1983
DOI: 10.2514/3.8079
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Inviscid axisymmetric jet impingement with recirculating stagnation regions

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Cited by 21 publications
(10 citation statements)
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“…Looney & Walsh (1984) and Bouainouche et al (1997) considered the impinging turbulent plane jet. The second approach to describing impinging jet flow fields involves separating the flow into regions where distinct approximations of the Navier-Stokes equations are valid (Strand 1964;Scholtz & Trass 1970;Rubel 1980Rubel , 1983. This approach is more desirable for our purposes, since we are mainly concerned with the small region of flow located just above the impingement plane, where boundary layer approximations can be made.…”
Section: Introductionmentioning
confidence: 99%
“…Looney & Walsh (1984) and Bouainouche et al (1997) considered the impinging turbulent plane jet. The second approach to describing impinging jet flow fields involves separating the flow into regions where distinct approximations of the Navier-Stokes equations are valid (Strand 1964;Scholtz & Trass 1970;Rubel 1980Rubel , 1983. This approach is more desirable for our purposes, since we are mainly concerned with the small region of flow located just above the impingement plane, where boundary layer approximations can be made.…”
Section: Introductionmentioning
confidence: 99%
“…͑38͒ with a velocity deficient core. The impingement of this type of profile was also investigated numerically by Rubel,17 who predicted the conditions at which areas of recirculation would develop near the stagnation point. Rubel used a family of velocity profiles described in terms of the location of the maximum velocity, r m , and the core velocity deficiency, d w -the difference between the maximum and centerline velocities.…”
Section: Stagnation Bubbles and Annular Jet Impingementmentioning
confidence: 99%
“…Although the field of jet impingement is extremely rich in the literature ͑see, for example, Martin 11 or Looney and Walsh 12 ͒, only a small number of investigators [13][14][15][16][17] have developed inviscid flow models, thereby enabling separate treatment of the boundary layer. Strand 13 obtained the flow field for potential jet impingement analytically.…”
Section: Introductionmentioning
confidence: 99%
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“…The boundary conditions of U I = 0 along the sphere surface and ∂V I /∂β = ∂W I /∂β = ω I = 0 in the equatorial plane cannot be fulfilled by (2.20) and should be satisfied through the presence of local boundary layers. The solution of (2.20) has been discussed in the literature (Rubel 1983;Phares et al 2000), but here it is further complicated by the presence of a recirculation region where the value of the vorticity is unknown, so that equation (2.20) cannot be solved directly, but we need to solve (2.13)-(2.16) instead. Nevertheless the solution as η → ∞ must approach the inflow, so that the outflow asymptotes to…”
Section: )mentioning
confidence: 99%