2003
DOI: 10.1016/s0021-9991(03)00323-1
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An adaptive numerical scheme for high-speed reactive flow on overlapping grids

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Cited by 81 publications
(138 citation statements)
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“…Note here that this slice is sufficiently removed from the computational boundaries so that no disturbance generated at the boundaries has yet had opportunity to interact with it. The computational method is a second-order highresolution Godunov method as discussed in [14]. Errors are computed using the L 1 norm for all primitive quantities and results presented in Table 6 Convergence results for shock polar along the line x = −0.25 for y ∈ [0, 0.2].…”
Section: More Complex Flowsmentioning
confidence: 99%
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“…Note here that this slice is sufficiently removed from the computational boundaries so that no disturbance generated at the boundaries has yet had opportunity to interact with it. The computational method is a second-order highresolution Godunov method as discussed in [14]. Errors are computed using the L 1 norm for all primitive quantities and results presented in Table 6 Convergence results for shock polar along the line x = −0.25 for y ∈ [0, 0.2].…”
Section: More Complex Flowsmentioning
confidence: 99%
“…On the other hand, the importance of accurate treatment of all discontinuities, including linear jumps, is paramount in the overall efficacy of a given simulation. The difficulties associated with the computation of discontinuous solutions has been the driver behind such developments as high-resolution methods [10][11][12] and adaptive mesh refinement [13,14].…”
Section: Introductionmentioning
confidence: 99%
“…The second special case involves a more difficult set of equations given by the reactive Euler equations. This set of equations was considered in our previous papers [2] and [3] for two-dimensional flow in stationary and moving domains. Here, our focus is on reactive and non-reactive flow in three dimensions for which we consider the nonlinear conservation equations given by…”
Section: Model Equationsmentioning
confidence: 99%
“…The first is a linear advection-diffusion equation, and the second is the (nonlinear) reactive Euler equations of gas dynamics. The first equation provides a useful test case to study the behavior of the numerical approach and to verify its accuracy quantitatively, while the second builds on our earlier work in [2,3] and illustrates the numerical approach for a more difficult set of equations. While a brief description of the discretization of these two PDEs is given, the emphasis of the discussion is on the extension of the numerical approach for parallel computations in three-dimensional geometries.…”
Section: Introductionmentioning
confidence: 99%
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