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Eurotherm Conference No. 95: Computational Thermal Radiation in Participating Media IV

IOP Publishing

Journal of Physics: Conference Series 369 (2012) 012021

doi:10.1088/1742-6596/369/1/012021

calculations of the angular distribution of polarization transmitted by slab, and figure 4 provides a comparison of the reflected radiation.

Figure 3. Polarization of the transmitted radiation. Figure 4. Polarization of the reflected radiation.

For the best fit, we used the parameters: N = 71, K = 171, M = 20 in the code MVDOM and 30 streams in the code Pstar. The comparison of results showed the perfect coincidence at the computer accuracy level, but the computation time was 11 seconds for MVDOM and for the program Pstar more than 180 seconds.

7. Conclusions

The discretized VRTE for a slab has a unique analytic solution in the matrix form. The high level of optimization of linear algebra packages permits a single algorithm implementation on a computer for this solution. Various implementations differ in the method of the solution anisotropic part elimination. Taking into account our algorithm analysis, the analytical anisotropy elimination on the basis of MSH is supposedly a more precise algorithm than TMS. At the algorithm implementation it is necessary to use the algorithm of sparse matrices, and when using the Intel processor the application of MKL library is very essential.

References

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