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  • Cambridge University Press (CUP)  (17)
  • Davis, S. H.  (17)
Medientyp
Verlag/Herausgeber
  • Cambridge University Press (CUP)  (17)
Sprache
Erscheinungszeitraum
  • 1
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1987
    In:  Journal of Fluid Mechanics Vol. 174 ( 1987-01), p. 327-356
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 174 ( 1987-01), p. 327-356
    Kurzfassung: We consider the oscillatory motion of a solid plate into and out of a bath of liquid. Assuming that the displacement amplitude of the plate motion is small and that the capillary number is small, the problem reduces to solving an interfacial boundaryvalue problem for the response of the contact line. The characteristic contact angle versus contact-line speed relationship includes contact-angle hysteresis which is assumed small and comparable to the amplitude of the plate motion. Sinusoidal and square-wave plate motions are considered. We find that the contact line moves with the plate if the contact line is fixed, but has relative motion otherwise. It would then advance part of the time, recede part of the time, and remain stationary in the transition periods. Further, we find that both contact-angle hysteresis and steepening of the contact angle with increasing contact-line speed are dissipative effects.
    Materialart: Online-Ressource
    ISSN: 0022-1120 , 1469-7645
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1987
    ZDB Id: 1472346-3
    ZDB Id: 218334-1
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  • 2
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1984
    In:  Journal of Fluid Mechanics Vol. 144 ( 1984-07), p. 133-151
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 144 ( 1984-07), p. 133-151
    Kurzfassung: A horizontal layer is heated from below and cooled from above so that the enclosed single-component liquid is frozen in the upper part of the layer. When the imposed temperature difference is such that the Rayleigh number across the liquid is supercritical, there is Bénard convection coupled with the dynamics of the solidification interface. An experiment is presented which shows that the interfacial corrugations that result are two-dimensional when this solid is thin but hexagonal when the solid is thick. A weakly nonlinear convective instability theory is presented which explains this behaviour, and isolates this ‘purely thermal’ mechanism of pattern selection. Jump behaviour is seen in the liquid-layer thickness at the onset of hexagonal convection.
    Materialart: Online-Ressource
    ISSN: 0022-1120 , 1469-7645
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1984
    ZDB Id: 1472346-3
    ZDB Id: 218334-1
    Bibliothek Standort Signatur Band/Heft/Jahr Verfügbarkeit
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  • 3
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1988
    In:  Journal of Fluid Mechanics Vol. 195, No. -1 ( 1988-10), p. 463-
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 195, No. -1 ( 1988-10), p. 463-
    Materialart: Online-Ressource
    ISSN: 0022-1120 , 1469-7645
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1988
    ZDB Id: 1472346-3
    ZDB Id: 218334-1
    Bibliothek Standort Signatur Band/Heft/Jahr Verfügbarkeit
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  • 4
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1992
    In:  Journal of Fluid Mechanics Vol. 242 ( 1992-09), p. 529-547
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 242 ( 1992-09), p. 529-547
    Kurzfassung: A long-wave evolution equation is used to study a falling film on a vertical plate. For certain wavenumbers there exists a two-dimensional strongly nonlinear permanent wave. A new secondary instability is identified in which the three-dimensional disturbance is spatially synchronous with the two-dimensional wave. The instability grows for sufficiently small cross-stream wavenumbers and does not require a threshold amplitude; the two-dimensional wave is always unstable. In addition, the nonlinear evolution of three-dimensional layers is studied by posing various initial-value problems and numerically integrating the long-wave evolution equation.
    Materialart: Online-Ressource
    ISSN: 0022-1120 , 1469-7645
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1992
    ZDB Id: 1472346-3
    ZDB Id: 218334-1
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  • 5
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1996
    In:  Journal of Fluid Mechanics Vol. 321 ( 1996-08-25), p. 279-298
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 321 ( 1996-08-25), p. 279-298
    Kurzfassung: We consider a long-wave evolution equation that governs a draining film on a heated plate and hence is capable of describing both surface-wave and thermocapillary instabilities. When the flow and heat transfer rates are moderate, we show, via weakly nonlinear analysis of a truncated system and numerical simulation of the full nonlinear evolution equation, that coupled temporal instabilities can create surface deformations that lead to an array of rivulets aligned with the flow. This work thus demonstrates a mechanism of rivulet formation based solely on instability phenomena.
    Materialart: Online-Ressource
    ISSN: 0022-1120 , 1469-7645
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1996
    ZDB Id: 1472346-3
    ZDB Id: 218334-1
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  • 6
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1994
    In:  Journal of Fluid Mechanics Vol. 277 ( 1994-10-25), p. 55-83
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 277 ( 1994-10-25), p. 55-83
    Kurzfassung: We consider the two-layer flow of immiscible, viscous, incompressible fluids in an inclined channel. We use long-wave theory to obtain a strongly nonlinear evolution equation which describes the motion of the interface. This equation includes the physical effects of viscosity stratification, density stratification, and shear. A weakly nonlinear analysis of this equation yields a Kuramoto–Sivashinsky equation, which possesses a quadratic nonlinearity. However, certain physical situations exist in two-layer flow for which modifications of the Kuramoto–Sivashinsky equation are physically pertinent. In particular, the presence of the second layer can mediate the wave-steepening instability found in single-phase falling films, requiring the inclusion of a cubic nonlinearity in the weakly nonlinear analysis. The introduction of the cubic nonlinearity destroys the symmetry-breaking bifurcations of the Kuramoto–Sivashinsky equation, and new isolated solution branches emerge as the strength of the cubic nonlinearity increases. Bistability between these new solutions and those associated with the Kuramoto–Sivashinsky equation is found, as well as the formation of a hysteresis loop from smaller-amplitude travelling waves to larger-amplitude travelling waves. The physical implications of these dynamics to the phenomenon of laminar flooding in a channel are discussed.
