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Theory and Modern Applications

Table 1 The errors of numerical solutions and rate of convergence at \(T=20\) using \(h=\tau \)

From: Novel advances in high-order numerical algorithm for evaluation of the shallow water wave equations

 

τ = h

Rate

\(\|\cdot \|_{\infty }\)

Rate

CPU time (s)

Scheme I

0.5

5.4875 × 10−6

2.2094 × 10−6

0.0857

0.25

3.3976 × 10−7

4.0136

1.3672 × 10−7

4.0144

0.3099

0.125

2.1207 × 10−8

4.0019

8.5434 × 10−9

4.0003

1.0363

0.0625

1.3250 × 10−9

4.0004

5.3515 × 10−10

3.9968

8.8850

Scheme II [30]

0.5

1.8618 × 10−2

7.0602 × 10−3

0.0813

0.25

4.7664 × 10−3

1.9657

1.8134 × 10−3

1.9610

0.4885

0.125

1.1996 × 10−3

1.9903

4.5739 × 10−4

1.9872

5.5283

0.0625

3.0053 × 10−4

1.9970

1.1465 × 10−4

1.9962

47.0629

Scheme III [18, 19]

0.5

1.4946 × 10−3

5.2670 × 10−4

0.0591

0.25

1.3373 × 10−4

1.9808

5.1894 × 10−4

1.9777

0.3434

0.125

9.5127 × 10−5

1.9930

3.3644 × 10−5

1.9909

2.4583

0.0625

2.3828 × 10−5

1.9972

8.4277 × 10−6

1.9971

22.0431

  1. Scheme II is exactly the same scheme with those in [18, 19] in the case of RLW equation when the parameter θ in [19] is chosen to be 0.