-
1
-
-
62849123215
-
-
0301-9322, 10.1016/j.ijmultiphaseflow.2009.02.004
-
H. Kim, G. DeWitt, T. McKrell, J. Buongiorno, and L. -W. Hu, Int. J. Multiphase Flow 0301-9322 35, 427 (2009). 10.1016/j.ijmultiphaseflow.2009.02.004
-
(2009)
Int. J. Multiphase Flow
, vol.35
, pp. 427
-
-
Kim, H.1
Dewitt, G.2
McKrell, T.3
Buongiorno, J.4
Hu, L.-W.5
-
2
-
-
74549192205
-
-
0017-9310, 10.1016/j.ijheatmasstransfer.2009.11.029
-
H. Kim, J. Buongiorno, L. -W. Hu, and T. McKrell, Int. J. Heat Mass Transfer 0017-9310 53, 1542 (2010). 10.1016/j.ijheatmasstransfer.2009.11.029
-
(2010)
Int. J. Heat Mass Transfer
, vol.53
, pp. 1542
-
-
Kim, H.1
Buongiorno, J.2
Hu, L.-W.3
McKrell, T.4
-
5
-
-
33750494721
-
All-nanoparticle thin-film coatings
-
DOI 10.1021/nl061776m
-
D. Lee, M. F. Rubner, and R. E. Cohen, Nano Lett. 1530-6984 6, 2305 (2006). 10.1021/nl061776m (Pubitemid 44663823)
-
(2006)
Nano Letters
, vol.6
, Issue.10
, pp. 2305-2312
-
-
Lee, D.1
Rubner, M.F.2
Cohen, R.E.3
-
6
-
-
85021792427
-
-
0019-7866, 10.1021/ie50320a024
-
R. N. Wenzel, Ind. Eng. Chem. 0019-7866 28, 988 (1936). 10.1021/ie50320a024
-
(1936)
Ind. Eng. Chem.
, vol.28
, pp. 988
-
-
Wenzel, R.N.1
-
7
-
-
0024103716
-
DYNAMICS AND LEIDENFROST TEMPERATURE OF DROPS IMPACTING ON A HOT SURFACE AT SMALL ANGLES
-
DOI 10.1016/0894-1777(88)90016-7
-
S. C. Yao and K. Y. Cai, Exp. Therm. Fluid Sci. 0894-1777 1, 363 (1988). 10.1016/0894-1777(88)90016-7 (Pubitemid 18665129)
-
(1988)
Experimental Thermal and Fluid Science
, vol.1
, Issue.4
, pp. 363-371
-
-
Yao Shi-Chune1
Cai Kang Yuan2
-
8
-
-
79952083740
-
-
The reported value of LFP is the nominal temperature of the test surface. Obviously, the local temperature at which the liquid-solid contact occurs must be below the critical point
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The reported value of LFP is the nominal temperature of the test surface. Obviously, the local temperature at which the liquid-solid contact occurs must be below the critical point.
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-
-
-
10
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-
0037493526
-
Leidenfrost drops
-
DOI 10.1063/1.1572161
-
A. -L. Biance, C. Clanet, and D. Quere, Phys. Fluids 1070-6631 15, 1632 (2003). 10.1063/1.1572161 (Pubitemid 36785210)
-
(2003)
Physics of Fluids
, vol.15
, Issue.6
, pp. 1632-1637
-
-
Biance, A.-L.1
Clanet, C.2
Quere, D.3
-
11
-
-
0036794222
-
A cavity activation and bubble growth model of the Leidenfrost point
-
DOI 10.1115/1.1470487
-
J. D. Bernardin and I. Mudawar, J. Heat Transfer 0022-1481 124, 864 (2002). 10.1115/1.1470487 (Pubitemid 35181754)
-
(2002)
Journal of Heat Transfer
, vol.124
, Issue.5
, pp. 864-874
-
-
Bernardin, J.D.1
Mudawar, I.2
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12
-
-
79952079681
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Note that these values of nucleation superheat are much higher than those normally encountered on engineering surfaces where microcavities are present
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Note that these values of nucleation superheat are much higher than those normally encountered on engineering surfaces where microcavities are present.
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13
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79952084398
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The calculated value of the heterogeneous nucleation temperature at d=1 nm is higher than the homogeneous nucleation temperature (∼300 °C for water at atmospheric pressure) because the size of the vapor embryos responsible for homogeneous nucleation is of the order of a few nanometers. Therefore, the fluid nucleates homogeneously before it does so heterogeneously
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The calculated value of the heterogeneous nucleation temperature at d=1 nm is higher than the homogeneous nucleation temperature (∼300 °C for water at atmospheric pressure) because the size of the vapor embryos responsible for homogeneous nucleation is of the order of a few nanometers. Therefore, the fluid nucleates homogeneously before it does so heterogeneously.
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