Research Article

A Direct Meshless Method for Solving Two-Dimensional Second-Order Hyperbolic Telegraph Equations

Table 1

Numerical results for Example 1.

MethodstRMSE

DMM10.51.33E − 064.13E − 075.15E − 07
DMM20.51.62E − 065.02E − 077.09E − 07
[8]0.51.24E − 053.24E − 06
[19]0.57.82E − 063.11E − 05
[20]0.51.74E − 057.15E − 054.59E − 05
DMM116.64E − 071.27E − 072.12E − 07
DMM219.38E − 061.79E − 062.66E − 06
[8]12.67E − 054.27E − 06
[9]19.97E − 045.98E − 032.27E − 03
[10]13.75E − 062.47E − 054.57E − 06
[19]12.07E − 051.01E − 05
[20]18.15E − 065.45E − 052.51E − 05
DMM124.24E − 066.24E − 079.16E − 07
DMM222.76E − 064.06E − 075.30E − 07
[8]23.20E − 053.94E − 06
[9]21.09E − 038.50E − 032.87E − 03
[10]24.47E − 063.83E − 055.61E − 06
[19]23.01E − 068.25E − 06
[20]29.36E − 068.13E − 052.41E − 05