Theory and Modern Applications
r | Exact solution | HBT method [46] | Block-pulse method [45] | Presented method | Absolute error |
---|---|---|---|---|---|
\(\underline{u} ( x,r )\) | |||||
0 | 0.000000000 | 0.000000000 | 0.007956 | 0.000000000 | 8.58708660e−11 |
0.1 | 0.050000000 | 0.050000000 | 0.056347 | 0.050000000 | 6.79634155e−11 |
0.2 | 0.100000000 | 0.100000000 | 0.104737 | 0.100000000 | 5.21343024e−11 |
0.3 | 0.150000000 | 0.150000000 | 0.153128 | 0.150000000 | 3.83835130e−11 |
0.4 | 0.200000000 | 0.200000000 | 0.201519 | 0.200000000 | 2.67110889e−11 |
0.5 | 0.250000000 | 0.250000000 | 0.266040 | 0.250000000 | 1.53477231e−12 |
0.6 | 0.300000000 | 0.300000000 | 0.314430 | 0.300000000 | 8.80506779e−13 |
0.7 | 0.350000000 | 0.350000000 | 0.362820 | 0.350000000 | 4.41124914e−13 |
0.8 | 0.400000000 | 0.400000000 | 0.411210 | 0.400000000 | 2.16571205e−13 |
0.9 | 0.45000000 | 0.450000000 | 0.359603 | 0.450000000 | 1.03909548e−11 |
u̅(x,r) | |||||
0 | 1.000000000 | 1.000000000 | 1.024160 | 1.000000000 | 1.00612851e−11 |
0.1 | 0.950000000 | 0.950000000 | 0.975770 | 0.950000000 | 9.72248948e−12 |
0.2 | 0.900000000 | 0.900000000 | 0.927379 | 0.900000000 | 7.29647454e−12 |
0.3 | 0.850000000 | 0.850000000 | 0.878988 | 0.850000000 | 2.78301826e−12 |
0.4 | 0.800000000 | 0.800000000 | 0.830598 | 0.800000000 | 3.81765730e−12 |
0.5 | 0.750000000 | 0.750000000 | 0.766077 | 0.750000000 | 0.00000000e+00 |
0.6 | 0.700000000 | 0.700000000 | 0.717986 | 0.700000000 | 3.09223758e−12 |
0.7 | 0.650000000 | 0.650000000 | 0.669290 | 0.650000000 | 6.18458618e−12 |
0.8 | 0.600000000 | 0.600000000 | 0.630905 | 0.600000000 | 9.27682375e−12 |
0.9 | 0.550000000 | 0.550000000 | 0.572514 | 0.550000000 | 4.72755612e−11 |