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@article{ISI:000207079300006, |
13 |
Abstract = {Non-equilibrium Molecular Dynamics Simulation |
14 |
methods have been used to study the ability of |
15 |
Embedded Atom Method models of the metals copper and |
16 |
gold to reproduce the equilibrium and |
17 |
non-equilibrium behavior of metals at a stationary |
18 |
and at a moving solid/liquid interface. The |
19 |
equilibrium solid/vapor interface was shown to |
20 |
display a simple termination of the bulk until the |
21 |
temperature of the solid reaches approximate to 90\% |
22 |
of the bulk melting point. At and above such |
23 |
temperatures the systems exhibit a surface |
24 |
disodering known as surface melting. Non-equilibrium |
25 |
simulations emulating the action of a picosecond |
26 |
laser on the metal were performed to determine the |
27 |
regrowth velocity. For copper, the action of a 20 ps |
28 |
laser with an absorbed energy of 2-5 mJ/cm(2) |
29 |
produced a regrowth velocity of 83-100 m/s, in |
30 |
reasonable agreement with the value obtained by |
31 |
experiment (>60 m/s). For gold, similar conditions |
32 |
produced a slower regrowth velocity of 63 m/s at an |
33 |
absorbed energy of 5 mJ/cm(2). This is almost a |
34 |
factor of two too low in comparison to experiment |
35 |
(>100 m/s). The regrowth velocities of the metals |
36 |
seems unexpectedly close to experiment considering |
37 |
that the free-electron contribution is ignored in |
38 |
the Embeeded Atom Method models used.}, |
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Address = {4 PARK SQUARE, MILTON PARK, ABINGDON OX14 4RN, |
40 |
OXON, ENGLAND}, |
41 |
Affiliation = {Clancy, P (Reprint Author), Cornell Univ, Sch Chem |
42 |
Engn, Ithaca, NY 14853 USA. {[}Richardson, Clifton |
43 |
F.; Clancy, Paulette] Cornell Univ, Sch Chem Engn, |
44 |
Ithaca, NY 14853 USA.}, |
45 |
Author = {Richardson, Clifton F. and Clancy, Paulette}, |
46 |
Date-Added = {2010-04-07 11:24:36 -0400}, |
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Date-Modified ={2010-04-07 11:24:36 -0400}, |
48 |
Doc-Delivery-Number ={V04SY}, |
49 |
Issn = {0892-7022}, |
50 |
Journal = {MOLECULAR SIMULATION}, |
51 |
Journal-Iso = {Mol. Simul.}, |
52 |
Keywords = {Non-equilibrium computer simulation; molecular |
53 |
dynamics; crystal growth; Embedded Atom Method |
54 |
models of metals}, |
55 |
Language = {English}, |
56 |
Number = {5-6}, |
57 |
Number-Of-Cited-References ={36}, |
58 |
Pages = {335-355}, |
59 |
Publisher = {TAYLOR \& FRANCIS LTD}, |
60 |
Subject-Category ={Chemistry, Physical; Physics, Atomic, Molecular |
61 |
\& Chemical}, |
62 |
Times-Cited = {7}, |
63 |
Title = {PICOSECOND LASER PROCESSING OF COPPER AND GOLD: A |
64 |
COMPUTER SIMULATION STUDY}, |
65 |
Type = {Article}, |
66 |
Unique-Id = {ISI:000207079300006}, |
67 |
Volume = {7}, |
68 |
Year = {1991} |
69 |
} |
70 |
|
71 |
@article{ISI:000167766600035, |
72 |
Abstract = {Molecular dynamics simulations are used to |
73 |
investigate the separation of water films adjacent |
74 |
to a hot metal surface. The simulations clearly show |
75 |
that the water layers nearest the surface overheat |
76 |
and undergo explosive boiling. For thick films, the |
77 |
expansion of the vaporized molecules near the |
78 |
surface forces the outer water layers to move away |
79 |
from the surface. These results are of interest for |
80 |
mass spectrometry of biological molecules, steam |
81 |
cleaning of surfaces, and medical procedures.}, |
82 |
Address = {1155 16TH ST, NW, WASHINGTON, DC 20036 USA}, |
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Affiliation = {Garrison, BJ (Reprint Author), Penn State Univ, |
84 |
Dept Chem, University Pk, PA 16802 USA. Penn State |
85 |
Univ, Dept Chem, University Pk, PA 16802 USA. Penn |
86 |
State Univ, Inst Mat Res, University Pk, PA 16802 |
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USA. Univ Virginia, Dept Mat Sci \& Engn, |
88 |
Charlottesville, VA 22903 USA.}, |
89 |
Author = {Dou, YS and Zhigilei, LV and Winograd, N and |
90 |
Garrison, BJ}, |
91 |
Date-Added = {2010-03-11 15:32:14 -0500}, |
92 |
Date-Modified ={2010-03-11 15:32:14 -0500}, |
93 |
Doc-Delivery-Number ={416ED}, |
94 |
Issn = {1089-5639}, |
95 |
Journal = {J. Phys. Chem. A}, |
96 |
Journal-Iso = {J. Phys. Chem. A}, |
97 |
Keywords-Plus ={MOLECULAR-DYNAMICS SIMULATIONS; ASSISTED |
98 |
LASER-DESORPTION; FROZEN AQUEOUS-SOLUTIONS; |
99 |
COMPUTER-SIMULATION; ORGANIC-SOLIDS; VELOCITY |
100 |
DISTRIBUTIONS; PARTICLE BOMBARDMENT; |
101 |
