Solve the Maxwell equation in 2D using a finite domain time difference algorithm. Fields are constant in third direction.
Emilia L.K. Blåsten
2fc52c4130
Fix linker issues
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| .gitignore | 8 лет назад | |
| LICENSE | 9 лет назад | |
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| README.md | 7 лет назад | |
| abctmz.c | 3 лет назад | |
| abctmz.h | 3 лет назад | |
| ezinc.h | 3 лет назад | |
| grid1dez.c | 3 лет назад | |
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| gridtmz.c | 3 лет назад | |
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| incident.c | 3 лет назад | |
| incident.h | 3 лет назад | |
| material.c | 3 лет назад | |
| material.h | 3 лет назад | |
| plot2d.c | 3 лет назад | |
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| ricker.c | 3 лет назад | |
| snapshot2d.c | 3 лет назад | |
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| source.c | 3 лет назад | |
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| tfsftmz.c | 3 лет назад | |
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| tmzdemo2.c | 3 лет назад | |
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README.md
FDTD_2D_Maxwell
Solve the Maxwell equation in 2D using a finite domain time difference algorithm. The fields are assumed to stay constant in the third direction.
Based on a well-known FDTD algorithm. The author learned about that algorithm from John Schneider's book [1]. In addition the SDL (Simple Directmedia Layer) library version 2 is used to display the waves.
The SDL library is licensed under the zlib license. This project is licensed under the GNU Affero General Public License version 3 or any later version, at your choice.
[1] Understanding the Finite-Difference Time-Domain Method, John B. Schneider, www.eecs.wsu.edu/~schneidj/ufdtd, 2010.