-
1
-
-
84861670287
-
-
1st ed., edited by M. Rubinstein and R. Colby (Oxford University Press, Inc., New York).
-
Polymer Phyiscs, 1st ed., edited by, M. Rubinstein, and, R. Colby, (Oxford University Press, Inc., New York, 2003).
-
(2003)
Polymer Phyiscs
-
-
-
2
-
-
0033898191
-
-
10.1021/ma991983r
-
H. Tao and T. Lodge, Macromolecules 33, 1747 (2000). 10.1021/ma991983r
-
(2000)
Macromolecules
, vol.33
, pp. 1747
-
-
Tao, H.1
Lodge, T.2
-
6
-
-
0034909360
-
-
10.1016/S0006-3495(01)75737-2
-
R. D. Groot and K. L. Rabone, Biophys. J. 81, 725 (2001). 10.1016/S0006-3495(01)75737-2
-
(2001)
Biophys. J.
, vol.81
, pp. 725
-
-
Groot, R.D.1
Rabone, K.L.2
-
7
-
-
0034635240
-
-
10.1209/epl/i2000-00183-2
-
N. A. Spenley, Europhys. Lett. 49, 534 (2000). 10.1209/epl/i2000-00183-2
-
(2000)
Europhys. Lett.
, vol.49
, pp. 534
-
-
Spenley, N.A.1
-
14
-
-
77956841485
-
-
10.1122/1.3473925
-
N. Hoda and R. G. Larson, J. Rheol. 54, 1061 (2010). 10.1122/1.3473925
-
(2010)
J. Rheol.
, vol.54
, pp. 1061
-
-
Hoda, N.1
Larson, R.G.2
-
15
-
-
0003423425
-
-
2nd ed., edited by R. Bird, C. Curtiss, R. Armstrong, and O. Hassager (Wiley, New York).
-
Dynamics of Polymeric Liquids, Volume 2: Kinetic Theory, 2nd ed., edited by, R. Bird, C. Curtiss, R. Armstrong, and, O. Hassager, (Wiley, New York, 1987).
-
(1987)
Dynamics of Polymeric Liquids, Volume 2: Kinetic Theory
-
-
-
17
-
-
70349898767
-
-
10.1021/ma9011329
-
F. Lahmar, C. Tzoumanekas, D. N. Theodorou, and B. Rousseau, Macromolecules 42, 7485 (2009). 10.1021/ma9011329
-
(2009)
Macromolecules
, vol.42
, pp. 7485
-
-
Lahmar, F.1
Tzoumanekas, C.2
Theodorou, D.N.3
Rousseau, B.4
-
18
-
-
70349897834
-
-
10.1021/ma901131c
-
C. Tzoumanekas, F. Lahmar, B. Rousseau, and D. N. Theodorou, Macromolecules 42, 7474 (2009). 10.1021/ma901131c
-
(2009)
Macromolecules
, vol.42
, pp. 7474
-
-
Tzoumanekas, C.1
Lahmar, F.2
Rousseau, B.3
Theodorou, D.N.4
-
19
-
-
84861698152
-
-
BT 1.06), which persisted even when the timestewas reduced to δt 0.001 τ. We speculate that the marginal performance of the DPD thermostat for SRP occurs due to the choice of chain parameters and the additional energy introduced by the segmental repulsive forces.
-
BT 1.06), which persisted even when the timestep was reduced to δt 0.001 τ. We speculate that the marginal performance of the DPD thermostat for SRP occurs due to the choice of chain parameters and the additional energy introduced by the segmental repulsive forces.
-
-
-
-
21
-
-
0002467378
-
-
10.1006/jcph.1995.1039
-
S. J. Plimpton, J. Comput. Phys. 117, 1 (1995). 10.1006/jcph.1995.1039
-
(1995)
J. Comput. Phys.
, vol.117
, pp. 1
-
-
Plimpton, S.J.1
-
22
-
-
0842330642
-
-
10.1063/1.1628670
-
R. Auhl, G. Grest, K. Kremer, and S. Plimpton, J. Chem. Phys. 119, 12718 (2003). 10.1063/1.1628670
-
(2003)
J. Chem. Phys.
, vol.119
, pp. 12718
-
-
Auhl, R.1
Grest, G.2
Kremer, K.3
Plimpton, S.4
-
23
-
-
0003631032
-
-
1st ed., edited by W. Mattice and U. Suter (John Wiley and Sons, New York).
-
Conformational Theory of Large Molecules the Rotational Isomeric State Model in Macromolecular Systems, 1st ed., edited by, W. Mattice, and, U. Suter, (John Wiley and Sons, New York, 1994).
-
(1994)
Conformational Theory of Large Molecules the Rotational Isomeric State Model in Macromolecular Systems
-
-
-
27
-
-
84861701195
-
-
edited by R. Tanner and K. Walters (Elsevier Science, Amsterdam).
-
Rheology, An Historical Prospective, edited by, R. Tanner, and, K. Walters, (Elsevier Science, Amsterdam, 1998).
-
(1998)
Rheology, An Historical Prospective
-
-
-
29
-
-
0003399724
-
-
2nd ed., edited by D. Frenkel and B. Smit (Academic Press, New York).
-
Understanding Molecular Simulation, 2nd ed., edited by, D. Frenkel, and, B. Smit, (Academic Press, New York, 2002).
-
(2002)
Understanding Molecular Simulation
-
-
|