Contains velocity and gradient data to compute eddy viscosity
Type | Visibility | Attributes | Name | Initial | |||
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type(tem_communication_type), | public | :: | sendBuffer |
Communication buffers to communicate visoscity field Local Fluids required by remote processes |
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type(tem_communication_type), | public | :: | recvBuffer |
My halos which are fluids on remote processes |
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type(tem_communication_type), | public | :: | sendBufferFromCoarser |
Local ghostFromCoarser required by remote processes |
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type(tem_communication_type), | public | :: | sendBufferFromFiner |
Local ghostFromFiner required by remote processes |
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type(tem_communication_type), | public | :: | recvBufferFromCoarser |
My halos which are ghostFromCoarser on remote processes |
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type(tem_communication_type), | public | :: | recvBufferFromFiner |
My halos which are ghostFromFiner on remote processes |
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real(kind=rk), | public, | allocatable | :: | visc(:) |
Normalized turbulence viscosity i.e. viscosity scaled to current level i.e. visc/dtL Size: nSize (nFluids+nGhosts+nHalos) Used gradData to compute viscosity for nFluids and nGhosts. This viscosity is interpolated and scaled for setting nonEq term interpolation routines. The source element of interpolation might be halo so they are communicated. Simple scaling assumping norm of strainrate tensor |S| in different level is small: Schneider, A. (2015). A Consistent Large Eddy Approach for Lattice Boltzmann Methods and its Application to Complex Flows. Technical University Kaiserslautern. v_c = 4 v_f. Scaled visc: v^s = v/dt. => v^s_c dtL_c = 4 v^s_f dtL_f => v^s_c = 2 v^s_f Kolmogorov scaling: Touil, H., Ricot, D., & Lévêque, E. (2014). Direct and large-eddy simulation of turbulent flows on composite multi-resolution grids by the lattice Boltzmann method. Journal of Computational Physics, 256, 220–233. v^s_c = 2^(1/3) v^s_f |