2.16.75 Problems 7401 to 7500

Table 2.166: Main lookup table. Sorted sequentially by problem number.

#

ODE

Program classification

CAS classification

Solved?

Verified?

time (sec)

7401

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

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]]

1.35

7402

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

second_order_ode_missing_x, second_order_ode_missing_y

[[_2nd_order, _missing_x]]

7.969

7403

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

second_order_ode_missing_x, second_order_ode_missing_y

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

0.861

7404

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

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]]

1.96

7405

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

second_order_ode_missing_x, second_order_ode_missing_y

[[_2nd_order, _missing_x]]

10.206

7406

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

second_order_ode_missing_x, second_order_ode_missing_y

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

3.548

7407

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

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]]

2.497

7408

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

second_order_ode_missing_y

[[_2nd_order, _missing_y]]

0.847

7409

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

second_order_ode_missing_y

[[_2nd_order, _missing_y], [_2nd_order, _reducible, _mu_xy]]

2.054

7410

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.508

7411

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

unknown

[[_2nd_order, _missing_x]]

N/A

0.286

7412

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

2.526

7413

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _missing_x]]

0.868

7414

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.882

7415

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

1.089

7416

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

1.2

7417

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.204

7418

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.121

7419

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

1.461

7420

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

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]]

1.809

7421

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

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]]

2.117

7422

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

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]]

2.456

7423

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

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]]

2.502

7424

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

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]]

2.882

7425

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

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]]

3.535

7426

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

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]]

3.253

7427

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

kovacic, second_order_linear_constant_coeff, second_order_ode_can_be_made_integrable

[[_2nd_order, _missing_x]]

1.953

7428

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.684

7429

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.777

7430

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _with_linear_symmetries]]

0.701

7431

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.808

7432

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.698

7433

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

kovacic, second_order_linear_constant_coeff

[[_2nd_order, _linear, _nonhomogeneous]]

0.876

7434

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

66.283

7435

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

13.249

7436

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

second_order_ode_missing_x

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

6.76

7437

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

51.904

7438

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

second_order_ode_missing_x

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

4.56

7439

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

second_order_ode_missing_x

[[_2nd_order, _missing_x], [_2nd_order, _reducible, _mu_x_y1], [_2nd_order, _reducible, _mu_y_y1]]

1.328

7440

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

9.137

7441

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

second_order_ode_missing_x

[[_2nd_order, _missing_x]]

14.752

7442

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

second_order_nonlinear_solved_by_mainardi_lioville_method

[_Liouville, [_2nd_order, _reducible, _mu_xy]]

0.515

7443

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

second_order_nonlinear_solved_by_mainardi_lioville_method

[_Liouville, [_2nd_order, _reducible, _mu_xy]]

0.707

7444

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

unknown

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

N/A

0.104

7445

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

unknown

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

N/A

0.483

7446

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

second_order_ode_missing_x

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

3.796

7447

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

second_order_ode_missing_x

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

4.171

7448

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

homogeneousTypeC, first_order_ode_lie_symmetry_lookup

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

3.04

7449

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

unknown

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

N/A

0.112

7450

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

second_order_nonlinear_solved_by_mainardi_lioville_method

[_Liouville, [_2nd_order, _reducible, _mu_xy]]

0.357

7451

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

second_order_ode_missing_y, second_order_nonlinear_solved_by_mainardi_lioville_method

[[_2nd_order, _missing_y], _Liouville, [_2nd_order, _reducible, _mu_xy]]

3.006

7452

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

second_order_nonlinear_solved_by_mainardi_lioville_method

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

2.058

7453

\[ {}10 y^{\prime \prime }+x^{2} y^{\prime }+\frac {3 {y^{\prime }}^{2}}{y} = 0 \]

second_order_nonlinear_solved_by_mainardi_lioville_method

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

2.379

7454

\[ {}10 y^{\prime \prime }+\left ({\mathrm e}^{x}+3 x \right ) y^{\prime }+\frac {3 \,{\mathrm e}^{y} {y^{\prime }}^{2}}{\sin \left (y\right )} = 0 \]

unknown

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

N/A

0.521

7455

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

kovacic, second_order_euler_ode, exact linear second order ode, second_order_integrable_as_is

[[_2nd_order, _linear, _nonhomogeneous]]

4.401

7456

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

kovacic

[[_2nd_order, _linear, _nonhomogeneous]]

1.743

7457

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

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)]‘]]

