It is known that streaming can be generated in a liquid bridge by vibrating an end wall. This phenomenon has been used in an attempt to minimize thermocapillary flow during crystal growth in a floating zone, by inducing such a streaming running in the opposite direction to it [Grugel et al., J. Cryst. Growth 142, 209 (1994)]. In the present theoretical study, the nature of this streaming and its effects on the average flow and temperature fields in a floating zone are investigated. It is noticed that in the experiment, the applied frequencies were high enough such that the corresponding wavelengths of the capillary ripples were much smaller than the dimensions of the zone. It is believed that the ripples were a traveling wave that generated the streaming in the direction of the wave propagation as a result of Stokes drift. For such a wave to be traveling, it must be dissipated sufficiently by viscosity upon reaching the other wall to guarantee negligible reflection there. Accordingly, a model is formulated to study the reduction of thermocapillary flow in a floating zone by means of streaming. It is found that for a half zone, streaming can minimize the thermocapillary flow near the vibrating wall and make the temperature uniform across the zone there. For a full zone, streaming can minimize the flow but cannot make the temperature uniform near the wall. For a long full zone, streaming can similarly minimize the flow. But in addition, the temperature near each wall is uniform with or without streaming.

1.
D.
Schwabe
,
A.
Scharmann
,
F.
Preisser
, and
R.
Oeder
, “
Experiments on surface tension driven flow in floating zone melting
,”
J. Cryst. Growth
43
,
305
(
1978
).
2.
D.
Schwabe
,
F.
Preisser
, and
A.
Scharmann
, “
Verification of the oscillatory state of thermocapillary convection in a floating zone under low gravity
,”
Acta Astron.
9
,
265
(
1982
).
3.
C. H.
Chun
, “
Marangoni convection in a floating zone under reduced gravity
,”
J. Cryst. Growth
48
,
600
(
1980
).
4.
F.
Preisser
,
D.
Schwabe
, and
A.
Scharmann
, “
Steady and oscillatory thermocapillary convection in liquid columns with free cylindrical surface
,”
J. Fluid Mech.
126
,
545
(
1983
).
5.
R.
Velten
,
D.
Schwabe
, and
A.
Scharmann
, “
The periodic instability of thermocapillary convection in cylindrical liquid bridges
,”
Phys. Fluids A
3
,
267
(
1991
).
6.
Y.
Kamotani
,
S.
Ostrach
, and
A.
Pline
, “
A thermocapillary convection experiment in microgravity
,”
J. Heat Transfer
117
,
611
(
1995
).
7.
S. Ostrach and Y. Kamotani, “Surface tension driven convection experiment-2 (STDCE-2),” Third Microgravity Fluid Physics Conference, NASA Lewis Research Center, Cleveland, OH, 13–15 July 1996 (unpublished).
8.
Y.
Kamotani
,
J.
Masud
, and
A.
Pline
, “
Oscillatory convection due to combined buoyancy and thermocapillarity
,”
J. Thermophys. Heat Transfer
10
,
102
(
1996
).
9.
H.
Kimura
,
M. F.
Harvey
,
D. J.
O’Connor
,
G. D.
Robertson
, and
G. C.
Valley
, “
Magnetic field effects on float-zone Si crystal growth
,”
J. Cryst. Growth
62
,
523
(
1983
).
10.
G. D.
Robertson
, Jr.
and
D.
O’Connor
, “
Magnetic field effects on float-zone Si crystal growth. II
,”
J. Cryst. Growth
76
,
100
(
1986
).
11.
Ch.-H.
Chun
, “
Marangoni convection in a floating zone under reduced gravity
,”
J. Cryst. Growth
48
,
600
(
1980
).
12.
W. W.
Fowlis
and
G. O.
Roberts
, “
Confinement of thermocapillary floating zone flow by uniform rotation
,”
J. Cryst. Growth
74
,
301
(
1986
).
13.
R. F. Dressler, “Suppression or control of liquid convection in float zones in a zero-gravity environment by viscous gas shear,” U.S. Patent 4,615,760 (October 7, 1986).
14.
R. F.
Dressler
and
N. S.
Sivakumaran
, “
Noncontaminating method to reduce Marangoni convection in microgravity float zones
,”
J. Cryst. Growth
88
,
148
(
1988
).
15.
A.
Eyer
and
H.