MASS-SPECTROMETRY; PHASE EXPLOSION; LIQUID WATER}, |
102 |
Language = {English}, |
103 |
Month = {MAR 29}, |
104 |
Number = {12}, |
105 |
Number-Of-Cited-References ={65}, |
106 |
Pages = {2748-2755}, |
107 |
Publisher = {AMER CHEMICAL SOC}, |
108 |
Subject-Category ={Chemistry, Physical; Physics, Atomic, Molecular |
109 |
\& Chemical}, |
110 |
Times-Cited = {66}, |
111 |
Title = {Explosive boiling of water films adjacent to heated |
112 |
surfaces: A microscopic description}, |
113 |
Type = {Article}, |
114 |
Unique-Id = {ISI:000167766600035}, |
115 |
Volume = {105}, |
116 |
Year = {2001} |
117 |
} |
118 |
|
119 |
@article{ISI:000273472300004, |
120 |
Abstract = {The reverse nonequilibrium molecular dynamics |
121 |
(RNEMD) method calculates the shear viscosity of a |
122 |
fluid by imposing a nonphysical exchange of momentum |
123 |
and measuring the resulting shear velocity |
124 |
gradient. In this study we investigate the range of |
125 |
momentum flux values over which RNEMD yields usable |
126 |
(linear) velocity gradients. We find that nonlinear |
127 |
velocity profiles result primarily from gradients in |
128 |
fluid temperature and density. The temperature |
129 |
gradient results from conversion of heat into bulk |
130 |
kinetic energy, which is transformed back into heat |
131 |
elsewhere via viscous heating. An expression is |
132 |
derived to predict the temperature profile resulting |
133 |
from a specified momentum flux for a given fluid and |
134 |
simulation cell. Although primarily bounded above, |
135 |
we also describe milder low-flux limitations. RNEMD |
136 |
results for a Lennard-Jones fluid agree with |
137 |
equilibrium molecular dynamics and conventional |
138 |
nonequilibrium molecular dynamics calculations at |
139 |
low shear, but RNEMD underpredicts viscosity |
140 |
relative to conventional NEMD at high shear.}, |
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Address = {CIRCULATION \& FULFILLMENT DIV, 2 HUNTINGTON |
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QUADRANGLE, STE 1 N O 1, MELVILLE, NY 11747-4501 |
143 |
USA}, |
144 |
Affiliation = {Tenney, CM (Reprint Author), Univ Notre Dame, Dept |
145 |
Chem \& Biomol Engn, 182 Fitzpatrick Hall, Notre |
146 |
Dame, IN 46556 USA. {[}Tenney, Craig M.; Maginn, |
147 |
Edward J.] Univ Notre Dame, Dept Chem \& Biomol |
148 |
Engn, Notre Dame, IN 46556 USA.}, |
149 |
Article-Number ={014103}, |
150 |
Author = {Tenney, Craig M. and Maginn, Edward J.}, |
151 |
Author-Email = {ed@nd.edu}, |
152 |
Date-Added = {2010-03-09 13:08:41 -0500}, |
153 |
Date-Modified ={2010-03-09 13:08:41 -0500}, |
154 |
Doc-Delivery-Number ={542DQ}, |
155 |
Doi = {10.1063/1.3276454}, |
156 |
Funding-Acknowledgement ={U.S. Department of Energy |
157 |
{[}DE-FG36-08G088020]}, |
158 |
Funding-Text = {Support for this work was provided by the |
159 |
U.S. Department of Energy (Grant |
160 |
No. DE-FG36-08G088020)}, |
161 |
Issn = {0021-9606}, |
162 |
Journal = {J. Chem. Phys.}, |
163 |
Journal-Iso = {J. Chem. Phys.}, |
164 |
Keywords = {Lennard-Jones potential; molecular dynamics method; |
165 |
Navier-Stokes equations; viscosity}, |
166 |
Keywords-Plus ={CURRENT AUTOCORRELATION-FUNCTION; IONIC LIQUID; |
167 |
SIMULATIONS; TEMPERATURE}, |
168 |
Language = {English}, |
169 |
Month = {JAN 7}, |
170 |
Number = {1}, |
171 |
Number-Of-Cited-References ={20}, |
172 |
Publisher = {AMER INST PHYSICS}, |
173 |
Subject-Category ={Physics, Atomic, Molecular \& Chemical}, |
174 |
Times-Cited = {0}, |
175 |
Title = {Limitations and recommendations for the calculation |
176 |
of shear viscosity using reverse nonequilibrium |
177 |
molecular dynamics}, |
178 |
Type = {Article}, |
179 |
Unique-Id = {ISI:000273472300004}, |
180 |
Volume = {132}, |
181 |
Year = {2010}, |
182 |
Bdsk-Url-1 = {http://dx.doi.org/10.1063/1.3276454} |
183 |
} |
184 |
|
185 |
@article{Clancy:1992, |
186 |
Abstract = {The regrowth velocity of a crystal from a melt |
187 |
depends on contributions from the thermal |
188 |
conductivity, heat gradient, and latent heat. The |
189 |
relative contributions of these terms to the |
190 |
regrowth velocity of the pure metals copper and gold |
191 |
during liquid-phase epitaxy are evaluated. These |
192 |
results are used to explain how results from |
193 |
previous nonequilibrium molecular-dynamics |
194 |
simulations using classical potentials are able to |
195 |
predict regrowth velocities that are close to the |
196 |
experimental values. Results from equilibrium |
197 |
molecular dynamics showing the nature of the |
198 |
