2.16.155 Problems 15401 to 15500

Table 2.326: Main lookup table. Sorted sequentially by problem number.

#

ODE

Program classification

CAS classification

Solved?

Verified?

time (sec)

15401

\[ {}x^{2} y^{\prime \prime }+4 x y^{\prime }+2 y = 2 \ln \left (x \right )^{2}+12 x \]

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]]

3.657

15402

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

kovacic, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _linear, _nonhomogeneous]]

4.355

15403

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

kovacic, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _with_linear_symmetries]]

0.848

15404

\[ {}\left (2 x +1\right ) y^{\prime \prime }+\left (-2+4 x \right ) y^{\prime }-8 y = 0 \]

kovacic

[[_2nd_order, _with_linear_symmetries]]

0.714

15405

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

kovacic, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[_Jacobi]

1.088

15406

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

kovacic, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _with_linear_symmetries]]

1.181

15407

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

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.287

15408

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

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.844

15409

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

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.562

15410

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

reduction_of_order

[[_2nd_order, _exact, _linear, _nonhomogeneous]]

0.324

15411

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

reduction_of_order

[[_2nd_order, _exact, _linear, _nonhomogeneous]]

0.283

15412

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

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.352

15413

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

reduction_of_order

[[_2nd_order, _linear, _nonhomogeneous]]

0.536

15414

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

reduction_of_order

[[_2nd_order, _linear, _nonhomogeneous]]

0.374

15415

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

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.623

15416

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

reduction_of_order

[[_2nd_order, _with_linear_symmetries]]

0.359

15417

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.5

15418

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

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]]

1.326

15419

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.586

15420

\[ {}y^{\prime \prime }+y = \frac {1}{\sqrt {\sin \left (x \right )^{5} \cos \left (x \right )}} \]

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

2.762

15421

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

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

0.472

15422

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.582

15423

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.625

15424

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

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]]

3.529

15425

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

higher_order_linear_constant_coefficients_ODE

[[_3rd_order, _missing_y]]

0.315

15426

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

kovacic, second_order_ode_missing_y

[[_2nd_order, _missing_y]]

1.488

15427

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

kovacic, second_order_ode_missing_y, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _missing_y]]

1.468

15428

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

second_order_ode_missing_y, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _missing_y]]

0.908

15429

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

kovacic, second_order_ode_missing_y

[[_2nd_order, _missing_y]]

0.764

15430

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

second_order_ode_missing_y

[[_2nd_order, _missing_y]]

0.911

15431

\[ {}4 x y^{\prime \prime }+2 y^{\prime }+y = 1 \]

i.c.

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, _with_linear_symmetries]]

N/A

2.32

15432

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

i.c.

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]]

N/A

2.353

15433

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

i.c.

kovacic, exact linear second order ode, second_order_integrable_as_is, second_order_ode_missing_y

[[_2nd_order, _missing_y]]

2.061

15434

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

i.c.

kovacic, second_order_change_of_variable_on_y_method_2, second_order_ode_non_constant_coeff_transformation_on_B

[[_2nd_order, _with_linear_symmetries]]

N/A

1.839

15435

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

i.c.

second_order_change_of_variable_on_y_method_2

[[_2nd_order, _linear, _nonhomogeneous]]

N/A

0.892

15436

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

i.c.

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _linear, _nonhomogeneous]]

N/A

8.398

15437

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

i.c.

second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

N/A

0.788

15438

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

i.c.

kovacic, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

N/A

1.733

15439

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.384

15440

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.363

15441

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

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _missing_x]]

0.253

15442

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

1.035

15443

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

N/A

0.378

15444

\[ {}x^{\prime \prime }-x \,{\mathrm e}^{x^{\prime }} = 0 \]

second_order_ode_missing_x

[[_2nd_order, _missing_x], [_2nd_order, _reducible, _mu_x_y1]]

0.585

15445

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

N/A

0.542

15446

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

second_order_ode_missing_x

[[_2nd_order, _missing_x], _Liouville, [_2nd_order, _reducible, _mu_x_y1], [_2nd_order, _reducible, _mu_xy]]

0.524

15447

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

second_order_integrable_as_is, second_order_ode_missing_x, exact nonlinear second order ode

[[_2nd_order, _missing_x], [_2nd_order, _exact, _nonlinear], [_2nd_order, _reducible, _mu_x_y1], [_2nd_order, _reducible, _mu_xy]]

0.703

15448

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

N/A

0.385

15449

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

2.363

15450

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

0.679

15451

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

2.101

15452

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

N/A

1.0

15453

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

i.c.

second_order_integrable_as_is, second_order_ode_missing_x, exact nonlinear second order ode

[[_2nd_order, _missing_x], [_2nd_order, _exact, _nonlinear], [_2nd_order, _reducible, _mu_x_y1], [_2nd_order, _reducible, _mu_xy]]

8.125

15454

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

1.275

15455

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

4.601

15456

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

i.c.

