1977
DOI: 10.32917/hmj/1206135965
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Stability of difference schemes for nonsymmetric linear hyperbolic systems with variable coefficients

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Cited by 10 publications
(3 citation statements)
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“…where k ε max the maximal norm of all wave vectors in the medium which can be estimated by ρ(ε)k max with k max being the maximal wave vector of the initial pulse in vacuum and ρ(ε) the maximal spectral radius of the symmetric matrix ε(x) over x (or simply the maximum of ε(x) if the medium is isotropic). This can be understood from the following principle [17]. A finite difference scheme with variable coefficients is stable if all the corresponding schemes with frozen (i.e., fixed to a particular value everywhere in space) coefficients are stable.…”
Section: A Modified Temporal Leapfrog Schemementioning
confidence: 99%
See 1 more Smart Citation
“…where k ε max the maximal norm of all wave vectors in the medium which can be estimated by ρ(ε)k max with k max being the maximal wave vector of the initial pulse in vacuum and ρ(ε) the maximal spectral radius of the symmetric matrix ε(x) over x (or simply the maximum of ε(x) if the medium is isotropic). This can be understood from the following principle [17]. A finite difference scheme with variable coefficients is stable if all the corresponding schemes with frozen (i.e., fixed to a particular value everywhere in space) coefficients are stable.…”
Section: A Modified Temporal Leapfrog Schemementioning
confidence: 99%
“…Here the idea of the frozen coefficients [17] has been used again. The left hand side of inequality (5.16) is nothing but the spectral radius of ∆tH F 0 with frozen plasma frequencies so that ω p = ω max p .…”
Section: An Example Of the Lorentz Modelmentioning
confidence: 99%
“…Typical examples are Friedrichs-Lax scheme and modified Lax-Wedroff scheme. (See Yamaguti and Nogi [6], Kametaka [9], Vaillancourt [8], Koshiba-Kumanogo [10], Sintani-Tomoeda [11], etc.) An A-stability theorem similar to Theorem 1.2 was given for a dissipative scheme of dissipative hermitian systems by B. Gustafsson [7].…”
Section: For All X and T;' A Smooth Diagonalizer î'(X T;') Or Symmementioning
confidence: 99%