P. Grassia et Gm. Homsy, THERMOCAPILLARY AND BUOYANT FLOWS WITH LOW-FREQUENCY JITTER - I - JITTER CONFINED TO THE PLANE, Physics of fluids (1994), 10(6), 1998, pp. 1273-1290
A temperature gradient is applied along a fluid filled slot with a fla
t upper interface, establishing how via thermocapillarity and/or buoya
ncy. There is a known parallel. flow along the slot, in which the flui
d velocity varies vertically, and there is a known convected temperatu
re profile. This parallel flow is then subjected to gravitational modu
lation or ''jitter'' which is applied at low frequency and in various
directions. For gravity modulations in the plane of the basic flow, an
alytic solutions for velocity and temperature profiles are obtained fo
r jitter of arbitrary amplitude. These solutions involve modifications
to the earlier parallel flow solutions. Jitter in the vertical direct
ion generates vorticity due to coupling with the applied horizontal te
mperature gradient. This alternately cooperates or competes with the s
teady basic how over a cycle of the modulation, but does not qualitati
vely change the flow or temperature profiles. Jitter applied along the
slot produces vorticity only when coupled to vertical convected tempe
rature gradients and so is important when the basic flow is sufficient
ly strong (large Marangoni and/or Rayleigh number). Various cases are
considered for the basic flow, which may be driven by thermocapillarit
y alone, by vertical gravity alone or by a mixture of thermocapillarit
y and Vertical gravity. When strong streamwise jitter is added to any
of these cases, the flow profile alternates during the modulation cycl
e between boundary layer structures and vertically stacked cells. The
type of structure selected depends on the sense of the horizontal ther
mal stratification with respect to the jitter, and in that part of the
cycle where this stratification is unstable, there are particular amp
litudes of jitter which can give strong cellular motions or runaways.
These runaways represent a resonant interaction with stationary Raylei
gh-Benard cells. (C) 1998 American Institute of Physics.