2010
DOI: 10.1134/s0015462810050029
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Numerical modeling of three-dimensional vortex structures in hypersonic transverse flow past a cylinder

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Cited by 3 publications
(2 citation statements)
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“…The third mechanism was proposed in works 3,4 where it was shown that in case of transverse hypersonic (M ∞ ≥ 5) flow past bodies with cylindrical bluntness of the frontal surface, a steady-state 3D flow mode consisting of paired vortices that are periodic along Z axis of the cylinder can exist simultaneously with a plane (two-dimensional) mode. Physical essence of the third mechanism is the following.…”
Section: Introductionmentioning
confidence: 97%
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“…The third mechanism was proposed in works 3,4 where it was shown that in case of transverse hypersonic (M ∞ ≥ 5) flow past bodies with cylindrical bluntness of the frontal surface, a steady-state 3D flow mode consisting of paired vortices that are periodic along Z axis of the cylinder can exist simultaneously with a plane (two-dimensional) mode. Physical essence of the third mechanism is the following.…”
Section: Introductionmentioning
confidence: 97%
“…[1][2][3][4][5] One can distinguish three basic mechanisms representing physical reasons for the development of such structures: I) external excitation of vortices induced by spatial inhomogeneity of the free stream or boundary conditions on the body; II) internal excitation caused by the development of transverse flow instability in the neighborhood of the leading stagnation line (Taylor-Görtler instability, for example) 2 ; III) self-generation of spanperiodic structures under homogeneous external conditions supported by a strong interaction between the bow shock and the vortex flow in the compressed layer. [3][4][5] The fact that vortex structures can appear as a result of external impact is theoretically understood and in the present study the first mechanism is considered only as one way of initial perturbation of the primary (plane) flow mode.…”
Section: Introductionmentioning
confidence: 99%