Theory and Modern Applications
From: A mass-conservative higher-order ADI method for solving unsteady convection–diffusion equations
τ | ∥⋅∥ | Rate | \(\|\cdot \|_{\infty }\) | Rate | |
---|---|---|---|---|---|
DHOC-ADI | 0.1 | 2.13489 × 10−2 | – | 8.43103 × 10−2 | – |
0.05 | 2.67308 × 10−3 | 2.99758 | 1.15578 × 10−2 | 2.86684 | |
0.025 | 6.60480 × 10−4 | 2.01692 | 2.76702 × 10−3 | 2.06247 | |
0.0125 | 1.64559 × 10−4 | 2.00491 | 6.84316 × 10−4 | 2.01560 |
τ | ∥⋅∥ | Rate | \(\|\cdot \|_{\infty }\) | Rate | |
---|---|---|---|---|---|
HOC-ADI | 0.1 | 2.13481 × 10−2 | – | 8.43028 × 10−2 | – |
0.05 | 2.67269 × 10−3 | 2.99774 | 1.15540 × 10−2 | 2.86718 | |
0.025 | 6.60210 × 10−4 | 2.01730 | 2.76494 × 10−3 | 2.06308 | |
0.0125 | 1.64320 × 10−4 | 2.00642 | 6.81863 × 10−4 | 2.01969 |