Theory and Modern Applications
From: A mass-conservative higher-order ADI method for solving unsteady convection–diffusion equations
h | τ | 0.1 | 0.2 | 0.3 | 0.4 | 0.5 | 0.6 | 0.7 | 0.8 | 0.9 | |
---|---|---|---|---|---|---|---|---|---|---|---|
DHOC-ADI | 0.01 | 0.001 | 4.54 | 4.81 | 5.07 | 5.33 | 5.57 | 5.80 | 6.01 | 6.19 | 6.33 |
0.1 | 0.0001 | 0.75 | 0.83 | 0.90 | 0.97 | 0.10 | 0.11 | 0.11 | 0.12 | 0.12 | |
HOC-ADI [14] | 0.01 | 0.001 | 4.59 | 4.86 | 5.13 | 5.38 | 5.62 | 5.84 | 6.04 | 6.21 | 6.35 |
0.1 | 0.0001 | 273 | 262 | 248 | 229 | 206 | 177 | 143 | 104 | 58.8 | |
EHOC-ADI [16] | 0.01 | 0.001 | 4.60 | 4.87 | 5.13 | 5.38 | 5.62 | 5.84 | 6.04 | 6.21 | 6.35 |
0.1 | 0.0001 | 316 | 302 | 283 | 259 | 229 | 192 | 150 | 100 | 44.6 | |
RHOC-ADI [17] | 0.01 | 0.001 | 4.62 | 4.88 | 5.14 | 5.40 | 5.63 | 5.85 | 6.04 | 6.21 | 6.34 |
0.1 | 0.0001 | 571 | 535 | 488 | 430 | 361 | 280 | 187 | 81.3 | 37.3 | |
Nazir [30] | 0.01 | 0.001 | 0.88 | 1.45 | 1.68 | 1.54 | 1.02 | 1.98 | 7.68 | 1.54 | 1.56 |
Dehghan [31] | 0.01 | 0.001 | 0.91 | 1.54 | 1.84 | 1.77 | 1.33 | 0.56 | 0.38 | 1.18 | 1.31 |
Mohammadi [32] | 0.01 | 0.001 | 1.73 | 1.02 | 0.39 | 1.96 | 3.59 | 5.25 | 6.94 | 8.57 | 9.13 |