2015
DOI: 10.1016/j.compfluid.2015.07.023
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Further study on the geometric conservation law for finite volume method on dynamic unstructured mesh

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Cited by 12 publications
(12 citation statements)
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“…(43) are equivalent, but as with Eqs. (34), (25) and (29), these relationships are not satisfied upon discretization. Therefore, for reference purposes, results obtained using this discretization are referred to as being obtained with the "inconsistent" method.…”
Section: Methods 1 Methodsmentioning
confidence: 99%
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“…(43) are equivalent, but as with Eqs. (34), (25) and (29), these relationships are not satisfied upon discretization. Therefore, for reference purposes, results obtained using this discretization are referred to as being obtained with the "inconsistent" method.…”
Section: Methods 1 Methodsmentioning
confidence: 99%
“…35, the time derivative of (QJ) has been rewritten in a nonconservative form. While common, [28][29][30] this approach requires investigation to quantify potentially undesirable effects. Additionally, this relationship is similar to Eqs.…”
Section: ∂ ∂T ω(T)mentioning
confidence: 99%
“…to satisfy the DGCL, the volume V * ,n+1 must be modified [21]. With the firstorder Euler time discretized scheme, Eq.…”
Section: Geometric Conservation Lawmentioning
confidence: 99%
“…As the DGCL scheme1 is much easy to implement, and only one time level (F n+1/2 ) is needed to calculate the flux at cell interface, it can natural couple with current ALE-type DUGKS. Though DGCL scheme2 and scheme3 are much complex, further improved ALE-type DUGKS framework such as highorder DUGKS [28] or multi-time-level implicit method [21] which the geometry information at intermediate time-levels are much difficult to define [29], these two schemes are the good choice. Besides, the scheme2 and scheme3 are the volume-constrained scheme, the face-constrained scheme [21] also can be used but not considered in this paper.…”
Section: Geometric Conservation Lawmentioning
confidence: 99%
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