solid-vapor interface of an |
199 |
embedded-atom-method-modeled Cu57Ni43 alloy at a |
200 |
temperature corresponding to 62\% of the melting |
201 |
point are presented. The regrowth of this alloy |
202 |
following a simulation of a laser-processing |
203 |
experiment is also given, with use of nonequilibrium |
204 |
molecular-dynamics techniques. The thermal |
205 |
conductivity and temperature gradient in the |
206 |
simulation of the alloy are compared to those for |
207 |
the pure metals.}, |
208 |
Address = {ONE PHYSICS ELLIPSE, COLLEGE PK, MD 20740-3844 |
209 |
USA}, |
210 |
Affiliation = {CORNELL UNIV,SCH CHEM ENGN,ITHACA,NY 14853.}, |
211 |
Author = {Richardson, C.~F. and Clancy, P}, |
212 |
Date-Added = {2010-01-12 16:17:33 -0500}, |
213 |
Date-Modified ={2010-04-08 17:18:25 -0400}, |
214 |
Doc-Delivery-Number ={HX378}, |
215 |
Issn = {0163-1829}, |
216 |
Journal = {Phys. Rev. B}, |
217 |
Journal-Iso = {Phys. Rev. B}, |
218 |
Keywords-Plus ={SURFACE SEGREGATION; MOLECULAR-DYNAMICS; |
219 |
TRANSITION-METALS; SOLIDIFICATION; GROWTH; CU; NI}, |
220 |
Language = {English}, |
221 |
Month = {JUN 1}, |
222 |
Number = {21}, |
223 |
Number-Of-Cited-References ={24}, |
224 |
Pages = {12260-12268}, |
225 |
Publisher = {AMERICAN PHYSICAL SOC}, |
226 |
Subject-Category ={Physics, Condensed Matter}, |
227 |
Times-Cited = {11}, |
228 |
Title = {CONTRIBUTION OF THERMAL-CONDUCTIVITY TO THE |
229 |
CRYSTAL-REGROWTH VELOCITY OF |
230 |
EMBEDDED-ATOM-METHOD-MODELED METALS AND |
231 |
METAL-ALLOYS}, |
232 |
Type = {Article}, |
233 |
Unique-Id = {ISI:A1992HX37800010}, |
234 |
Volume = {45}, |
235 |
Year = {1992} |
236 |
} |
237 |
|
238 |
@article{ISI:000090151400044, |
239 |
Abstract = {We have applied a new nonequilibrium molecular |
240 |
dynamics (NEMD) method {[}F. Muller-Plathe, |
241 |
J. Chem. Phys. 106, 6082 (1997)] previously applied |
242 |
to monatomic Lennard-Jones fluids in the |
243 |
determination of the thermal conductivity of |
244 |
molecular fluids. The method was modified in order |
245 |
to be applicable to systems with holonomic |
246 |
constraints. Because the method involves imposing a |
247 |
known heat flux it is particularly attractive for |
248 |
systems involving long-range and many-body |
249 |
interactions where calculation of the microscopic |
250 |
heat flux is difficult. The predicted thermal |
251 |
conductivities of liquid n-butane and water using |
252 |
the imposed-flux NEMD method were found to be in a |
253 |
good agreement with previous simulations and |
254 |
experiment. (C) 2000 American Institute of |
255 |
Physics. {[}S0021-9606(00)50841-1].}, |
256 |
Address = {2 HUNTINGTON QUADRANGLE, STE 1NO1, MELVILLE, NY |
257 |
11747-4501 USA}, |
258 |
Affiliation = {Bedrov, D (Reprint Author), Univ Utah, Dept Chem \& |
259 |
Fuels Engn, 122 S Cent Campus Dr,Rm 304, Salt Lake |
260 |
City, UT 84112 USA. Univ Utah, Dept Chem \& Fuels |
261 |
Engn, Salt Lake City, UT 84112 USA. Univ Utah, Dept |
262 |
Mat Sci \& Engn, Salt Lake City, UT 84112 USA.}, |
263 |
Author = {Bedrov, D and Smith, GD}, |
264 |
Date-Added = {2009-11-05 18:21:18 -0500}, |
265 |
Date-Modified ={2009-11-05 18:21:18 -0500}, |
266 |
Doc-Delivery-Number ={369BF}, |
267 |
Issn = {0021-9606}, |
268 |
Journal = {J. Chem. Phys.}, |
269 |
Journal-Iso = {J. Chem. Phys.}, |
270 |
Keywords-Plus ={EFFECTIVE PAIR POTENTIALS; TRANSPORT-PROPERTIES; |
271 |
CANONICAL ENSEMBLE; NORMAL-BUTANE; ALGORITHMS; |
272 |
SHAKE; WATER}, |
273 |
Language = {English}, |
274 |
Month = {NOV 8}, |
275 |
Number = {18}, |
276 |
Number-Of-Cited-References ={26}, |
277 |
Pages = {8080-8084}, |
278 |
Publisher = {AMER INST PHYSICS}, |
279 |
Subject-Category ={Physics, Atomic, Molecular \& Chemical}, |
280 |
Times-Cited = {23}, |
281 |
Title = {Thermal conductivity of molecular fluids from |
282 |
molecular dynamics simulations: Application of a new |
283 |
imposed-flux method}, |
284 |
Type = {Article}, |
285 |
Unique-Id = {ISI:000090151400044}, |
286 |
Volume = {113}, |
287 |
Year = {2000} |
288 |
} |
289 |
|
290 |
@article{ISI:000231042800044, |
291 |
Abstract = {The reverse nonequilibrium molecular dynamics |
292 |
method for thermal conductivities is adapted to the |
293 |
investigation of molecular fluids. The method |
294 |
generates a heat flux through the system by suitably |
295 |
exchanging velocities of particles located in |
296 |
different regions. From the resulting temperature |
297 |
gradient, the thermal conductivity is then |
298 |
calculated. Different variants of the algorithm and |
299 |
their combinations with other system parameters are |
