Table 2 represents the values of the numerical solutions using fourth-order Runge–Kutta method in the interval t \(\in\) [0, 300]

1.8812E−15

1

0

0

1.5247E−15

0.809035

− 1.09756E−15

− 0.587738

5.9028E−16

0.309102

− 1.77911E−15

− 0.951001

− 5.6779E−16

− 0.308864

− 1.78633E−15

− 0.951064

− 1.5106E−15

− 0.808859

− 1.11651E−15

− 0.587913

− 1.8809E−15

− 0.999934

− 2.35325E−17

− 0.000245929

− 1.5383E−15

− 0.809126

1.07833E−15

0.5875

− 6.1263E−16

− 0.309316

1.77147E−15

0.950862

5.4519E−16

0.30861

1.79318E−15

0.951078

1.4963E−15

0.808661

1.13524E−15

0.588073

1.8803E−15

0.999868

4.70583E−17

0.000491738

1.5517E−15

0.809217

− 1.05894E−15

− 0.587262

6.3487E−16

0.309529

− 1.76355E−15

− 0.950724

− 5.225E−16

− 0.308356

− 1.79974E−15

− 0.951091

− 1.4818E−15

− 0.808463

− 1.1538E−15

− 0.588234

− 1.8795E−15

− 0.999802

− 7.05736E−17

− 0.000737578

− 1.5648E−15

− 0.809309

1.03937E−15

0.587025

− 6.5702E−16

− 0.309743

1.75536E−15

0.950585

4.9974E−16

0.308102

1.80602E−15

0.951104

1.4671E−15

0.808265

1.17217E−15

0.588394

1.8783E−15

0.999736

9.40748E−17

0.000983447

1.5777E−15

0.809399

− 1.01965E−15

− 0.586787

6.7906E−16

0.309956

− 1.74689E−15

− 0.950446

− 4.7689E−16

− 0.307848

− 1.81201E−15

− 0.951117

− 1.4521E−15

− 0.808067

− 1.19036E−15

− 0.588553

− 1.8769E−15

− 0.99967

− 1.17558E−16

− 0.00122914

− 1.5903E−15

− 0.80949

9.99769E−16

0.586549

− 7.0098E−16

− 0.310169

1.73814E−15

0.950307

4.5398E−16

0.307593

1.81772E−15

0.95113

1.4369E−15

0.807869

1.20835E−15

0.588713

1.8751E−15

0.999603

1.41019E−16

0.00147495