1994
DOI: 10.1016/0301-679x(94)90023-x
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Stability of a rigid rotor in turbulent hybrid porous journal bearings

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Cited by 12 publications
(13 citation statements)
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“…Basic geometry of the four-lobe four pocket hybrid journal bearing is illustrated in Figure 1. For a finite journal bearing system operating in turbulent regime, the usual Reynolds equation is modified by using turbulent lubrication theory of Constantinecscu and is expressed as follows 35 where, G¯α and G¯β are turbulent coefficients and functions of local Reynolds number Re* in turbulent regime 35,42
Figure 1.Geometrically imperfect four-lobe four pocket hybrid journal bearing.
…”
Section: Discussionmentioning
confidence: 99%
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“…Basic geometry of the four-lobe four pocket hybrid journal bearing is illustrated in Figure 1. For a finite journal bearing system operating in turbulent regime, the usual Reynolds equation is modified by using turbulent lubrication theory of Constantinecscu and is expressed as follows 35 where, G¯α and G¯β are turbulent coefficients and functions of local Reynolds number Re* in turbulent regime 35,42
Figure 1.Geometrically imperfect four-lobe four pocket hybrid journal bearing.
…”
Section: Discussionmentioning
confidence: 99%
“…The frictional torque exerted on journal surface is defined in nondimensional form as 35,42 where, τ¯c is known as normalized turbulent coquette shearing stress and defined as τ¯c =1, for laminar flow …”
Section: Discussionmentioning
confidence: 99%
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“…[1] to [3] by substituting Eq. [5] and gathering the e 0 ; e 1 e it and e 0 f 1 e it terms, a set of linear differential equations in p , and p 0 are solved simultaneously with appropriate boundary conditions for steady-state pressures in the film as well as porous regions. The partial derivatives are written in finite difference form using a central difference method and then solved by using the Gauss-Seidel iteration method with a successive overrelaxation (SOR) scheme.…”
Section: Linearized Methodsmentioning
confidence: 99%