1988
DOI: 10.1007/978-1-4613-9874-5_53
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Turbulent Transport of He II in Active and Passive Phase Separators Using Slit Devices and Porous Media

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Cited by 3 publications
(2 citation statements)
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“…24 It has been known for some time that the transition from linear flow to chaos is quite complex, as shown by Tough 28 for ZNMF. The recent nonlinear VLPS regime of the slit device has been described 23 x(p,ST) 3 S(p,/p m )(tiJp)drt (29) (where T u = T d + AJ). The related mass-flux density j 0 (=mass flow rate m divided by the total plug cross section) is Jo = (30) It has been recognized for a considerable time that mutual friction in porous media and fine ducts is altered significantly, in particular for fine pores.…”
Section: Nonlinear Vlps Regimementioning
confidence: 99%
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“…24 It has been known for some time that the transition from linear flow to chaos is quite complex, as shown by Tough 28 for ZNMF. The recent nonlinear VLPS regime of the slit device has been described 23 x(p,ST) 3 S(p,/p m )(tiJp)drt (29) (where T u = T d + AJ). The related mass-flux density j 0 (=mass flow rate m divided by the total plug cross section) is Jo = (30) It has been recognized for a considerable time that mutual friction in porous media and fine ducts is altered significantly, in particular for fine pores.…”
Section: Nonlinear Vlps Regimementioning
confidence: 99%
“…20 and subsequent VLPS work. 23 In the latter reference, it has been possible to show that the slit device is subject to limitations similar to those of the porous plug. The apparently "linear regime" of the VLPS slit has been identified as an analog of ZNMF conditions in the nonlinear regime in wide ducts.…”
Section: Introductionmentioning
confidence: 96%