-
2
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-
0034690061
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-
J.J. Niemela, L. Skrbek, K.R. Sreenivasan, and R.J. Donnelly, Nature (London) 404, 837 (2000).
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(2000)
Nature (London)
, vol.404
, pp. 837
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Niemela, J.J.1
Skrbek, L.2
Sreenivasan, K.R.3
Donnelly, R.J.4
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9
-
-
85036289523
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-
These are (Formula presented) pure solvents purchased from Acros Organics, Ltd
-
These are (Formula presented) pure solvents purchased from Acros Organics, Ltd.
-
-
-
-
11
-
-
85036242829
-
-
C.L. Yaws, Chemical Properties Handbook (McGraw-Hill, New York, 1999)
-
C.L. Yaws, Chemical Properties Handbook (McGraw-Hill, New York, 1999).
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-
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15
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-
85036352312
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-
We achieve the density match between the glass spheres and the liquid by first spinning the suspension in a centrifuge and then drawing out the middle part of the suspension with a syringe needle after the liquid has settled for a long time
-
We achieve the density match between the glass spheres and the liquid by first spinning the suspension in a centrifuge and then drawing out the middle part of the suspension with a syringe needle after the liquid has settled for a long time.
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-
-
-
16
-
-
85036406443
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-
Because the large refractive index of the fluid (compared to water) causes bending of the laser beams, we are not able to position them very close to the surface of the plate where there is a large refractive index gradient. Thus we do not know whether the velocity profile in Fig. 11 will become linear inside the thermal layer (Formula presented) for the present one, which is also the lowest point measured)
-
Because the large refractive index of the fluid (compared to water) causes bending of the laser beams, we are not able to position them very close to the surface of the plate where there is a large refractive index gradient. Thus we do not know whether the velocity profile in Fig. 11 will become linear inside the thermal layer (Formula presented) for the present one, which is also the lowest point measured).
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-
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-
20
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0033602414
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J.A. Glazier, T. Segawa, A. Naert, and M. Sano, Nature (London) 398, 307 (1999).
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(1999)
Nature (London)
, vol.398
, pp. 307
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Glazier, J.A.1
Segawa, T.2
Naert, A.3
Sano, M.4
-
24
-
-
85036259387
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-
The flow at this Pr is very slow, so even with very long averages the data still show large scatter
-
The flow at this Pr is very slow, so even with very long averages the data still show large scatter.
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-
-
-
31
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-
85036167090
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-
The highest shear Reynolds number based on the boundary layer thickness, (Formula presented), reached in the experiment is about 200, whereas the critical value for instability is about 420 [see, for example, L.D. Landau and E.M. Lifshitz, Fluid Mechanics (Pergamon Press, Oxford, 1987)]
-
The highest shear Reynolds number based on the boundary layer thickness, (Formula presented), reached in the experiment is about 200, whereas the critical value for instability is about 420 [see, for example, L.D. Landau and E.M. Lifshitz, Fluid Mechanics (Pergamon Press, Oxford, 1987)].
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33
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0024698819
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B. Castaing, G. Gunaratne, F. Heslot, L.P. Kadanoff, A. Libchaber, S. Thomae, X.-Z. Wu, S. Zaleski, and G. Zanetti, J. Fluid Mech. 204, 1 (1989).
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(1989)
J. Fluid Mech.
, vol.204
, pp. 1
-
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Castaing, B.1
Gunaratne, G.2
Heslot, F.3
Kadanoff, L.P.4
Libchaber, A.5
Thomae, S.6
Wu, X.-Z.7
Zaleski, S.8
Zanetti, G.9
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36
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0035337311
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X. Chavanne, F. Chillà, B. Chabaud, B. Castaing, and B. Hébral, Phys. Fluids 13, 1300 (2001).
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(2001)
Phys. Fluids
, vol.13
, pp. 1300
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Chavanne, X.1
Chillà, F.2
Chabaud, B.3
Castaing, B.4
Hébral, B.5
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