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Table 1 The errors for numerical solutions \(u^n\) of the scheme (11)–(14) at different time t with various h and \(\tau =h^2\)

From: On the convergence of a high-accuracy compact conservative scheme for the modified regularized long-wave equation

t

\(h=0.2\)

0.1

0.05

0.025

\(e^n_{\epsilon _1}\)

\(e^n_{\epsilon _2}\)

\(e^n_{\epsilon _1}\)

\(e^n_{\epsilon _2}\)

\(e^n_{\epsilon _1}\)

\(e^n_{\epsilon _2}\)

\(e^n_{\epsilon _1}\)

\(e^n_{\epsilon _2}\)

2

3.7504e−3

6.8705e−3

2.3827e−4

4.3361e−4

1.4930e−5

2.7153e−5

9.3409e−7

1.6997e−6

4

7.1325e−3

1.3403e−2

4.5011e−4

8.438e−4

2.8167e−5

5.2812e−5

1.7639e−6

3.3089e−6

6

1.0303e−2

1.9666e−2

6.5000e−4

1.2367e−3

4.0665e−5

7.7372e−5

2.5487e−6

4.8528e−6

8

1.3432e−2

2.5820e−2

8.4767e−4

1.6227e−3

5.3023e−5

1.0151e−4

3.3268e−6

6.3733e−6

10

1.6551e−2

3.1935e−2

1.0447e−3

2.0063e−3

6.5345e−5

1.2549e−4

4.1045e−6

7.8878e−6