-
1
-
-
4043104154
-
-
(Springer Science & Business Media, New York)
-
P.-G. De Gennes, F. Brochard-Wyart, and D. Quéré, Capillarity and Wetting Phenomena: Drops, Bubbles, Pearls, Waves (Springer Science & Business Media, New York, 2013).
-
(2013)
Capillarity and Wetting Phenomena: Drops, Bubbles, Pearls, Waves
-
-
De Gennes, P.-G.1
Brochard-Wyart, F.2
Quéré, D.3
-
3
-
-
84923322076
-
-
P. Huber, J. Phys.: Condens. Matter 27, 103102 (2015). JCOMEL 0953-8984 10.1088/0953-8984/27/10/103102
-
(2015)
J. Phys.: Condens. Matter
, vol.27
, pp. 103102
-
-
Huber, P.1
-
4
-
-
34347098155
-
-
R. Lucas, Kolloid-Z. 23, 15 (1918). CPMSB6 0303-402X 10.1007/BF01461107
-
(1918)
Kolloid-Z.
, vol.23
, pp. 15
-
-
Lucas, R.1
-
5
-
-
34548193292
-
-
E. W. Washburn, Phys. Rev. 17, 273 (1921). PHRVAO 0031-899X 10.1103/PhysRev.17.273
-
(1921)
Phys. Rev.
, vol.17
, pp. 273
-
-
Washburn, E.W.1
-
9
-
-
79051470231
-
-
F. Caupin, M. W. Cole, S. Balibar, and J. Treiner, Europhysics Lett. 82, 56004 (2008). EULEEJ 0295-5075 10.1209/0295-5075/82/56004
-
(2008)
Europhysics Lett.
, vol.82
, pp. 56004
-
-
Caupin, F.1
Cole, M.W.2
Balibar, S.3
Treiner, J.4
-
11
-
-
67650114634
-
-
S. Gruener, T. Hofmann, D. Wallacher, A. V. Kityk, and P. Huber, Phys. Rev. E 79, 067301 (2009). PLEEE8 1539-3755 10.1103/PhysRevE.79.067301
-
(2009)
Phys. Rev. e
, vol.79
, pp. 067301
-
-
Gruener, S.1
Hofmann, T.2
Wallacher, D.3
Kityk, A.V.4
Huber, P.5
-
12
-
-
84930684557
-
-
E. Oyarzua, J. H. Walther, A. Mejía, and H. A. Zambrano, Phys. Chem. Chem. Phys. 17, 14731 (2015). PPCPFQ 1463-9076 10.1039/C5CP01862E
-
(2015)
Phys. Chem. Chem. Phys.
, vol.17
, pp. 14731
-
-
Oyarzua, E.1
Walther, J.H.2
Mejía, A.3
Zambrano, H.A.4
-
19
-
-
84928790628
-
-
K. Falk, B. Coasne, R. Pellenq, F.-J. Ulm, and L. Bocquet, Nat. Commun. 6, 6949 (2015). 2041-1723 10.1038/ncomms7949
-
(2015)
Nat. Commun.
, vol.6
, pp. 6949
-
-
Falk, K.1
Coasne, B.2
Pellenq, R.3
Ulm, F.-J.4
Bocquet, L.5
-
21
-
-
34147162778
-
-
R. C. Tolman, J. Chem. Phys. 17, 333 (1949). JCPSA6 0021-9606 10.1063/1.1747247
-
(1949)
J. Chem. Phys.
, vol.17
, pp. 333
-
-
Tolman, R.C.1
-
25
-
-
77949413206
-
-
T. Hofmann, M. Tasinkevych, A. Checco, E. Dobisz, S. Dietrich, and B. M. Ocko, Phys. Rev. Lett. 104, 106102 (2010). PRLTAO 0031-9007 10.1103/PhysRevLett.104.106102
-
(2010)
Phys. Rev. Lett.