300 |
tested: exchange of atomic velocities versus |
301 |
exchange of molecular center-of-mass velocities, |
302 |
different exchange frequencies, molecular models |
303 |
with bond constraints versus models with flexible |
304 |
bonds, united-atom versus all-atom models, and |
305 |
presence versus absence of a thermostat. To help |
306 |
establish the range of applicability, the algorithm |
307 |
is tested on different models of benzene, |
308 |
cyclohexane, water, and n-hexane. We find that the |
309 |
algorithm is robust and that the calculated thermal |
310 |
conductivities are insensitive to variations in its |
311 |
control parameters. The force field, in contrast, |
312 |
has a major influence on the value of the thermal |
313 |
conductivity. While calculated and experimental |
314 |
thermal conductivities fall into the same order of |
315 |
magnitude, in most cases the calculated values are |
316 |
systematically larger. United-atom force fields seem |
317 |
to do better than all-atom force fields, possibly |
318 |
because they remove high-frequency degrees of |
319 |
freedom from the simulation, which, in nature, are |
320 |
quantum-mechanical oscillators in their ground state |
321 |
and do not contribute to heat conduction.}, |
322 |
Address = {1155 16TH ST, NW, WASHINGTON, DC 20036 USA}, |
323 |
Affiliation = {Zhang, MM (Reprint Author), Int Univ Bremen, POB |
324 |
750 561, D-28725 Bremen, Germany. Int Univ Bremen, |
325 |
D-28725 Bremen, Germany. Banco Cent Brasil, Desup, |
326 |
Diesp, BR-01310922 Sao Paulo, Brazil.}, |
327 |
Author = {Zhang, MM and Lussetti, E and de Souza, LES and |
328 |
M\"{u}ller-Plathe, F}, |
329 |
Date-Added = {2009-11-05 18:17:33 -0500}, |
330 |
Date-Modified ={2009-11-05 18:17:33 -0500}, |
331 |
Doc-Delivery-Number ={952YQ}, |
332 |
Doi = {10.1021/jp0512255}, |
333 |
Issn = {1520-6106}, |
334 |
Journal = {J. Phys. Chem. B}, |
335 |
Journal-Iso = {J. Phys. Chem. B}, |
336 |
Keywords-Plus ={LENNARD-JONES LIQUIDS; TRANSPORT-COEFFICIENTS; |
337 |
SWOLLEN POLYMERS; SHEAR VISCOSITY; MODEL SYSTEMS; |
338 |
SIMULATION; BENZENE; FLUIDS; POTENTIALS; DIFFUSION}, |
339 |
Language = {English}, |
340 |
Month = {AUG 11}, |
341 |
Number = {31}, |
342 |
Number-Of-Cited-References ={42}, |
343 |
Pages = {15060-15067}, |
344 |
Publisher = {AMER CHEMICAL SOC}, |
345 |
Subject-Category ={Chemistry, Physical}, |
346 |
Times-Cited = {17}, |
347 |
Title = {Thermal conductivities of molecular liquids by |
348 |
reverse nonequilibrium molecular dynamics}, |
349 |
Type = {Article}, |
350 |
Unique-Id = {ISI:000231042800044}, |
351 |
Volume = {109}, |
352 |
Year = {2005}, |
353 |
Bdsk-Url-1 = {http://dx.doi.org/10.1021/jp0512255%7D} |
354 |
} |
355 |
|
356 |
@article{ISI:A1997YC32200056, |
357 |
Abstract = {Equilibrium molecular dynamics simulations have |
358 |
been carried out in the microcanonical ensemble at |
359 |
300 and 255 K on the extended simple point charge |
360 |
(SPC/E) model of water {[}Berendsen et al., |
361 |
J. Phys. Chem. 91, 6269 (1987)]. In addition to a |
362 |
number of static and dynamic properties, thermal |
363 |
conductivity lambda has been calculated via |
364 |
Green-Kubo integration of the heat current time |
365 |
correlation functions (CF's) in the atomic and |
366 |
molecular formalism, at wave number k=0. The |
367 |
calculated values (0.67 +/- 0.04 W/mK at 300 K and |
368 |
0.52 +/- 0.03 W/mK at 255 K) are in good agreement |
369 |
with the experimental data (0.61 W/mK at 300 K and |
370 |
0.49 W/mK at 255 K). A negative long-time tail of |
371 |
the heat current CF, more apparent at 255 K, is |
372 |
responsible for the anomalous decrease of lambda |
373 |
with temperature. An analysis of the dynamical modes |
374 |
contributing to lambda has shown that its value is |
375 |
due to two low-frequency exponential-like modes, a |
376 |
faster collisional mode, with positive contribution, |
377 |
and a slower one, which determines the negative |
378 |
long-time tail. A comparison of the molecular and |
379 |
atomic spectra of the heat current CF has suggested |
380 |
that higher-frequency modes should not contribute to |
381 |
lambda in this temperature range. Generalized |
382 |
thermal diffusivity D-T(k) decreases as a function |
383 |
of k, after an initial minor increase at k = |
384 |
k(min). The k dependence of the generalized |
385 |
thermodynamic properties has been calculated in the |
386 |
atomic and molecular formalisms. The observed |
387 |
differences have been traced back to intramolecular |
388 |