2.368

7458

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

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)]‘]]

3.397

7459

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

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]]

2.776

7460

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

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]]

4.483

7461

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

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)]‘]]

2.283

7462

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

unknown

[[_2nd_order, _linear, _nonhomogeneous]]

N/A

2.789

7463

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

second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _with_linear_symmetries]]

12.477

7464

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

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]]

7.69

7465

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

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]]

2.961

7466

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

second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _linear, _nonhomogeneous]]

3.692

7467

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

second_order_change_of_variable_on_x_method_1, second_order_change_of_variable_on_x_method_2

[[_2nd_order, _linear, _nonhomogeneous]]

6.803

7468

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

kovacic, second_order_change_of_variable_on_y_method_2

[[_2nd_order, _with_linear_symmetries]]

7.704

7469

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

kovacic

[[_2nd_order, _with_linear_symmetries]]

0.753

7470

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

kovacic, second_order_change_of_variable_on_y_method_1

[_Lienard]

1.487

7471

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

kovacic, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _linear, _nonhomogeneous]]

2.708

7472

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

kovacic, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _linear, _nonhomogeneous]]

3.88

7473

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

kovacic, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _linear, _nonhomogeneous]]

1.444

7474

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

kovacic, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _linear, _nonhomogeneous]]

8.422

7475

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

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _with_linear_symmetries]]

1.449

7476

\[ {}4 x^{2} y^{\prime \prime }+4 x^{5} y^{\prime }+\left (x^{8}+6 x^{4}+4\right ) y = 0 \]

kovacic

[[_2nd_order, _with_linear_symmetries]]

1.969

7477

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

unknown

[[_2nd_order, _with_linear_symmetries]]

N/A

0.097

7478

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

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[[_2nd_order, _with_linear_symmetries]]

1.171

7479

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

kovacic, second_order_bessel_ode, second_order_change_of_variable_on_y_method_1

[_Lienard]

1.082

7480

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

linear, exactWithIntegrationFactor, first_order_ode_lie_symmetry_lookup

[_linear]

1.737

7481

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

exactWithIntegrationFactor

[_rational]

2.504

7482

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

riccati

[[_Riccati, _special]]

1.388

7483

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

higher_order_linear_constant_coefficients_ODE

[[_high_order, _linear, _nonhomogeneous]]

0.503

7484

\[ {}x^{2} y^{\prime \prime }-x \left (6+x \right ) y^{\prime }+10 y = 0 \]

second order series method. Regular singular point. Difference is integer

[[_2nd_order, _with_linear_symmetries]]

4.208

7485

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

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

[_Bessel]

2.123

7486

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

second_order_bessel_ode

[_Bessel]

1.115

7487

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

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_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)]‘]]

2.481

7488

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

unknown

[[_3rd_order, _with_linear_symmetries]]

N/A

0.19

7489

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

i.c.

quadrature

[_quadrature]

0.567

7490

\[ {}\left [\begin {array}{c} x^{\prime }=3 x+y \\ y^{\prime }=-x+y \end {array}\right ] \]

system of linear ODEs

system of linear ODEs

0.668

7491

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

kovacic

[_Gegenbauer]

1.222

7492

\[ {}\left (x^{2}-1\right ) y^{\prime \prime }-6 x y^{\prime }+12 y = 0 \]

kovacic

[_Gegenbauer]

1.273

7493

\[ {}\left (x^{2}+3\right ) y^{\prime \prime }-7 x y^{\prime }+16 y = 0 \]

kovacic

[[_2nd_order, _with_linear_symmetries]]

1.48

7494

\[ {}\left (x^{2}-1\right ) y^{\prime \prime }+8 x y^{\prime }+12 y = 0 \]

kovacic

[_Gegenbauer]

1.233

7495

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

kovacic

[[_2nd_order, _with_linear_symmetries]]

0.226

7496

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

kovacic

[[_2nd_order, _with_linear_symmetries]]

1.582

7497

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

kovacic

[[_2nd_order, _with_linear_symmetries]]

1.26

7498

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

kovacic

[[_2nd_order, _with_linear_symmetries]]

0.989

7499

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

kovacic

[[_2nd_order, _with_linear_symmetries]]

1.579

7500

\[ {}\left (x^{2}-6 x +10\right ) y^{\prime \prime }-4 \left (x -3\right ) y^{\prime }+6 y = 0 \]

kovacic

[[_2nd_order, _with_linear_symmetries]]

1.768