2.16.115 Problems 11401 to 11500

Table 2.246: Main lookup table. Sorted sequentially by problem number.

#

ODE

Program classification

CAS classification

Solved?

Verified?

time (sec)

11401

\[ {}7 t^{2} x^{\prime } = 3 x-2 t \]

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

0.96

11402

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

unknown

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

N/A

0.551

11403

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

unknown

[‘y=_G(x,y’)‘]

N/A

1.834

11404

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

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

0.79

11405

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

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.692

11406

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

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

0.746

11407

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

exact, linear, differentialType, first_order_ode_lie_symmetry_lookup

[_linear]

0.892

11408

\[ {}\theta ^{\prime } = -a \theta +{\mathrm e}^{b t} \]

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.01

11409

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

exact, linear, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.603

11410

\[ {}x^{\prime }+\frac {5 x}{t} = t +1 \]

i.c.

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.069

11411

\[ {}x^{\prime } = \left (a +\frac {b}{t}\right ) x \]

i.c.

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.794

11412

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

i.c.

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.167

11413

\[ {}N^{\prime } = N-9 \,{\mathrm e}^{-t} \]

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

0.785

11414

\[ {}\cos \left (\theta \right ) v^{\prime }+v = 3 \]

exact, linear, separable, first_order_ode_lie_symmetry_lookup

[_separable]

2.734

11415

\[ {}R^{\prime } = \frac {R}{t}+t \,{\mathrm e}^{-t} \]

i.c.

linear, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.165

11416

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

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[[_linear, ‘class A‘]]

1.173

11417

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

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

0.963

11418

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

i.c.

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

2.41

11419

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

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]]

1.671

11420

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

riccati, homogeneousTypeC, first_order_ode_lie_symmetry_lookup

[[_homogeneous, ‘class C‘], _Riccati]

0.888

11421

\[ {}x^{\prime } = a x+b \]

quadrature

[_quadrature]

0.44

11422

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

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.148

11423

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

bernoulli, homogeneousTypeD2, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

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

1.877

11424

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

riccati, bernoulli, first_order_ode_lie_symmetry_lookup

[[_1st_order, _with_linear_symmetries], _Bernoulli]

0.825

11425

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

exact, bernoulli, separable, first_order_ode_lie_symmetry_lookup

[_separable]

3.64

11426

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

riccati, bernoulli, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

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

1.054

11427

\[ {}x^{\prime } = a x+b x^{3} \]

quadrature

[_quadrature]

2.036

11428

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

bernoulli, first_order_ode_lie_symmetry_lookup

[_Bernoulli]

1.114

11429

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

exact, linear, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

1.018

11430

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

exact

[_exact]

1.697

11431

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

exact

[NONE]

6.304

11432

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

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

1.022

11433

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

exact, riccati, separable, homogeneousTypeD2, first_order_ode_lie_symmetry_lookup

[_separable]

0.919

11434

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

exact, separable, first_order_ode_lie_symmetry_lookup

[_separable]

3.178

11435

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

i.c.

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.587

11436

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

i.c.

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]]

1.146

11437

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

i.c.

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.597

11438

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

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.479

11439

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

i.c.

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.548

11440

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

i.c.

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]]

1.262

11441

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

i.c.

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.575

11442

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

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.453

11443

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

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.185

11444

\[ {}x^{\prime \prime }-4 x^{\prime }+6 x = 0 \]

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.036

11445

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

2.809

11446

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

4.975

11447

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

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.132

11448

\[ {}\frac {x^{\prime \prime }}{2}+\frac {5 x^{\prime }}{6}+\frac {2 x}{9} = 0 \]

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.487

11449

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

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.422

11450

\[ {}x^{\prime \prime }+\frac {x^{\prime }}{8}+x = 0 \]

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

1.143

11451

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.739

11452

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.902

11453

\[ {}x^{\prime \prime }+x^{\prime }+x = 12 \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.627

11454

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.733

11455

\[ {}x^{\prime \prime }+x^{\prime }+x = 5 \sin \left (7 t \right ) \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.403

11456

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.605

11457

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.656

11458

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.636

11459

\[ {}x^{\prime \prime }+x^{\prime }+x = 4 t +5 \,{\mathrm e}^{-t} \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.781

11460

\[ {}x^{\prime \prime }+x^{\prime }+x = 5 \sin \left (2 t \right )+t \,{\mathrm e}^{t} \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.425

11461

\[ {}x^{\prime \prime }+x^{\prime }+x = t^{3}+1-4 t \cos \left (t \right ) \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.012

11462

\[ {}x^{\prime \prime }+x^{\prime }+x = -6+2 \,{\mathrm e}^{2 t} \sin \left (t \right ) \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.516

11463

\[ {}x^{\prime \prime }+7 x = t \,{\mathrm e}^{3 t} \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.832

11464

\[ {}x^{\prime \prime }-x^{\prime } = 6+{\mathrm e}^{2 t} \]

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]]

1.875

11465

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.579

11466

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.452

11467

\[ {}x^{\prime \prime }+x = 9 \,{\mathrm e}^{-t} \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.61

11468

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.682

11469

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.833

11470

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

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.822

11471

\[ {}x^{\prime \prime }-3 x^{\prime }-40 x = 2 \,{\mathrm e}^{-t} \]

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.705

11472

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

i.c.

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]]

1.99

11473

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

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.481

11474

\[ {}x^{\prime \prime }+\frac {x^{\prime }}{100}+4 x = \cos \left (2 t \right ) \]

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.072

11475

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

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.326

11476

\[ {}x^{\prime \prime }+3025 x = \cos \left (45 t \right ) \]

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.223

11477

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

kovacic, second_order_euler_ode

[[_Emden, _Fowler]]

0.654

11478

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

kovacic, second_order_euler_ode

[[_Emden, _Fowler]]

0.582

11479

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

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]]

2.817

11480

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

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

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

3.08

11481

\[ {}t^{2} x^{\prime \prime }-7 t x^{\prime }+16 x = 0 \]

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]]

1.664

11482

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

i.c.

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)]‘]]

1.609

11483

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

i.c.

kovacic, second_order_euler_ode, second_order_ode_missing_y

[[_2nd_order, _missing_y]]

1.187

11484

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

i.c.

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]]

2.863

11485

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

i.c.

kovacic, second_order_ode_missing_y

[[_2nd_order, _missing_y]]

4.904

11486

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.783

11487

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.494

11488

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.47

11489

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

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is

[[_2nd_order, _exact, _linear, _nonhomogeneous]]

1.755

11490

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.758

11491

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

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.562

11492

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

kovacic, second_order_ode_missing_y, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _missing_y]]

1.708

11493

\[ {}t^{2} x^{\prime \prime }-3 t x^{\prime }+3 x = 4 t^{7} \]

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, _with_linear_symmetries]]

2.57

11494

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.55

11495

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

reduction_of_order

[[_2nd_order, _exact, _linear, _homogeneous]]

0.423

11496

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

reduction_of_order

[_Hermite]

0.525

11497

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

reduction_of_order

[[_2nd_order, _missing_x]]

0.214

11498

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

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.581

11499

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

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.727

11500

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_x]]

0.286