or intermolecular rotational effects and related to |
389 |
the partial structure functions. Finally, from the |
390 |
results we calculated it appears that the SPC/E |
391 |
model gives results in better agreement with |
392 |
experimental data than the transferable |
393 |
intermolecular potential with four points TIP4P |
394 |
water model {[}Jorgensen et al., J. Chem. Phys. 79, |
395 |
926 (1983)], with a larger improvement for, e.g., |
396 |
diffusion, viscosities, and dielectric properties |
397 |
and a smaller one for thermal conductivity. The |
398 |
SPC/E model shares, to a smaller extent, the |
399 |
insufficient slowing down of dynamics at low |
400 |
temperature already found for the TIP4P water |
401 |
model.}, |
402 |
Address = {ONE PHYSICS ELLIPSE, COLLEGE PK, MD 20740-3844 |
403 |
USA}, |
404 |
Affiliation = {UNIV PISA,DIPARTIMENTO CHIM \& CHIM IND,I-56126 |
405 |
PISA,ITALY. CNR,IST FIS ATOM \& MOL,I-56127 |
406 |
PISA,ITALY.}, |
407 |
Author = {Bertolini, D and Tani, A}, |
408 |
Date-Added = {2009-10-30 15:41:21 -0400}, |
409 |
Date-Modified ={2009-10-30 15:41:21 -0400}, |
410 |
Doc-Delivery-Number ={YC322}, |
411 |
Issn = {1063-651X}, |
412 |
Journal = {Phys. Rev. E}, |
413 |
Journal-Iso = {Phys. Rev. E}, |
414 |
Keywords-Plus ={TIME-CORRELATION-FUNCTIONS; LENNARD-JONES LIQUID; |
415 |
TRANSPORT-PROPERTIES; SUPERCOOLED WATER; DENSITY; |
416 |
SIMULATIONS; RELAXATION; VELOCITY; ELECTRON; |
417 |
FLUIDS}, |
418 |
Language = {English}, |
419 |
Month = {OCT}, |
420 |
Number = {4}, |
421 |
Number-Of-Cited-References ={35}, |
422 |
Pages = {4135-4151}, |
423 |
Publisher = {AMERICAN PHYSICAL SOC}, |
424 |
Subject-Category ={Physics, Fluids \& Plasmas; Physics, |
425 |
Mathematical}, |
426 |
Times-Cited = {18}, |
427 |
Title = {Thermal conductivity of water: Molecular dynamics |
428 |
and generalized hydrodynamics results}, |
429 |
Type = {Article}, |
430 |
Unique-Id = {ISI:A1997YC32200056}, |
431 |
Volume = {56}, |
432 |
Year = {1997} |
433 |
} |
434 |
|
435 |
@article{Meineke:2005gd, |
436 |
Abstract = {OOPSE is a new molecular dynamics simulation program |
437 |
that is capable of efficiently integrating equations |
438 |
of motion for atom types with orientational degrees |
439 |
of freedom (e.g. #sticky# atoms and point |
440 |
dipoles). Transition metals can also be simulated |
441 |
using the embedded atom method (EAM) potential |
442 |
included in the code. Parallel simulations are |
443 |
carried out using the force-based decomposition |
444 |
method. Simulations are specified using a very |
445 |
simple C-based meta-data language. A number of |
446 |
advanced integrators are included, and the basic |
447 |
integrator for orientational dynamics provides |
448 |
substantial improvements over older quaternion-based |
449 |
schemes.}, |
450 |
Address = {111 RIVER ST, HOBOKEN, NJ 07030 USA}, |
451 |
Author = {Meineke, M. A. and Vardeman, C. F. and Lin, T and Fennell, |
452 |
CJ and Gezelter, J. D.}, |
453 |
Date-Added = {2009-10-01 18:43:03 -0400}, |
454 |
Date-Modified ={2010-04-13 09:11:16 -0400}, |
455 |
Doi = {DOI 10.1002/jcc.20161}, |
456 |
Isi = {000226558200006}, |
457 |
Isi-Recid = {142688207}, |
458 |
Isi-Ref-Recids ={67885400 50663994 64190493 93668415 46699855 |
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461 |
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462 |
99223832 142688208 94600872 91658572 54857943 |
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468 |
97861662 71842426 130707771 125809946 66381889 |
469 |
99676497}, |
470 |
Journal = {J. Comp. Chem.}, |
471 |
Keywords = {OOPSE; molecular dynamics}, |
472 |
Month = feb, |
473 |
Number = {3}, |
474 |
Pages = {252-271}, |
475 |
Publisher = {JOHN WILEY \& SONS INC}, |
476 |
Times-Cited = {9}, |
477 |
Title = {OOPSE: An object-oriented parallel simulation engine |
478 |
for molecular dynamics}, |
479 |
Volume = {26}, |
480 |
Year = {2005}, |
481 |
Bdsk-Url-1 = |
482 |
{http://gateway.isiknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcAuth=Alerting&SrcApp=Alerting&DestApp=WOS&DestLinkType=FullRecord;KeyUT=000226558200006}, |
483 |
Bdsk-Url-2 = {http://dx.doi.org/10.1002/jcc.20161} |
484 |
} |
485 |
|
486 |
@article{ISI:000080382700030, |
487 |
Abstract = {A nonequilibrium method for calculating the shear |
488 |
viscosity is presented. It reverses the |
489 |
cause-and-effect picture customarily used in |
490 |
nonequilibrium molecular dynamics: the effect, the |
491 |
momentum flux or stress, is imposed, whereas the |
492 |
cause, the velocity gradient or shear rate, is |
493 |
