2002
DOI: 10.1007/s004660100261
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Channel flow past bluff-body: outlet boundary condition, vortex shedding and effects of buoyancy

Abstract: Structure of laminar¯ow and heat transfer, in a two-dimensional horizontal plane channel differentially heated, with a built-in triangular prism is investigated from the numerical solutions of complete Navier±Stokes and energy equations. Results are obtained for Reynolds and Grashof numbers ranging respectively from 30 to 200 and from 0 to 1.5´10 4 at Pr 0.71. In forced convection, results are specially presented to show how the vortex shedding at downstream affects the upstream. Also, two correlations giving … Show more

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Cited by 25 publications
(14 citation statements)
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“…The inlet velocity profile is parabolic while the exit boundary conditions are chosen to minimize the distortion of the unsteady vortices shed from the cylinder and to reduce perturbations that reflect back in to the domain. A detailed investigation carried out by Abbassi et al (2002) show that the convective boundary condition (CBC) given by:…”
Section: Governing Equationsmentioning
confidence: 99%
“…The inlet velocity profile is parabolic while the exit boundary conditions are chosen to minimize the distortion of the unsteady vortices shed from the cylinder and to reduce perturbations that reflect back in to the domain. A detailed investigation carried out by Abbassi et al (2002) show that the convective boundary condition (CBC) given by:…”
Section: Governing Equationsmentioning
confidence: 99%
“…It is noted here that, as mentioned by Sohankar et al [22] and Abbassi et al [23], the convective boundary condition reduces the number of iterations per time step and allows a shorter downstream computational domain when compared to the case of the Neumann boundary condition. The square obstacle is assumed to be isothermally heated at ℎ , exchanging heat to the fluid flowing around it.…”
Section: Governing Equationsmentioning
confidence: 69%
“…Previous studies also yielded the relation of the recirculation length varying with Re for squares [10,11] and triangulars [12], as well as the linear relation of vortex shedding frequency, St , varying with 1/2 Re  for squares and triangles [13]. For the inviscid flow past polygonal obstacles, we also found studies for pure potential flow [14] and the vortex flow [15,16].…”
Section: Introductionmentioning
confidence: 77%
“…(13), which involves the equivalent Reynolds number, to study the features of viscous flow past odd-sided polygons, including the 1st critical Reynolds numbers and flow patterns. In this paper, we only consider the polygon whose rear stagnation point coincides with one of its apices.…”
Section: Viscous Flow Past Polygonsmentioning
confidence: 99%
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