Magnetizing force was applied for natural convection of air in a shallow cylindrical enclosure heated from below and cooled from above. The cylinder measured 45 mm in diameter and 14.8 mm in height. The convection enclosure was located 66 mm above or below the coil center in the bore of a super-conducting magnet. The average Nusselt numbers were enhanced about twice at the location +66 mm above the coil center under 3.40 Tesla and decreased to Nu=1.121.28 at the location −66 mm below the coil center for the Rayleigh number from 3520 to 6980. These two locations were selected as the most effective positions for application of the magnetizing force in this super-conducting magnet. A model equation for magnetizing force was derived and numerically computed for Pr=0.7 and Ra=2100 and 7000. One turn coil was presumed as a model of thousand turns real superconductor. The magnetic strength is represented by a new parameter γ and varied from 2345 to 9124. By adjusting the location of the enclosure in the bore of the super-conducting magnet, the average Nusselt number of 1.14 at Ra=2100 varied from 1.8 to 1.0001 depending on the magnetic strength, and that of 2.02 at Ra=7000 varied from 2.6 to 1.0003. These data are plotted versus magnetic Rayleigh number Ram=RaγBz2/Z+1R=0,Z=0.5 at the center of the enclosure and agreed well with Silveston’s data for a classical nonmagnetic field.

1.
Faraday
,
M.
,
1847
, “
On the Diamagnetic Conditions of Flame and Gases
,”
Philos. Mag.
,
31
(
210
), pp.
401
421
.
2.
Pauling
,
L.
,
Wood
,
R. E.
, and
Sturdivant
,
J. H.
,
1946
, “
An Instrument for Determining the Partial Pressure of Oxygen in a Gas
,”
J. Am. Chem. Soc.
,
68
, pp.
795
798
.
3.
Braithwaite
,
D.
,
Beaugnon
,
E.
, and
Tournier
,
R.
,
1991
, “
Magnetically Controlled Convection in a Paramagnetic Fluid
,”
Nature (London)
,
354
, pp.
134
136
.
4.
Silveston
,
P. L.
,
1958
, “
Wa¨medurchgang in waagerechten Flussigkeitsschichten
,”
Part 1, Forsch, Ing. Wes.
,
24
, pp.
29
32
and pp. 59–69.
5.
Wakayama
,
N. I.
,
1991
, “
Behavior of Flow Under Gradient Magnetic Fields
,”
J. Appl. Phys.
,
69
(
4
), pp.
2734
2736
.
6.
Wakayama
,
N. I.
,
1991
, “
Effect of a Decreasing Magnetic Field on the Flow of Nitrogen Gas
,”
Chem. Phys. Lett.
,
185
(
5-6
), pp.
449
451
.
7.
Wakayama
,
N. I.
,
1993
, “
Magnetic Promotion of Combustion in Diffusion Flames
,”
Combust. Flame
,
93
(
3
), pp.
207
214
.
8.
Wakayama
,
N. I.
,
Ito
,
H.
,
Kuroda
,
Y.
,
Fujita
,
O.
, and
Ito
,
K.
,
1996
, “
Magnetic Support of Combustion in Diffusion Flames Under Micro Gravity
,”
Combust. Flame
,
107
(
1-2
), pp.
187
192
.
9.
Bai
,
B.
,
Yabe
,
A.
,
Qi
,
J.
, and
Wakayama
,
N. I.
,
1999
, “
Quantitative Analysis of Air Convection Caused by Magnetic-Fluid Coupling
,”
AIAA J.
,
37
(
12
), pp.
1538
1543
.
10.
Ikezoe
,
Y.
,
Hirota
,
N.
,
Nakagawa
,
J.
, and
Kitazawa
,
K.
,
1998
, “
Making Water Levitate
,”
Nature (London)
,
393
, pp.
749
750
.
11.
Ikezoe
,
Y.
,
Hirota
,
N.
,
Sakihama
,
T.
,
Mogi
,
K.
,
Uetake
,
H.
,
Homma
,
T.
,
Nakagawa
,
J.
,
Sugawara
,
H.
, and
Kitazawa
,
K.
,
1998
, “
Acceleration Effect on the Rate of Dissolution of Oxygen in a Magnetic Field,” (Japanese
),
Journal of Japan Institute of Applied Magnetics
,
22
(
4-2
), pp.
821
824
.
12.
Uetake
,
H.
,
Nakagawa
,
J.
,
Hirota
,
N.
, and
Kitazawa
,
K.
,
1999
, “
Nonmechanical Magnetothermal Wind Blower by a Superconducting Magnet
,”
J. Appl. Phys.
,
85
(
8
), pp.
5735
5737
.
13.
Nakagawa
,
J.
,
Hirota
,
N.
,
Kitazawa
,
K.
, and
Shoda
,
M.
,
1999
, “
Magnetic Field Enhancement of Water Vaporization
,”
J. Appl. Phys.
,
86
(
5
), pp.
2923
2925
.
14.
Ozoe
,
H.
, and
Churchill
,
S. W.
,
1973
, “
Hydrodynamic Stability and Natural Convection in Newtonian and Non-Newtonian Fluids Heated From Below
,”
AIChE Symp. Ser.
,
69
(
131
), pp.
126
133
.
15.
Tagawa
,
T.
,
Shigemitsu
,
R.
, and
Ozoe
,
H.
,
2002
, “
Magnetizing Force Modeled and Numerically Solved for Natural Convection of Air in a Cubic Enclosure: Effect of the Direction of the Magnetic Field
,”
Int. J. Heat Mass Transf.
,
45
, pp.
267
277
.
16.
Kaneda
,
M.
,
Tagawa
,
T.
, and
Ozoe
,
H.
,
2002
, “
Convection Induced by a Cusp-Shaped Magnetic Field for Air in a Cube Heated From Above and Cooled From Below
,”
ASME J. Heat Transfer
,
124
, pp.
17
25
.
17.
Hellums
,
J. D.
, and
Churchill
,
S. W.
,
1964
, “
Simplification of the Mathematical Description of Boundary and Initial Value Problem
,”
AIChE J.
,
10
, pp.
110
114
.
18.
Hirt, C. W., Nichols, B. D., and Romero, N. C., 1975, “A Numerical Solution Algorithm for Transient Fluid Flows,” Los Alamos Scientific Laboratory, LA-5852.
19.
Yamanaka
,
Y.
,
Kakimoto
,
K.
,
Ozoe
,
H.
, and
Churchill
,
S. W.
,
1998
, “
Rayleigh-Benard Oscillatory Natural Convection of Liquid Gallium Heated From Below
,”
Chem. Eng. J.
,
71
(
3
), pp.
201
206
.
20.
Hatanaka, M., Tagawa, T., and Ozoe, H., 2000, “Numerical Computation of Oscillatory Rayleigh-Benard Natural Convection of Gallium in a Rectangular Region With Aspect Ratios Equal to Five,” Proc. of Symposium on Energy Engineering in the 21st century (SEE 2000), Hong Kong, 1, pp. 288–294.
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