = \frac {1}{{\mathrm e}^{2 t}+1} \]

1

1

1

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y, second_order_linear_constant_coeff

[[_2nd_order, _missing_y]]

3.274











14850

\[ {}y^{\prime \prime }-3 y^{\prime }+2 y = -4 \,{\mathrm e}^{-2 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.534











14851

\[ {}y^{\prime \prime }-6 y^{\prime }+13 y = 3 \,{\mathrm e}^{-2 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

1.025











14852

\[ {}y^{\prime \prime }+9 y^{\prime }+20 y = -2 t \,{\mathrm e}^{t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.578











14853

\[ {}y^{\prime \prime }+7 y^{\prime }+12 y = 3 t^{2} {\mathrm e}^{-4 t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.593











14854

\[ {}y^{\prime \prime \prime }+3 y^{\prime \prime }-9 y^{\prime }+5 y = {\mathrm e}^{t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _with_linear_symmetries]]

0.766











14855

\[ {}y^{\prime \prime \prime }-12 y^{\prime }-16 y = {\mathrm e}^{4 t}-{\mathrm e}^{-2 t} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _linear, _nonhomogeneous]]

0.961











14856

\[ {}y^{\prime \prime \prime \prime }+6 y^{\prime \prime \prime }+18 y^{\prime \prime }+30 y^{\prime }+25 y = {\mathrm e}^{-t} \cos \left (2 t \right )+{\mathrm e}^{-2 t} \sin \left (t \right ) \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _linear, _nonhomogeneous]]

53.383











14857

\[ {}y^{\prime \prime \prime \prime }+4 y^{\prime \prime \prime }+14 y^{\prime \prime }+20 y^{\prime }+25 y = t^{2} \]

1

1

1

higher_order_linear_constant_coefficients_ODE

[[_high_order, _with_linear_symmetries]]

0.361











14858

\[ {}y^{\prime \prime }+5 y^{\prime }+6 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.646











14859

\[ {}y^{\prime \prime }+10 y^{\prime }+16 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.624











14860

\[ {}y^{\prime \prime }+16 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

4.389











14861

\[ {}y^{\prime \prime }+25 y = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

4.296











14862

\[ {}y^{\prime \prime }-4 y = t \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.78











14863

\[ {}y^{\prime \prime }+3 y^{\prime }-4 y = {\mathrm e}^{t} \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.86











14864

\[ {}y^{\prime \prime }+9 y = \sin \left (3 t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.433











14865

\[ {}y^{\prime \prime }+y = \cos \left (t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.142











14866

\[ {}y^{\prime \prime }+4 y = \tan \left (2 t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.158











14867

\[ {}y^{\prime \prime }+y = \csc \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.833











14868

\[ {}y^{\prime \prime }-8 y^{\prime }+16 y = \frac {{\mathrm e}^{4 t}}{t^{3}} \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.697











14869

\[ {}y^{\prime \prime }-8 y^{\prime }+16 y = \frac {{\mathrm e}^{4 t}}{t^{3}} \]

i.c.

1

0

0

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

N/A

0.809











14870

\[ {}y^{\prime \prime }-2 y^{\prime }+y = {\mathrm e}^{t} \ln \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.706











14871

\[ {}y^{\prime \prime }-2 y^{\prime }+y = {\mathrm e}^{t} \ln \left (t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

1.311











14872

\[ {}y^{\prime \prime }-2 t y^{\prime }+t^{2} y = 0 \]

1

1

1

kovacic, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _with_linear_symmetries]]

1.487











14873

\[ {}y^{\prime \prime }+3 y^{\prime }-4 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.351











14874

\[ {}y^{\prime \prime }+4 y^{\prime }+4 y = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.41











14875

\[ {}t^{2} y^{\prime \prime }-5 t y^{\prime }+5 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_Emden, _Fowler]]

3.047











14876

\[ {}x^{2} y^{\prime \prime }+7 x y^{\prime }+8 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.328











14877

\[ {}x^{2} y^{\prime \prime }-4 x y^{\prime }+6 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_1, second_order_change_of_variable_on_y_method_2, linear_second_order_ode_solved_by_an_integrating_factor

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.554











14878

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

2.039











14879

\[ {}2 x^{2} y^{\prime \prime }+5 x y^{\prime }+y = 0 \]

i.c.

