2.16.113 Problems 11201 to 11300

Table 2.242: Main lookup table. Sorted sequentially by problem number.

#

ODE

Program classification

CAS classification

Solved?

Verified?

time (sec)

11201

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

quadrature

[_quadrature]

0.601

11202

\[ {}\left (2 x y^{\prime }-y\right )^{2} = 8 x^{3} \]

linear

[_linear]

0.988

11203

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

quadrature

[_quadrature]

0.446

11204

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

linear, quadrature

[_quadrature]

0.855

11205

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

dAlembert

[[_1st_order, _with_linear_symmetries], _dAlembert]

1.593

11206

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

dAlembert

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

0.349

11207

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

dAlembert

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

0.381

11208

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

riccati, first_order_ode_lie_symmetry_calculated

[[_homogeneous, ‘class C‘], _Riccati]

2.116

11209

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

first_order_ode_lie_symmetry_calculated

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

5.934

11210

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

dAlembert

[[_1st_order, _with_linear_symmetries], _dAlembert]

0.498

11211

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

dAlembert

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

140.131

11212

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

dAlembert

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

0.736

11213

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

dAlembert

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

0.397

11214

\[ {}{y^{\prime }}^{3}-4 x y y^{\prime }+8 y^{2} = 0 \]

first_order_ode_lie_symmetry_calculated

[[_1st_order, _with_linear_symmetries]]

136.206

11215

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

clairaut

[[_1st_order, _with_linear_symmetries], _rational, _Clairaut]

0.709

11216

\[ {}4 \,{\mathrm e}^{2 y} {y^{\prime }}^{2}+2 x y^{\prime }-1 = 0 \]

unknown

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

N/A

4.438

11217

\[ {}4 \,{\mathrm e}^{2 y} {y^{\prime }}^{2}+2 \,{\mathrm e}^{2 x} y^{\prime }-{\mathrm e}^{2 x} = 0 \]

dAlembert

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

1.338

11218

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

unknown

[‘y=_G(x,y’)‘]

N/A

204.26

11219

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

first_order_ode_lie_symmetry_calculated

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

10.509

11220

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

dAlembert

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

3.897

11221

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

first_order_ode_lie_symmetry_calculated

[[_1st_order, _with_linear_symmetries]]

133.768

11222

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

dAlembert

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

0.736

11223

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

unknown

[‘y=_G(x,y’)‘]

N/A

5.846

11224

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

quadrature

[_quadrature]

1.152

11225

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

clairaut

[[_1st_order, _with_linear_symmetries], _Clairaut]

0.422

11226

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

first_order_ode_lie_symmetry_calculated

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

6.652

11227

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

dAlembert

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

0.42

11228

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

dAlembert, first_order_nonlinear_p_but_separable

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

1.473

11229

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

first_order_ode_lie_symmetry_calculated

[_rational]

72.443

11230

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

separable

[_separable]

6.134

11231

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

clairaut

[[_1st_order, _with_linear_symmetries], _rational, _Clairaut]

0.564

11232

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

separable

[_separable]

0.957

11233

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

first_order_ode_lie_symmetry_calculated

[[_1st_order, _with_linear_symmetries]]

8.293

11234

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

unknown

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

N/A

3.427

11235

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

clairaut

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

0.363

11236

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

dAlembert

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

0.373

11237

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

clairaut

[[_homogeneous, ‘class G‘], _Clairaut]

0.776

11238

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

quadrature

[_quadrature]

0.37

11239

\[ {}8 \left (1+y^{\prime }\right )^{3} = 27 \left (x +y\right ) \left (1-y^{\prime }\right )^{3} \]

dAlembert

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

473.104

11240

\[ {}4 {y^{\prime }}^{2} = 9 x \]

quadrature

[_quadrature]

0.282

11241

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

quadrature

[_quadrature]

0.886

11242

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.229

11243

\[ {}y^{\prime \prime }-6 y^{\prime }+25 y = 0 \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.593

11244

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.228

11245

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.223

11246

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.281

11247

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.253

11248

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

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.119

11249

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.272

11250

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

higher_order_linear_constant_coefficients_ODE

[[_high_order, _missing_x]]