, vol.104
, pp. 106102
-
-
Hofmann, T.1
Tasinkevych, M.2
Checco, A.3
Dobisz, E.4
Dietrich, S.5
Ocko, B.M.6
-
26
-
-
84870348688
-
-
L. Guillemot, T. Biben, A. Galarneau, G. Vigier, and E. Charlaix, Proc. Natl. Acad. Sci. USA 109, 19557 (2012). PNASA6 0027-8424 10.1073/pnas.1207658109
-
(2012)
Proc. Natl. Acad. Sci. USA
, vol.109
, pp. 19557
-
-
Guillemot, L.1
Biben, T.2
Galarneau, A.3
Vigier, G.4
Charlaix, E.5
-
27
-
-
34547295815
-
-
S. Lichter, A. Martini, R. Q. Snurr, and Q. Wang, Phys. Rev. Lett. 98, 226001 (2007). PRLTAO 0031-9007 10.1103/PhysRevLett.98.226001
-
(2007)
Phys. Rev. Lett.
, vol.98
, pp. 226001
-
-
Lichter, S.1
Martini, A.2
Snurr, R.Q.3
Wang, Q.4
-
29
-
-
84874877863
-
-
S. K. Kannam, B. D. Todd, J. S. Hansen, and P. J. Daivis, J. Chem. Phys. 138, 094701 (2013). JCPSA6 0021-9606 10.1063/1.4793396
-
(2013)
J. Chem. Phys.
, vol.138
, pp. 094701
-
-
Kannam, S.K.1
Todd, B.D.2
Hansen, J.S.3
Daivis, P.J.4
-
31
-
-
83455177058
-
-
L. Joly, J. Chem. Phys. 135, 214705 (2011). JCPSA6 0021-9606 10.1063/1.3664622
-
(2011)
J. Chem. Phys.
, vol.135
, pp. 214705
-
-
Joly, L.1
-
33
-
-
84885351477
-
-
S. Gravelle, L. Joly, F. Detcheverry, C. Ybert, C. Cottin-Bizonne, and L. Bocquet, Proc. Natl. Acad. Sci. USA 110, 16367 (2013). PNASA6 0027-8424 10.1073/pnas.1306447110
-
(2013)
Proc. Natl. Acad. Sci. USA
, vol.110
, pp. 16367
-
-
Gravelle, S.1
Joly, L.2
Detcheverry, F.3
Ybert, C.4
Cottin-Bizonne, C.5
Bocquet, L.6
-
34
-
-
84908005718
-
-
S. Gravelle, L. Joly, C. Ybert, and L. Bocquet, J. Chem. Phys. 141, 18C526 (2014). JCPSA6 0021-9606 10.1063/1.4897253
-
(2014)
J. Chem. Phys.
, vol.141
, pp. 18C526
-
-
Gravelle, S.1
Joly, L.2
Ybert, C.3
Bocquet, L.4
-
35
-
-
84962343401
-
-
Note, however, that structuring effects can be accounted for in continuum descriptions, e.g., in the density functional theory framework [22,25]
-
Note, however, that structuring effects can be accounted for in continuum descriptions, e.g., in the density functional theory framework [22,25].
-
-
-
-
36
-
-
0002467378
-
-
S. Plimpton, J. Comput. Phys. 117, 1 (1995). JCTPAH 0021-9991 10.1006/jcph.1995.1039
-
(1995)
J. Comput. Phys.
, vol.117
, pp. 1
-
-
Plimpton, S.1
-
38
-
-
0029011701
-
-
W. D. Cornell, P. Cieplak, C. I. Bayly, I. R. Gould, K. M. Merz, D. M. Ferguson, D. C. Spellmeyer, T. Fox, J. W. Caldwell, and P. A. Kollman, J. Am. Chem. Soc. 117, 5179 (1995). JACSAT 0002-7863 10.1021/ja00124a002
-
(1995)