obtained from the simulation. It differs from other |
494 |
Norton-ensemble methods by the way in which the |
495 |
steady-state momentum flux is maintained. This |
496 |
method involves a simple exchange of particle |
497 |
momenta, which is easy to implement. Moreover, it |
498 |
can be made to conserve the total energy as well as |
499 |
the total linear momentum, so no coupling to an |
500 |
external temperature bath is needed. The resulting |
501 |
raw data, the velocity profile, is a robust and |
502 |
rapidly converging property. The method is tested on |
503 |
the Lennard-Jones fluid near its triple point. It |
504 |
yields a viscosity of 3.2-3.3, in Lennard-Jones |
505 |
reduced units, in agreement with literature |
506 |
results. {[}S1063-651X(99)03105-0].}, |
507 |
Address = {ONE PHYSICS ELLIPSE, COLLEGE PK, MD 20740-3844 USA}, |
508 |
Affiliation = {Muller-Plathe, F (Reprint Author), Max Planck Inst |
509 |
Polymerforsch, Ackermannweg 10, D-55128 Mainz, |
510 |
Germany. Max Planck Inst Polymerforsch, D-55128 |
511 |
Mainz, Germany.}, |
512 |
Author = {M\"{u}ller-Plathe, F}, |
513 |
Date-Added = {2009-10-01 14:07:30 -0400}, |
514 |
Date-Modified ={2009-10-01 14:07:30 -0400}, |
515 |
Doc-Delivery-Number ={197TX}, |
516 |
Issn = {1063-651X}, |
517 |
Journal = {Phys. Rev. E}, |
518 |
Journal-Iso = {Phys. Rev. E}, |
519 |
Language = {English}, |
520 |
Month = {MAY}, |
521 |
Number = {5, Part A}, |
522 |
Number-Of-Cited-References ={17}, |
523 |
Pages = {4894-4898}, |
524 |
Publisher = {AMERICAN PHYSICAL SOC}, |
525 |
Subject-Category ={Physics, Fluids \& Plasmas; Physics, |
526 |
Mathematical}, |
527 |
Times-Cited = {57}, |
528 |
Title = {Reversing the perturbation in nonequilibrium |
529 |
molecular dynamics: An easy way to calculate the |
530 |
shear viscosity of fluids}, |
531 |
Type = {Article}, |
532 |
Unique-Id = {ISI:000080382700030}, |
533 |
Volume = {59}, |
534 |
Year = {1999} |
535 |
} |
536 |
|
537 |
@article{ISI:000246190100032, |
538 |
Abstract = {Atomistic simulations are conducted to examine the |
539 |
dependence of the viscosity of |
540 |
1-ethyl-3-methylimidazolium |
541 |
bis(trifluoromethanesulfonyl)imide on temperature |
542 |
and water content. A nonequilibrium molecular |
543 |
dynamics procedure is utilized along with an |
544 |
established fixed charge force field. It is found |
545 |
that the simulations quantitatively capture the |
546 |
temperature dependence of the viscosity as well as |
547 |
the drop in viscosity that occurs with increasing |
548 |
water content. Using mixture viscosity models, we |
549 |
show that the relative drop in viscosity with water |
550 |
content is actually less than that that would be |
551 |
predicted for an ideal system. This finding is at |
552 |
odds with the popular notion that small amounts of |
553 |
water cause an unusually large drop in the viscosity |
554 |
of ionic liquids. The simulations suggest that, due |
555 |
to preferential association of water with anions and |
556 |
the formation of water clusters, the excess molar |
557 |
volume is negative. This means that dissolved water |
558 |
is actually less effective at lowering the viscosity |
559 |
of these mixtures when compared to a solute obeying |
560 |
ideal mixing behavior. The use of a nonequilibrium |
561 |
simulation technique enables diffusive behavior to |
562 |
be observed on the time scale of the simulations, |
563 |
and standard equilibrium molecular dynamics resulted |
564 |
in sub-diffusive behavior even over 2 ns of |
565 |
simulation time.}, |
566 |
Address = {1155 16TH ST, NW, WASHINGTON, DC 20036 USA}, |
567 |
Affiliation = {Maginn, EJ (Reprint Author), Univ Notre Dame, Dept |
568 |
Chem \& Biomol Engn, 182 Fitzpatrick Hall, Notre |
569 |
Dame, IN 46556 USA. Univ Notre Dame, Dept Chem \& |
570 |
Biomol Engn, Notre Dame, IN 46556 USA.}, |
571 |
Author = {Kelkar, Manish S. and Maginn, Edward J.}, |
572 |
Author-Email = {ed@nd.edu}, |
573 |
Date-Added = {2009-09-29 17:07:17 -0400}, |
574 |
Date-Modified ={2009-09-29 17:07:17 -0400}, |
575 |
Doc-Delivery-Number ={163VA}, |
576 |
Doi = {10.1021/jp0686893}, |
577 |
Issn = {1520-6106}, |
578 |
Journal = {J. Phys. Chem. B}, |
579 |
Journal-Iso = {J. Phys. Chem. B}, |
580 |
Keywords-Plus ={MOLECULAR-DYNAMICS SIMULATION; MOMENTUM IMPULSE |
581 |
RELAXATION; FORCE-FIELD; TRANSPORT-PROPERTIES; |
582 |
PHYSICAL-PROPERTIES; SIMPLE FLUID; CHLORIDE; MODEL; |
583 |
SALTS; ARCHITECTURE}, |
584 |
Language = {English}, |
585 |
Month = {MAY 10}, |
586 |
Number = {18}, |
587 |
Number-Of-Cited-References ={57}, |
