Efficient Parallel Solution of the 3D Stationary Boltzmann Transport Equation for Diffusive Problems

To solve the global stage, consuming the most CPU time, the mechanical fields are decomposed in a wavelet basis and the equilibrium is solved only for the largest

However, the study of the non-linear Boltzmann equation for soft potentials without cut-off [ 20 ], and in particular the spectral analysis its linearised version (see for instance [

Here we concentrate just on the effect of a thermal gradient and on the interaction of electrons with phonons and how it can be described by the Boltzmann

We apply the adjoint weighted equation method (AWE) for the direct solution of inverse problems of elasticity where the shear modulus distribution is reconstructed from given

In the second part, the three different methods for the computation of the seismic waves in the frequency-domain are discussed: (1) the time-domain approach combined with a

In overlapping Schwartz methods (3), the solutions are computed on overlapping domains and the boundary conditions for a given domain are defined at the

For the Landau equation, lower and upper bounds for the solution have been obtained in [21] using integration by parts techniques based on the classical Malliavin calculus..

As explained in section 3.4, a preliminary study reveals that the SP N iterative solver can be set up to perform only one iteration per resolution of equations (14), (15) or (16).