J. Am. Chem. Soc.
, vol.117
, pp. 5179
-
-
Cornell, W.D.1
Cieplak, P.2
Bayly, C.I.3
Gould, I.R.4
Merz, K.M.5
Ferguson, D.M.6
Spellmeyer, D.C.7
Fox, T.8
Caldwell, J.W.9
Kollman, P.A.10
-
39
-
-
84962343406
-
-
Simulations with flexible and fixed walls were shown to give similar results for the statics and friction of confined liquids in previous work [56-58]
-
Simulations with flexible and fixed walls were shown to give similar results for the statics and friction of confined liquids in previous work [56-58].
-
-
-
-
40
-
-
33750587438
-
-
H. J. C. Berendsen, J. P. M. Postma, W. F. van Gunsteren, A. DiNola, and J. R. Haak, J. Chem. Phys. 81, 3684 (1984). JCPSA6 0021-9606 10.1063/1.448118
-
(1984)
J. Chem. Phys.
, vol.81
, pp. 3684
-
-
Berendsen, H.J.C.1
Postma, J.P.M.2
Van Gunsteren, W.F.3
DiNola, A.4
Haak, J.R.5
-
42
-
-
84956680895
-
-
N. Giovambattista, A. B. Almeida, A. M. Alencar, and S. V. Buldyrev, J. Phys. Chem. C 120, 1597 (2016). 1932-7447 10.1021/acs.jpcc.5b10377
-
(2016)
J. Phys. Chem. C
, vol.120
, pp. 1597
-
-
Giovambattista, N.1
Almeida, A.B.2
Alencar, A.M.3
Buldyrev, S.V.4
-
44
-
-
84962343422
-
-
Line tension should play no role in the cylindrical and slit geometries we considered, because a change in the contact angle does not modify the length of the contact line
-
Line tension should play no role in the cylindrical and slit geometries we considered, because a change in the contact angle does not modify the length of the contact line.
-
-
-
-
45
-
-
84962372181
-
-
In practice, no spontaneous filling is observed and the initial condition is modified by preparing the tube in the already filled configuration. From there, the measured evolution corresponds to a capillary emptying with the water being ejected from the nanotube
-
In practice, no spontaneous filling is observed and the initial condition is modified by preparing the tube in the already filled configuration. From there, the measured evolution corresponds to a capillary emptying with the water being ejected from the nanotube.
-
-
-
-
46
-
-
84962343428
-
-
For hydrophobic tubes, water is forced to enter the channel by applying a pressure to the piston, until the tube is half-filled
-
For hydrophobic tubes, water is forced to enter the channel by applying a pressure to the piston, until the tube is half-filled.
-
-
-
-
48
-
-
39649089584
-
-
B. Corry, J. Phys. Chem. B 112, 1427 (2008). JPCBFK 1520-6106 10.1021/jp709845u
-
(2008)
J. Phys. Chem. B
, vol.112
, pp. 1427
-
-
Corry, B.1
-
54
-
-
79955580208
-
-
X. Qin, Q. Yuan, Y. Zhao, S. Xie, and Z. Liu, Nano Lett. 11, 2173 (2011). NALEFD 1530-6984 10.1021/nl200843g
-
(2011)
Nano Lett.
, vol.11
, pp. 2173
-
-
Qin, X.1
Yuan, Q.2
Zhao, Y.3
Xie, S.4
Liu, Z.5
-
58
-
-
0037434746
-
-
T. Werder, J. H. Walther, R. L. Jaffe, T. Halicioglu, and P. Koumoutsakos, J. Phys. Chem. B 107, 1345 (2003). JPCBFK 1520-6106 10.1021/jp0268112
-
(2003)
J. Phys. Chem. B
, vol.107
, pp. 1345
-
-
Werder, T.1
Walther, J.H.2
Jaffe, R.L.3
Halicioglu, T.4
Koumoutsakos, P.5
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