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test_cases:seven [2014/12/19 11:39] grenier |
test_cases:seven [2014/12/19 14:25] grenier |
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Advection with constant velocity is here added to conduction and phase change. Analytical solution are proposed from Kurylyk et al. 2014 paper based on a reassessment of solutions by Lunardini. Although not physically realistic (constant velocity) these solutions can be used for benchmarking purposes: "Lack of fidelity to physical processes does not limit ability to serve as benchmark" | Advection with constant velocity is here added to conduction and phase change. Analytical solution are proposed from Kurylyk et al. 2014 paper based on a reassessment of solutions by Lunardini. Although not physically realistic (constant velocity) these solutions can be used for benchmarking purposes: "Lack of fidelity to physical processes does not limit ability to serve as benchmark" | ||
- | The paper Kurylyk et al. 2014 describes at depth the analytical solutions available, the suggested benchmark cases and SUTRA code runs to compare with these solutions. | + | The paper Kurylyk et al. 2014 describes at depth the analytical solutions available, the suggested benchmark cases and SUTRA code runs to compare with these solutions. |
- | One may refer to " | + | A presentation of the TH1 Case by Barret Kurylyk was made during the kick off meeting ({{: |
- | Another source is the presentation | + | The recommanded benchmark Kurylyk et al 2014 Cases 2 and 3 are included in the InterFrost project as two TH1 cases differing |
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+ | **TH1 Test Case** | ||
Initial and boundary conditions: | Initial and boundary conditions: | ||
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- | The analytical solutions of Kurylyk et al 2014 are contained in this {{: | + | The analytical solutions of Kurylyk et al 2014 are accessible here as as xls {{: |
- | The approach used for SUTRA code is summed up in two figures | + | The approach used for SUTRA code is summed up in two figures |
{{ : | {{ : | ||