Abstract:
The numerical solving of the system of high-temperature radiative gas dynamics (HTRGD) equations is a computationally laborious task, since the interaction of radiation with matter is nonlinear and non-local. The radiation absorption coefficients depend on temperature, and the temperature field is determined by both gas-dynamic processes and radiation transport. The method of splitting into physical processes is usually used to solve the HTRGD system, one of the blocks consists of a joint solving of the radiative transport equation and the energy balance equation of matter under known pressure and temperature fields. Usually difference schemes with orders of convergence no higher than the second are used to solve this block. Due to computer memory limitations it is necessary to use not too detailed grids to solve complex technical problems. This increases the requirements for the order of approximation of difference schemes. In this work, bicompact schemes of a high order of approximation for the algorithm for the joint solution of the radiative transport equation and the energy balance equation are implemented for the first time. The proposed method can be applied to solve a wide range of practical problems, as it has high accuracy and it is suitable for solving problems with coefficient discontinuities. The non-linearity of the problem and the use of an implicit scheme lead to an iterative process that may slowly converge. In this paper, we use a multiplicative HOLO algorithm named the quasi-diffusion method by V.Ya.Goldin. The key idea of HOLO algorithms is the joint solving of high order (HO) and low order (LO) equations. The high-order equation (HO) is the radiative transport equation solved in the energy multigroup approximation, the system of quasi-diffusion equations in the multigroup approximation (LO$_1$) is obtained by averaging HO equations over the angular variable. The next step is averaging over energy, resulting in an effective one-group system of quasi-diffusion equations (LO$_2$), which is solved jointly with the energy equation. The solutions obtained at each stage of the HOLO algorithm are closely related that ultimately leads to an acceleration of the convergence of the iterative process. Difference schemes constructed by the method of lines within one cell are proposed for each of the stages of the HOLO algorithm. The schemes have the fourth order of approximation in space and the third order of approximation in time. Schemes for the transport equation were developed by B.V. Rogov and his colleagues, the schemes for the LO$_1$ and LO$_2$ equations were developed by the authors. An analytical test is constructed to demonstrate the declared orders of convergence. Various options for setting boundary conditions are considered and their influence on the order of convergence in time and space is studied.
Keywords:transport equation, quasi-diffusion method, HOLO algorithms for transport equation solving, diagonally implicit Runge – Kutta method
Citation:
E. N. Aristova, N. I. Karavaeva, “Bicompact schemes for the HOLO algorithm for joint solution of the transport equation and the energy equation”, Computer Research and Modeling, 15:6 (2023), 1429–1448
\Bibitem{AriKar23}
\by E.~N.~Aristova, N.~I.~Karavaeva
\paper Bicompact schemes for the HOLO algorithm for joint solution of the transport equation and the energy equation
\jour Computer Research and Modeling
\yr 2023
\vol 15
\issue 6
\pages 1429--1448
\mathnet{http://mi.mathnet.ru/crm1127}
\crossref{https://doi.org/10.20537/2076-7633-2023-15-6-1429-1448}
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https://www.mathnet.ru/eng/crm1127
https://www.mathnet.ru/eng/crm/v15/i6/p1429
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