    Materialart: Online-Ressource
    ISSN: 0022-1120 , 1469-7645
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1994
    ZDB Id: 1472346-3
    ZDB Id: 218334-1
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  • 7
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1982
    In:  Journal of Fluid Mechanics Vol. 120 ( 1982-07), p. 91-122
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 120 ( 1982-07), p. 91-122
    Kurzfassung: We consider liquid in a circular cylinder that undergoes nonlinear Marangoni insta- bility. The upper free surface of the liquid is taken to have large-enough surface tension that surface deflections are neglected. The side walls are adiabatic and impenetrable, and for mathematical simplicity the liquid is allowed to slip on the side walls. The linearized stability theory for heating from below gives the critical Marangoni number Mc as a function of cylinder dimensions, surface-cooling condition and Rayleigh number. The steady nonlinear convective states near Mc are calculated using an asymptotic theory, and the stability of these states is examined. At simple eigenvalues Mc the finite-amplitude states are determined. We find th at the Prandtl number of the liquid influences the stability of axisymmetric states, distinguishing upflow at the centre from downflow. Near those aspect ratios corresponding to double eigenvalues Me, where two convective states of linear theory are equally likely, the nonlinear theory predicts sequences of transitions from one steady convective state to another as the Marangoni number is increased. These transitions are determined and discussed in detail. Time-periodic convection is possible in certain cases.
    Materialart: Online-Ressource
    ISSN: 0022-1120 , 1469-7645
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1982
    ZDB Id: 1472346-3
    ZDB Id: 218334-1
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  • 8
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1995
    In:  European Journal of Applied Mathematics Vol. 6, No. 6 ( 1995-12), p. 639-652
    In: European Journal of Applied Mathematics, Cambridge University Press (CUP), Vol. 6, No. 6 ( 1995-12), p. 639-652
    Kurzfassung: A binary liquid that undergoes directional solidification is susceptible to morphological instabilities which cause the solid/liquid interface to change from a planar to a cellular state. This paper presents a numerical study of a class of long-wave equations that describe the evolution of interface morphology. We find new bifurcation points, new solution branches, and the existence of inverted hexagonal nodes and cells.
    Materialart: Online-Ressource
    ISSN: 0956-7925 , 1469-4425
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1995
    ZDB Id: 2002906-8
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  • 9
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1994
    In:  Journal of Fluid Mechanics Vol. 268 ( 1994-06-10), p. 231-265
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 268 ( 1994-06-10), p. 231-265
    Kurzfassung: We consider steady two-dimensional fluid flow and heat transfer near contact lines in single-phase and two-phase systems. Both single- and double-wedge geometries admit separable solutions in plane polar coordinates for both thermal and flow fields. We consider the class of functions which have bounded temperatures and velocities at the corner. When free surfaces are present, we seek local solutions , those that satisfy all local boundary conditions, and partial local solutions , those that satisfy all but the normal-stress boundary condition. Our aim in this work is to describe local fluid and heat flow in problems where these fields are coupled by determining for which wedge angles solutions exist, identifying singularities in the heat flux and stress which are present at contact lines, and determining the dependence of these singularities on the wedge angles. For thermal fields in two phases we identify two modes of heat transfer that are analogous to the two modes identified by Proudman & Asadullah (1988) for two-fluid flow. For non-isothermal flow, locally, convection does not play a role but coupling through thermocapillary effects on non-isothermal free surfaces can arise. We find that under non-isothermal conditions a planar free surface must leave a planar rigid boundary at an angle of π, the same angle found by Michael (1958) for an isothermal rigid/free wedge, in order to satisfy all local boundary conditions. Finally, we find that situations arise where no coupled solutions of the form sought can be found; we discuss means by which alternative solutions can be obtained.
    Materialart: Online-Ressource
    ISSN: 0022-1120 , 1469-7645
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1994
    ZDB Id: 1472346-3
    ZDB Id: 218334-1
    Bibliothek Standort Signatur Band/Heft/Jahr Verfügbarkeit
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  • 10
    Online-Ressource
    Online-Ressource
    Cambridge University Press (CUP) ; 1991
    In:  Journal of Fluid Mechanics Vol. 230 ( 1991-09), p. 117-146
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 230 ( 1991-09), p. 117-146
    Kurzfassung: A layer of volatile viscous liquid drains down a uniformly heated inclined plate. Long-wave instabilities of the uniform film are studied by deriving an evolution equation for two-dimensional disturbances. This equation incorporates viscosity, gravity, surface tension, thermocapillarity, and evaporation eifects. The linear theory derived from this describes the competition among the instabilities. Numerical solution of the evolution equation describes the finite-amplitude behaviour that determines the propensity for dryout of the film. Among the phenomena that appear are the tendency to wave breaking, the creation of secondary structures, and the preemption of dryout by mean flow.
    Materialart: Online-Ressource
    ISSN: 0022-1120 , 1469-7645
    Sprache: Englisch
    Verlag: Cambridge University Press (CUP)
    Publikationsdatum: 1991
    ZDB Id: 1472346-3
    ZDB Id: 218334-1
    Bibliothek Standort Signatur Band/Heft/Jahr Verfügbarkeit
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