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The Boltzmann transport equation under the gray relaxation-time approximation was numerically solved by discretizing the angular domain with the discrete ordinate method (DOM) and the spatial domain with the FEA.
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This paper describes the wavelet expansion method for discretizing the angular and spatial variables in the neutron transport equation.
This scheme is obtained by discretizing the implicit scheme (3.3).
The spatial movement stage can be obtained by discretizing the spatial terms of Eqs.
System (1) is derived by discretizing the original continuous-time system under the sampling period h.
We begin by discretizing the operator following the idea of Pérez (see [16]): (2.2).
Consequently, by discretizing the continuous implicit method, we provide an explicit general iterative method.
A linearization approach is adopted by discretizing the searched space for temperatures.
The numerical method is derived by discretizing the weak formulation.
In this subsection we carry out an exhaustive search of selective perturbations by discretizing the control parameters and signaling variables.
Then we formed scaling factors r1, r2, r3 by discretizing the distribution.
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