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.421

15457

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

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]]

1.14

15458

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

111.799

15459

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

3.641

15460

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

2.908

15461

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

i.c.

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

1.921

15462

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

i.c.

unknown

[[_3rd_order, _missing_x]]

N/A

0.0

15463

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

i.c.

unknown

[[_high_order, _missing_x]]

N/A

0.0

15464

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

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

[[_2nd_order, _missing_y]]

0.819

15465

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

i.c.

higher_order_missing_y

[[_high_order, _missing_y]]

0.757

15466

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

i.c.

higher_order_missing_y

[[_high_order, _missing_y]]

0.667

15467

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

i.c.

first order ode series method. Ordinary point, first order ode series method. Taylor series method

[_linear]

1.467

15468

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

i.c.

first order ode series method. Taylor series method

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

1.197

15469

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

i.c.

first order ode series method. Ordinary point, first order ode series method. Taylor series method

[_separable]

1.372

15470

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

i.c.

second order series method. Ordinary point, second order series method. Taylor series method

[[_Emden, _Fowler]]

1.148

15471

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

i.c.

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _missing_y]]

1.501

15472

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

i.c.

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _linear, _nonhomogeneous]]

4.568

15473

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

i.c.

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

40.846

15474

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

i.c.

unknown

[NONE]

N/A

0.0

15475

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

i.c.

first order ode series method. Ordinary point, first order ode series method. Taylor series method

[_separable]

1.181

15476

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

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _exact, _linear, _homogeneous]]

0.511

15477

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

i.c.

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

1.207

15478

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

i.c.

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

1.238

15479

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

i.c.

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

1.415

15480

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

second order series method. Ordinary point, second order series method. Taylor series method

[[_2nd_order, _with_linear_symmetries]]

0.629

15481

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

i.c.

first order ode series method. Taylor series method

[‘y=_G(x,y’)‘]

1.368

15482

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

second order series method. Regular singular point. Difference not integer

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

0.831

15483

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

first order ode series method. Ordinary point, first order ode series method. Taylor series method

[_separable]

0.543

15484

\[ {}9 x \left (1-x \right ) y^{\prime \prime }-12 y^{\prime }+4 y = 0 \]

second order series method. Regular singular point. Difference not integer

[_Jacobi]

1.122

15485

\[ {}x^{2} y^{\prime \prime }+x y^{\prime }+\left (4 x^{2}-\frac {1}{9}\right ) y = 0 \]

second_order_bessel_ode

[[_2nd_order, _with_linear_symmetries]]

0.582

15486

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

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _with_linear_symmetries]]

0.802

15487

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

second_order_bessel_ode

[[_2nd_order, _with_linear_symmetries]]

0.517

15488

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

second_order_bessel_ode

[[_2nd_order, _with_linear_symmetries]]

0.52

15489

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

second_order_bessel_ode

[[_2nd_order, _with_linear_symmetries]]

1.675

15490

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

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

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

0.894

15491

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

second_order_bessel_ode

[_Lienard]

0.542

15492

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

second_order_bessel_ode

[[_2nd_order, _with_linear_symmetries]]

0.556

15493

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.67

15494

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

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _with_linear_symmetries]]

0.481

15495

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.514

15496

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

kovacic, second_order_linear_constant_coeff, linear_second_order_ode_solved_by_an_integrating_factor

[[_2nd_order, _linear, _nonhomogeneous]]

1.8

15497

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.135

15498

\[ {}\left [\begin {array}{c} x_{1}^{\prime }=-2 t x_{1}^{2} \\ x_{2}^{\prime }=\frac {x_{2}+t}{t} \end {array}\right ] \]

system of linear ODEs

system of linear ODEs

N/A

0.119

15499

\[ {}\left [\begin {array}{c} x_{1}^{\prime }={\mathrm e}^{t -x_{1}} \\ x_{2}^{\prime }=2 \,{\mathrm e}^{x_{1}} \end {array}\right ] \]

system of linear ODEs

system of linear ODEs

N/A

0.246

15500

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

system of linear ODEs

system of linear ODEs

N/A

0.122