0.122

11251

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.531

11252

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

0.562

11253

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.498

11254

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _linear, _nonhomogeneous]]

0.234

11255

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

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.519

11256

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.42

11257

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _with_linear_symmetries]]

0.583

11258

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.739

11259

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _with_linear_symmetries]]

0.612

11260

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.461

11261

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.758

11262

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.291

11263

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

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

2.616

11264

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.648

11265

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

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.894

11266

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _with_linear_symmetries]]

1.954

11267

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

0.908

11268

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

higher_order_linear_constant_coefficients_ODE

[[_high_order, _with_linear_symmetries]]

0.211

11269

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

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]]

1.929

11270

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

higher_order_linear_constant_coefficients_ODE

[[_high_order, _linear, _nonhomogeneous]]

1.004

11271

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

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _with_linear_symmetries]]

0.353

11272

\[ {}x^{3} y^{\prime \prime \prime }+2 x^{2} y^{\prime \prime }+2 y = 10 x +\frac {10}{x} \]

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _exact, _linear, _nonhomogeneous]]

0.912

11273

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

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]]

3.465

11274

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

kovacic, second_order_change_of_variable_on_x_method_1

[[_2nd_order, _with_linear_symmetries]]

6.039

11275

\[ {}y^{\prime \prime }-5 y^{\prime }+6 y = \cos \left (x \right )-{\mathrm e}^{2 x} \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.721

11276

\[ {}y^{\prime \prime \prime \prime }-y = {\mathrm e}^{x} \cos \left (x \right ) \]

higher_order_linear_constant_coefficients_ODE

[[_high_order, _linear, _nonhomogeneous]]

2.065

11277

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

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.601

11278

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

0.587

11279

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

higher_order_linear_constant_coefficients_ODE

[[_high_order, _linear, _nonhomogeneous]]

0.226

11280

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

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_high_order, _linear, _nonhomogeneous]]

1.239

11281

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

0.198

11282

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.099

11283

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.996

11284

\[ {}y^{\prime \prime \prime \prime }-y^{\prime \prime \prime }-3 y^{\prime \prime }+5 y^{\prime }-2 y = {\mathrm e}^{3 x} \]

higher_order_linear_constant_coefficients_ODE

[[_high_order, _with_linear_symmetries]]

0.212

11285

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.797

11286

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

higher_order_ODE_non_constant_coefficients_of_type_Euler

[[_3rd_order, _exact, _linear, _nonhomogeneous]]

0.335

11287

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _linear, _nonhomogeneous]]

8.678

11288

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

kovacic, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

3.58

11289

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

kovacic

[[_2nd_order, _with_linear_symmetries]]

0.702

11290

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

kovacic, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _with_linear_symmetries]]

1.725

11291

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

kovacic, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _with_linear_symmetries]]

1.987

11292

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

kovacic, second_order_change_of_variable_on_y_method_1, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _linear, _nonhomogeneous]]

4.663

11293

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

kovacic, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _with_linear_symmetries]]

0.949

11294

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

unknown

[[_2nd_order, _with_linear_symmetries]]

N/A

1.31

11295

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

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _linear, _nonhomogeneous]]

1.154

11296

\[ {}y^{\prime \prime }+\left (2 \,{\mathrm e}^{x}-1\right ) y^{\prime }+{\mathrm e}^{2 x} y = {\mathrm e}^{4 x} \]

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

[[_2nd_order, _linear, _nonhomogeneous]]

7.931

11297

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

kovacic, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

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

1.29

11298

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

second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _with_linear_symmetries]]

7.284

11299

\[ {}x^{6} y^{\prime \prime }+3 x^{5} y^{\prime }+y = \frac {1}{x^{2}} \]

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _linear, _nonhomogeneous]]

2.721

11300

\[ {}x y^{\prime \prime }-\left (2 x^{2}+1\right ) y^{\prime }-8 x^{3} y = 4 x^{3} {\mathrm e}^{-x^{2}} \]

kovacic, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _linear, _nonhomogeneous]]

1.59