588 |
Pages = {4867-4876}, |
589 |
Publisher = {AMER CHEMICAL SOC}, |
590 |
Subject-Category ={Chemistry, Physical}, |
591 |
Times-Cited = {35}, |
592 |
Title = {Effect of temperature and water content on the shear |
593 |
viscosity of the ionic liquid |
594 |
1-ethyl-3-methylimidazolium |
595 |
bis(trifluoromethanesulfonyl)imide as studied by |
596 |
atomistic simulations}, |
597 |
Type = {Article}, |
598 |
Unique-Id = {ISI:000246190100032}, |
599 |
Volume = {111}, |
600 |
Year = {2007}, |
601 |
Bdsk-Url-1 = {http://dx.doi.org/10.1021/jp0686893%7D}, |
602 |
Bdsk-Url-2 = {http://dx.doi.org/10.1021/jp0686893} |
603 |
} |
604 |
|
605 |
@article{MullerPlathe:1997xw, |
606 |
Abstract = {A nonequilibrium molecular dynamics method for |
607 |
calculating the thermal conductivity is |
608 |
presented. It reverses the usual cause and effect |
609 |
picture. The ''effect,'' the heat flux, is imposed |
610 |
on the system and the ''cause,'' the temperature |
611 |
gradient is obtained from the simulation. Besides |
612 |
being very simple to implement, the scheme offers |
613 |
several advantages such as compatibility with |
614 |
periodic boundary conditions, conservation of total |
615 |
energy and total linear momentum, and the sampling |
616 |
of a rapidly converging quantity (temperature |
617 |
gradient) rather than a slowly converging one (heat |
618 |
flux). The scheme is tested on the Lennard-Jones |
619 |
fluid. (C) 1997 American Institute of Physics.}, |
620 |
Address = {WOODBURY}, |
621 |
Author = {M\"{u}ller-Plathe, F.}, |
622 |
Cited-Reference-Count ={13}, |
623 |
Date = {APR 8}, |
624 |
Date-Added = {2009-09-21 16:51:21 -0400}, |
625 |
Date-Modified ={2009-09-21 16:51:21 -0400}, |
626 |
Document-Type ={Article}, |
627 |
Isi = {ISI:A1997WR62000032}, |
628 |
Isi-Document-Delivery-Number ={WR620}, |
629 |
Iso-Source-Abbreviation ={J. Chem. Phys.}, |
630 |
Issn = {0021-9606}, |
631 |
Journal = {J. Chem. Phys.}, |
632 |
Language = {English}, |
633 |
Month = {Apr}, |
634 |
Number = {14}, |
635 |
Page-Count = {4}, |
636 |
Pages = {6082--6085}, |
637 |
Publication-Type ={J}, |
638 |
Publisher = {AMER INST PHYSICS}, |
639 |
Publisher-Address ={CIRCULATION FULFILLMENT DIV, 500 SUNNYSIDE BLVD, |
640 |
WOODBURY, NY 11797-2999}, |
641 |
Reprint-Address ={MullerPlathe, F, MAX PLANCK INST POLYMER RES, |
642 |
D-55128 MAINZ, GERMANY.}, |
643 |
Source = {J CHEM PHYS}, |
644 |
Subject-Category ={Physics, Atomic, Molecular & Chemical}, |
645 |
Times-Cited = {106}, |
646 |
Title = {A simple nonequilibrium molecular dynamics method |
647 |
for calculating the thermal conductivity}, |
648 |
Volume = {106}, |
649 |
Year = {1997} |
650 |
} |
651 |
|
652 |
@article{Muller-Plathe:1999ek, |
653 |
Abstract = {A novel non-equilibrium method for calculating |
654 |
transport coefficients is presented. It reverses the |
655 |
experimental cause-and-effect picture, e.g. for the |
656 |
calculation of viscosities: the effect, the momentum |
657 |
flux or stress, is imposed, whereas the cause, the |
658 |
velocity gradient or shear rates, is obtained from |
659 |
the simulation. It differs from other |
660 |
Norton-ensemble methods by the way, in which the |
661 |
steady-state fluxes are maintained. This method |
662 |
involves a simple exchange of particle momenta, |
663 |
which is easy to implement and to analyse. Moreover, |
664 |
it can be made to conserve the total energy as well |
665 |
as the total linear momentum, so no thermostatting |
666 |
is needed. The resulting raw data are robust and |
667 |
rapidly converging. The method is tested on the |
668 |
calculation of the shear viscosity, the thermal |
669 |
conductivity and the Soret coefficient (thermal |
670 |
diffusion) for the Lennard-Jones (LJ) fluid near its |
671 |
triple point. Possible applications to other |
672 |
transport coefficients and more complicated systems |
673 |
are discussed. (C) 1999 Elsevier Science Ltd. All |
674 |
rights reserved.}, |
675 |
Address = {THE BOULEVARD, LANGFORD LANE, KIDLINGTON, OXFORD OX5 |
676 |
1GB, OXON, ENGLAND}, |
677 |
Author = {M\"{u}ller-Plathe, F and Reith, D}, |
678 |
Date-Added = {2009-09-21 16:47:07 -0400}, |
679 |
Date-Modified ={2009-09-21 16:47:07 -0400}, |
680 |
Isi = {000082266500004}, |
681 |
Isi-Recid = {111564960}, |
682 |
Isi-Ref-Recids ={64516210 89773595 53816621 60134000 94875498 |
683 |
60964023 90228608 85968509 86405859 63979644 |
684 |
108048497 87560156 577165 103281654 111564961 |
685 |
83735333 99953572 88476740 110174781 111564963 |
686 |
6599000 75892253}, |
687 |
