1982
DOI: 10.1017/s0022112082000561
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A numerical study of vortex shedding from rectangles

Abstract: The purpose of this paper is to present numerical solutions for two-dimensional time-dependent flow about rectangles in infinite domains. The numerical method utilizes third-order upwind differencing for convection and a Leith type of temporal differencing. An attempted use of a lower-order scheme and its inadequacies are also described. The Reynolds-number regime investigated is from 100 to 2800. Other parameters that are varied are upstream velocity profile, angle of attack, and rectangle dimensions. The ini… Show more

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Cited by 349 publications
(141 citation statements)
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“…3 and 4, respectively. Some numerical results of Davis and Moore [24], Franke et al [25], Sohankar et al [26], Robichuax et al [27] and Saha et al [28] are also plotted in the figure for comparison. It is seen that the present calculation for the mean drag coefficient at Re = 250 is very close to the experimental data of Shimizu and Tanida [22].…”
Section: Computer Code Validationmentioning
confidence: 99%
“…3 and 4, respectively. Some numerical results of Davis and Moore [24], Franke et al [25], Sohankar et al [26], Robichuax et al [27] and Saha et al [28] are also plotted in the figure for comparison. It is seen that the present calculation for the mean drag coefficient at Re = 250 is very close to the experimental data of Shimizu and Tanida [22].…”
Section: Computer Code Validationmentioning
confidence: 99%
“…In contrast to the inviscid scheme utilized in the previous simulation, a finite difference method (Davis and Moore, [1982]; Davis et al, [1984]) was employed here to study the motions of the particles for various Stokes numbers at a flow Reynolds number of 100. The results are shown in Figure 3 for St = 0.01, 1.0, and 10.0.…”
mentioning
confidence: 99%
“…The higher order scheme of WAM is the second order leapfrog scheme (which has zero numerical diffusion). The higher order scheme of WW3 is the "ULTIMATE QUICKEST" scheme and limiter (see Tolman, 1995;Leonard, 1979;Davis andMoore, 1982, andLeonard, 1991). The QUICKEST scheme is third order when solved in one dimension.…”
Section: Improved Numerical Schemes For Propagation On a Gridmentioning
confidence: 99%