1

1

1

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _exact, _linear, _homogeneous]]

6.456











14880

\[ {}5 x^{2} y^{\prime \prime }-x y^{\prime }+2 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.429











14881

\[ {}x^{2} y^{\prime \prime }-7 x y^{\prime }+25 y = 0 \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_Emden, _Fowler]]

2.359











14882

\[ {}x^{2} y^{\prime \prime }-7 x y^{\prime }+15 y = 8 x \]

1

1

1

kovacic, second_order_euler_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

2.712











14883

\[ {}y^{\prime \prime }-4 y^{\prime }+4 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _missing_x]]

1.025











14884

\[ {}y^{\prime \prime }+2 y^{\prime }-3 y = x \,{\mathrm e}^{x} \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _linear, _nonhomogeneous]]

1.16











14885

\[ {}\left (2 x^{2}-1\right ) y^{\prime \prime }+2 x y^{\prime }-3 y = 0 \]

1

2

1

second order series method. Ordinary point, second order series method. Taylor series method

[_Gegenbauer, [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

1.023











14886

\[ {}3 x y^{\prime \prime }+11 y^{\prime }-y = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[[_Emden, _Fowler]]

1.482











14887

\[ {}2 x^{2} y^{\prime \prime }+5 x y^{\prime }-2 y = 0 \]

1

1

1

second order series method. Regular singular point. Difference not integer

[[_Emden, _Fowler], [_2nd_order, _linear, ‘_with_symmetry_[0,F(x)]‘]]

1.13











14888

\[ {}x^{2} y^{\prime \prime }-7 x y^{\prime }+\left (-2 x^{2}+7\right ) y = 0 \]

1

1

1

second order series method. Regular singular point. Difference is integer

[[_2nd_order, _with_linear_symmetries]]

3.89











14889

\[ {}x \left (1-x \right ) y^{\prime \prime }+\left (2 x +1\right ) y^{\prime }+10 y = 0 \]

1

1

1

second order series method. Regular singular point. Repeated root

[_Jacobi]

1.582











14890

\[ {}x \left (1+x \right ) y^{\prime \prime }+\left (1-2 x \right ) y^{\prime }-10 y = 0 \]

1

1

1

second order series method. Regular singular point. Repeated root

[[_2nd_order, _with_linear_symmetries]]

1.648











14891

\[ {}t \left (y y^{\prime \prime }+{y^{\prime }}^{2}\right )+y y^{\prime } = 1 \]

i.c.

1

1

1

second_order_integrable_as_is

[[_2nd_order, _exact, _nonlinear], [_2nd_order, _with_linear_symmetries], [_2nd_order, _reducible, _mu_y_y1], [_2nd_order, _reducible, _mu_xy]]

1.648











14892

\[ {}4 x^{\prime \prime }+9 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

8.311











14893

\[ {}9 x^{\prime \prime }+4 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

7.336











14894

\[ {}x^{\prime \prime }+64 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

16.018











14895

\[ {}x^{\prime \prime }+100 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

11.646











14896

\[ {}x^{\prime \prime }+x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

6.997











14897

\[ {}x^{\prime \prime }+4 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

6.296











14898

\[ {}x^{\prime \prime }+16 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

8.678











14899

\[ {}x^{\prime \prime }+256 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

27.919











14900

\[ {}x^{\prime \prime }+9 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

6.13











14901

\[ {}10 x^{\prime \prime }+\frac {x}{10} = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

6.366











14902

\[ {}x^{\prime \prime }+4 x^{\prime }+3 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.626











14903

\[ {}\frac {x^{\prime \prime }}{32}+2 x^{\prime }+x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.11











14904

\[ {}\frac {x^{\prime \prime }}{4}+2 x^{\prime }+x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.369











14905

\[ {}4 x^{\prime \prime }+2 x^{\prime }+8 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.602











14906

\[ {}x^{\prime \prime }+4 x^{\prime }+13 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.007