Leiste
, “
Striation-free silicon crystals by float-zoning with surface-coated melt
,”
J. Cryst. Growth
71
,
249
(
1985
).
16.
C. W.
Lan
and
S.
Kou
, “
Floating-zone crystal growth with a heated ring covering the melt surface
,”
J. Cryst. Growth
108
,
1
(
1991
).
17.
C. W.
Lan
and
S.
Kou
, “
Floating-zone crystal growth with heated and immersed shaper—experiments
,”
J. Cryst. Growth
108
,
541
(
1991
).
18.
H. Lamb, Hydrodynamics, 6th ed. (Dover, New York, 1945).
19.
M. S.
Longuet-Higgins
, “
Mass transport in water waves
,”
Philos. Trans. R. Soc. London, Ser. A
245
,
535
(
1953
).
20.
M. S.
Longuet-Higgins
, “
The trajectories of particles in steep, symmetric gravity waves
,”
J. Fluid Mech.
94
,
497
(
1979
).
21.
S. J.
Hogan
, “
Particle trajectories in nonlinear capillary waves
,”
J. Fluid Mech.
143
,
243
(
1984
).
22.
A. V.
Anilkumar
,
R. N.
Grugel
,
X. F.
Shen
,
C. P.
Lee
, and
T. G.
Wang
, “
Control of thermocapillary convection in a liquid bridge by vibration
,”
J. Appl. Phys.
73
,
4165
(
1993
).
23.
D. J.
Mollot
,
J.
Tsamopoulos
,
T. Y.
Chen
, and
N.
Ashgriz
, “
Nonlinear dynamics of capillary bridges: Experiments
,”
J. Fluid Mech.
255
,
411
(
1993
).
24.
C. P.
Lee
,
A. V.
Anilkumar
, and
T. G.
Wang
, “
Streaming generated in a liquid bridge due to nonlinear oscillations driven by the vibration of an end wall
,”
Phys. Fluids
8
,
3234
(
1996
).
25.
H. C.
Lee
, “
Drop formation in a liquid jet
,”
IBM J. Res. Dev.
18
,
364
(
1974
).
26.
T. Y.
Chen
and
J.
Tsamopoulos
, “
Nonlinear dynamics of capillary bridges: Theory
,”
J. Fluid Mech.
255
,
373
(
1993
).
27.
X. F. Shen, R. N. Grugel, A. V. Anilkumar, and T. G. Wang, “The influence of controlled surface streaming on thermocapillary convection during float-zone processing,” in Microstructural Design by Solidification Processing, edited by E. J. Lavernia and M. N. Gungor (The Minerals, Metals and Materials Society, London, 1992), p. 173.
28.
R. N.
Grugel
,
X. F.
Shen
,
A. V.
Anilkumar
, and
T. G.
Wang
, “
The influence of vibration on microstructural uniformity during floating-zone crystal growth
,”
J. Cryst. Growth
142
,
209
(
1994
).
29.
C. P. Lee, A. V. Anilkumar, and T. G. Wang, “The Balancing of Thermocapillary Flow in a Floating Zone by Ripple-driven Streaming,” 50th Annual Meeting of the Division of Fluid Dynamics of the American Physical Society, San Francisco, CA, 23–25 November 1997 (unpublished).
30.
E. Trinh (of Jet Propulsion Laboratory, private communication).
31.
L. D. Landau and E. M. Lifshits, Fluid Mechanics (Pergamon, New York, 1959).
32.
C. E.
Chang
and
W. R.
Wilcox
, “
Analysis of surface tension driven flow in floating zone melting
,”
Int. J. Heat Mass Transf.
19
,
355
(
1976
).
33.
P. A.
Clark
and
W. R.
Wilcox
, “
Influence of gravity on thermocapillary convection in floating zone melting of silicon
,”
J. Cryst. Growth
50
,
461
(
1980
).
34.
Y.
Zhang
and
J. I. D.
Alexander
, “
Sensitivity of liquid bridges subject to axial residual acceleration
,”
Phys. Fluids A
2
,
1966
(
1990
).
35.
M. J.
Marr-Lyon
,
D. B.
Thiessen
, and
P. L.
Marston
, “
Active acoustic stabilization of capillary bridges significantly beyond the Rayleigh limit: Experimental confirmation
,”
J. Acoust. Soc. Am.
99
,
2540
(
1996
).
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