Page 60 - IJOCTA-15-4
P. 60

MN. Khan et.al. / IJOCTA, Vol.15, No.4, pp.594-609 (2025)


                                    8
                                            Approximate
                                    7       Exact


                                    6


                                    5 s


                                    4

                                    3


                                    2
                                     0        0.2       0.4      0.6      0.8        1
                                                             x
                                        −4
                                     x 10







                                   2

                                 L ∞



                                   1






                                   0
                                    0       50      100     150      200     250     300
                                                             M


            Figure 1. Comparison of exact and approximate and the L ∞ error norm with respect to M using Haar
            wavelets for Test Problem 1


            time step size dt decreases. Table 2 presents a       Figure 3 illustrates the connection between ϑ
            comparison of the numerical results obtained us-  and the method’s accuracy as measured by the
            ing the proposed method with those from other     L ∞ norm. The data reveal that as ϑ rises from
            numerical methods. The results indicate that the  −50 to −10, the error decreases, signifying an im-
            proposed method achieves improved accuracy.       provement in the numerical solution’s precision.


            Table 3. A comparison of Haar wavelets with the results in 40  at ϑ = 1, γ = 1, T = 1 for Test Problem 2

                          dt      HWM        Implicit  Galerkin  Keller-Box    RKC      Saulyev I
                        0.0500 1.49e − 03 9.1e − 03 9.9e − 02     9.4e − 02  9.8e − 02 9.6e − 03
                        0.0250 7.46e − 04 2.3e − 03 3.0e − 02     2.4e − 02  3.7e − 02 2.5e − 03
                        0.0100 2.98e − 04 3.8e − 04 4.9e − 03     4.1e − 03  6.1e − 03 3.9e − 04
                        0.0050 1.49e − 04 9.4e − 05 1.2e − 03     1.0e − 03  1.5e − 03 9.6e − 05
                        0.0025 7.46e − 05 2.3e − 05 3.1e − 04     2.5e − 04  3.5e − 04 2.5e − 05
                        0.0010 2.98e − 05 4.1e − 05 5.0e − 05     4.0e − 05  6.0e − 05 4.3e − 06
                                                           602
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