1999
DOI: 10.1007/s007910050021
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Error estimators for the position of discontinuities in hyperbolic conservation laws with source terms which are solved using operator splitting

Abstract: When computing numerical solutions of hyperbolic conservation laws with source terms, one may obtain spurious solutions | these are unphysical solutions that only occur in numerics such a s s h o c k w aves moving with wrong speeds, cf. 7], 2], 1], 10], 3]. Therefore it is important to know h o w errors of the location of a discontinuity can be controlled.To d e r i v e appropriate error-estimates and to use them to control such errors, is the aim of our investigations in this paper. We restrict our considerat… Show more

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Cited by 15 publications
(16 citation statements)
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“…Eq. (1) is an advection equation with constant propagation speed a and with a nonlinear source term SðuÞ that becomes stiff for large m. The introduction of the more complex advection equation with variable propagation speed, as proposed in [7,17,19], does not modify the mechanism of generation of spurious wave speeds here investigated. Given the selected initial condition, it is easy to verify that the exact solution is…”
Section: The Scalar Problemmentioning
confidence: 93%
See 2 more Smart Citations
“…Eq. (1) is an advection equation with constant propagation speed a and with a nonlinear source term SðuÞ that becomes stiff for large m. The introduction of the more complex advection equation with variable propagation speed, as proposed in [7,17,19], does not modify the mechanism of generation of spurious wave speeds here investigated. Given the selected initial condition, it is easy to verify that the exact solution is…”
Section: The Scalar Problemmentioning
confidence: 93%
“…The scalar model problem, although insufficient to reproduce the physics of rapid combustion, does feature the same numerical difficulties observed in reacting flow problems and allows to easily understand the very nature of them [4]. For this reason it has been considered as a first step in the developments of numerical methods for this class of problems also in [7,17,19].…”
Section: Introductionmentioning
confidence: 96%
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“…Geometry of the post-shock burnt gas part follows {|y − 0.5| > 0. 25 and the unburnt gas occupies the rest of domain before the initial shock. Initial states are identical with those in Example 6 except the x-velocity of the post-shock part is increased to u b = 2000m/s > u CJ , to create a strong detonation wave.…”
Section: Reactive Euler Equations With Real-world Nonequilibrium Kinementioning
confidence: 99%
“…Therefore, many works have contributed to the analysis and development of underresolved numerical methods which are able to capture the correct shock/discontinuities location and speed without resolving the small chemical scales. Examples include the level set and front tracking methods [6,19,23,26,30], random choice method [10][11][12]24], random projection method [1][2][3] and many other works [4, 5, 7-9, 13, 14, 16, 17, 25, 27, 31, 32]. See Wang et al [33] for a comprehensive overview of the last two decades of this development.…”
Section: Introductionmentioning
confidence: 99%