Journal = {Computational and Theoretical Polymer Science}, |
688 |
Keywords = {viscosity; Ludwig-Soret effect; thermal |
689 |
conductivity; Onsager coefficents; non-equilibrium |
690 |
molecular dynamics}, |
691 |
Number = {3-4}, |
692 |
Pages = {203-209}, |
693 |
Publisher = {ELSEVIER SCI LTD}, |
694 |
Times-Cited = {15}, |
695 |
Title = {Cause and effect reversed in non-equilibrium |
696 |
molecular dynamics: an easy route to transport |
697 |
coefficients}, |
698 |
Volume = {9}, |
699 |
Year = {1999}, |
700 |
Bdsk-Url-1 = |
701 |
{http://gateway.isiknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcAuth=Alerting&SrcApp=Alerting&DestApp=WOS&DestLinkType=FullRecord;KeyUT=000082266500004} |
702 |
} |
703 |
|
704 |
@article{Viscardy:2007lq, |
705 |
Abstract = {The thermal conductivity is calculated with the |
706 |
Helfand-moment method in the Lennard-Jones fluid |
707 |
near the triple point. The Helfand moment of thermal |
708 |
conductivity is here derived for molecular dynamics |
709 |
with periodic boundary conditions. Thermal |
710 |
conductivity is given by a generalized Einstein |
711 |
relation with this Helfand moment. The authors |
712 |
compute thermal conductivity by this new method and |
713 |
compare it with their own values obtained by the |
714 |
standard Green-Kubo method. The agreement is |
715 |
excellent. (C) 2007 American Institute of Physics.}, |
716 |
Address = {CIRCULATION \& FULFILLMENT DIV, 2 HUNTINGTON |
717 |
QUADRANGLE, STE 1 N O 1, MELVILLE, NY 11747-4501 |
718 |
USA}, |
719 |
Author = {Viscardy, S. and Servantie, J. and Gaspard, P.}, |
720 |
Date-Added = {2009-09-21 16:37:20 -0400}, |
721 |
Date-Modified ={2009-09-21 16:37:20 -0400}, |
722 |
Doi = {DOI 10.1063/1.2724821}, |
723 |
Isi = {000246453900035}, |
724 |
Isi-Recid = {156192451}, |
725 |
Isi-Ref-Recids ={18794442 84473620 156192452 41891249 90040203 |
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729 |
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730 |
156192449}, |
731 |
Journal = {J. Chem. Phys.}, |
732 |
Month = may, |
733 |
Number = {18}, |
734 |
Publisher = {AMER INST PHYSICS}, |
735 |
Times-Cited = {3}, |
736 |
Title = {Transport and Helfand moments in the Lennard-Jones |
737 |
fluid. II. Thermal conductivity}, |
738 |
Volume = {126}, |
739 |
Year = {2007}, |
740 |
Bdsk-Url-1 = |
741 |
{http://gateway.isiknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcAuth=Alerting&SrcApp=Alerting&DestApp=WOS&DestLinkType=FullRecord;KeyUT=000246453900035}, |
742 |
Bdsk-Url-2 = {http://dx.doi.org/10.1063/1.2724821} |
743 |
} |
744 |
|
745 |
@article{Viscardy:2007bh, |
746 |
Abstract = {The authors propose a new method, the Helfand-moment |
747 |
method, to compute the shear viscosity by |
748 |
equilibrium molecular dynamics in periodic |
749 |
systems. In this method, the shear viscosity is |
750 |
written as an Einstein-type relation in terms of the |
751 |
variance of the so-called Helfand moment. This |
752 |
quantity is modified in order to satisfy systems |
753 |
with periodic boundary conditions usually considered |
754 |
in molecular dynamics. They calculate the shear |
755 |
viscosity in the Lennard-Jones fluid near the triple |
756 |
point thanks to this new technique. They show that |
757 |
the results of the Helfand-moment method are in |
758 |
excellent agreement with the results of the standard |
759 |
Green-Kubo method. (C) 2007 American Institute of |
760 |
Physics.}, |
761 |
Address = {CIRCULATION \& FULFILLMENT DIV, 2 HUNTINGTON |
762 |
QUADRANGLE, STE 1 N O 1, MELVILLE, NY 11747-4501 |
763 |
USA}, |
764 |
Author = {Viscardy, S. and Servantie, J. and Gaspard, P.}, |
765 |
Date-Added = {2009-09-21 16:37:19 -0400}, |
766 |
Date-Modified ={2009-09-21 16:37:19 -0400}, |
767 |
Doi = {DOI 10.1063/1.2724820}, |
768 |
Isi = {000246453900034}, |
769 |
Isi-Recid = {156192449}, |
770 |
Isi-Ref-Recids ={18794442 89109900 84473620 86837966 26564374 |
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132156782 156192451}, |
779 |
Journal = {J. Chem. Phys.}, |
780 |
Month = may, |
781 |
Number = {18}, |
782 |
Publisher = {AMER INST PHYSICS}, |
783 |
Times-Cited = {1}, |
784 |
Title = {Transport and Helfand moments in the Lennard-Jones |
785 |
fluid. I. Shear viscosity}, |
786 |
Volume = {126}, |
787 |
Year = {2007}, |
788 |
Bdsk-Url-1 = |
789 |
{http://gateway.isiknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcAuth=Alerting&SrcApp=Alerting&DestApp=WOS&DestLinkType=FullRecord;KeyUT=000246453900034}, |
790 |
Bdsk-Url-2 = {http://dx.doi.org/10.1063/1.2724820} |
791 |
} |
792 |
|