14907

\[ {}x^{\prime \prime }+4 x^{\prime }+20 x = 0 \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.061











14908

\[ {}x^{\prime \prime }+x = \left \{\begin {array}{cc} 1 & 0\le t <\pi \\ 0 & \pi \le t \end {array}\right . \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

6.295











14909

\[ {}x^{\prime \prime }+x = \left \{\begin {array}{cc} \cos \left (t \right ) & 0\le t <\pi \\ 0 & \pi \le t \end {array}\right . \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

10.138











14910

\[ {}x^{\prime \prime }+x = \left \{\begin {array}{cc} t & 0\le t <1 \\ 2-t & 1\le t <2 \\ 0 & 2\le t \end {array}\right . \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

8.455











14911

\[ {}x^{\prime \prime }+4 x^{\prime }+13 x = \left \{\begin {array}{cc} 1 & 0\le t <\pi \\ 1-t & \pi \le t <2 \pi \\ 0 & 2 \pi \le t \end {array}\right . \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

30.017











14912

\[ {}x^{\prime \prime }+x = \cos \left (t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.033











14913

\[ {}x^{\prime \prime }+x = \cos \left (t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.839











14914

\[ {}x^{\prime \prime }+x = \cos \left (\frac {9 t}{10}\right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.942











14915

\[ {}x^{\prime \prime }+x = \cos \left (\frac {7 t}{10}\right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.887











14916

\[ {}x^{\prime \prime }+\frac {x^{\prime }}{10}+x = 3 \cos \left (2 t \right ) \]

i.c.

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

3.029











14917

\[ {}\left [\begin {array}{c} x^{\prime }=6 \\ y^{\prime }=\cos \left (t \right ) \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

0.715











14918

\[ {}\left [\begin {array}{c} x^{\prime }=x \\ y^{\prime }=1 \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

0.76











14919

\[ {}\left [\begin {array}{c} x^{\prime }=0 \\ y^{\prime }=-2 y \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

0.281











14920

\[ {}\left [\begin {array}{c} x^{\prime }=x^{2} \\ y^{\prime }={\mathrm e}^{t} \end {array}\right ] \]

1

0

2

system of linear ODEs

system of linear ODEs

N/A

0.339











14921

\[ {}\left [\begin {array}{c} x_{1}^{\prime }=-3 x_{1} \\ x_{2}^{\prime }=1 \end {array}\right ] \]

i.c.

1

1

2

system of linear ODEs

system of linear ODEs

0.663











14922

\[ {}\left [\begin {array}{c} x_{1}^{\prime }=-x_{1}+1 \\ x_{2}^{\prime }=x_{2} \end {array}\right ] \]

i.c.

1

1

2

system of linear ODEs

system of linear ODEs

0.655











14923

\[ {}\left [\begin {array}{c} x^{\prime }=-3 x+6 y \\ y^{\prime }=4 x-y \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

0.449











14924

\[ {}\left [\begin {array}{c} x^{\prime }=8 x-y \\ y^{\prime }=x+6 y \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

0.408











14925

\[ {}\left [\begin {array}{c} x^{\prime }=-x-2 y \\ y^{\prime }=x+y \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

0.577











14926

\[ {}\left [\begin {array}{c} x^{\prime }=4 x+2 y \\ y^{\prime }=-x+2 y \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

0.635











14927

\[ {}\left [\begin {array}{c} x^{\prime }=y \\ y^{\prime }=-x+1 \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

1.323











14928

\[ {}\left [\begin {array}{c} x^{\prime }=y \\ y^{\prime }=-x+\sin \left (2 t \right ) \end {array}\right ] \]

1

1

2

system of linear ODEs

system of linear ODEs

1.405











14929

\[ {}x^{\prime \prime }-3 x^{\prime }+4 x = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.845











14930

\[ {}x^{\prime \prime }+6 x^{\prime }+9 x = 0 \]

1

1

1

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.439











14931

\[ {}x^{\prime \prime }+16 x = t \sin \left (t \right ) \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.638











14932

\[ {}x^{\prime \prime }+x = {\mathrm e}^{t} \]

1

1

1

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.738