A long and narrow solid strip coated with a thin liquid layer is used as a model of a generic fluid mass probe in a spacecraft propellant tank just after a small thruster firing. The drainage dynamics of the initial coating layer into the settled bulk fluid affects the interpretation of probe measurements as the sensors' signal depends strongly on whether a sensor is in contact with vapor or with liquid. We analyze the drainage under various conditions of zero-gravity (i.e., capillary drainage) and with gravity aligned with the strip length, corresponding to the thruster acceleration. Long-time analytical solutions are found for zero and non-zero gravity. In the case with gravity, an approximate solution is found using matched asymptotics. Estimates show that a thrust of 10−3g0 significantly reduces drainage times.

1.
A. A.
Darhuber
,
S. M.
Troian
,
J. M.
Davis
, and
S. M.
Miller
, “
Selective dip-coating of chemically micropatterned surfaces
,”
J. Appl. Phys.
88
,
5119
5126
(
2000
).
2.
J. M.
Davis
, “
Asymptotic analysis of liquid films dip-coated onto chemically micropatterned surfaces
,”
Phys. Fluids
17
,
038101
(
2005
).
3.
V.
Levich
,
Physicochemical Hydrodynamics
(
Prentice-Hall
,
Englewood Cliffs, NJ
,
1962
).
4.
M.
Weislogel
and
S.
Lichter
, “
Capillary flow in an interior corner
,”
J. Fluid Mech.
373
,
349
378
(
1998
).
5.
P.
Ayyaswamy
,
I.
Catton
, and
D.
Edwards
, “
Capillary flow in triangular grooves
,”
Trans. ASME: J. Appl. Mech.
41
,
332
336
(
1974
).
6.
L.
Romero
and
F.
Yost
, “
Flow in an open channel capillary
,”
J. Fluid Mech.
322
,
109
129
(
1996
).
7.
A.
Kovscek
and
C.
Radke
, “
Gas bubble snap-off under pressure-driven flow in constricted noncircular capillaries
,”
Colloids Surf. A
117
,
55
76
(
1996
).
8.
T.
Ransohoff
and
C.
Radke
, “
Laminar flow of a wetting liquid along the corners of a predominantly gas-occupied noncircular pore
,”
J. Colloid Interface Sci.
121
,
392
401
(
1988
).
9.
M.
Dong
and
I.
Chatzis
, “
The imbibition and flow of a wetting liquid along the corners of a square capillary
,”
J. Colloid Interface Sci.
172
,
278
288
(
1995
).
10.
C. A.
Perazzo
and
J.
Gratton
, “
Navier–Stokes solutions for parallel flow in rivulets on an inclined plane
,”
J. Fluid Mech.
507
,
367
379
(
2004
).
11.
N.
Tiwari
,
Z.
Mester
, and
J. M.
Davis
, “
Stability and transient dynamics of thin liquid films flowing over locally heated surfaces
,”
Phys. Rev. E
76
,
056306
(
2007
).
12.
U.
Rosendahl
,
A.
Ohlhoff
, and
M. E.
Dreyer
, “
Choked flows in open capillary channels: Theory, experiment and computations
,”
J. Fluid Mech.
518
,
187
214
(
2004
).
13.
U.
Rosendahl
,
A.
Grah
, and
M. E.
Dreyer
, “
Convective dominated flows in open capillary channels
,”
Phys. Fluids
22
,
052102
(
2010
).
14.
This is the result of using f a(1 − z)1/4 − 16(1 − z)3/2/45a2 to compute initial conditions at z = 1 − ε, and finding a such that the boundary condition f ′(0) = 0 is satisfied, viz., a ≈ 1.44026.
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