1971
DOI: 10.1143/jpsj.30.262
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Unsteady Flow past a Flat Plate Normal to the Direction of Motion

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Cited by 85 publications
(53 citation statements)
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“…Figure 19 shows the temporal variation of the computed bubble length (which is the length of the region of reverse flow on the centerline behind the plate normalized by plate height) obtained from the current simulations. Also included in the plot are results from the experiments of Taneda & Honji [43] and simulations of Koumoutsakos & Shiels [18] and we find an excellent match between the three data sets. Note also that this case demonstrates the ability of the solver to handle infinitesimally thin (membraneous) bodies.…”
Section: Suddenly Accelerated Normalmentioning
confidence: 57%
“…Figure 19 shows the temporal variation of the computed bubble length (which is the length of the region of reverse flow on the centerline behind the plate normalized by plate height) obtained from the current simulations. Also included in the plot are results from the experiments of Taneda & Honji [43] and simulations of Koumoutsakos & Shiels [18] and we find an excellent match between the three data sets. Note also that this case demonstrates the ability of the solver to handle infinitesimally thin (membraneous) bodies.…”
Section: Suddenly Accelerated Normalmentioning
confidence: 57%
“…Fig. 4 depicts how the vortex length normalized by the plate length, s/d, grows as a function of time and compares the simulation results with those of Taneda and Honji (Taneda and Honji, 1971). The vortex length is defined as the distance of the rear stagnation point from the plate (see Fig.…”
Section: Validation and Verificationmentioning
confidence: 96%
“…This leads to the formation of twin vortices behind the flat plate. The development of such vortices was studied experimentally by Taneda and Honji (Taneda and Honji, 1971). For validation, we choose their case with Re=126 to compare with their experimental results.…”
Section: Validation and Verificationmentioning
confidence: 99%
“…The second term in (14), proportional to At and involving volume integration, is +At([w x V x U" + (w.V)U" -w(V.U")],(U"*V)U").…”
Section: Convection Phasementioning
confidence: 99%