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10
11
12 @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.},
39 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},
47 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},
83 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
87 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.},
141 Address = {CIRCULATION \& FULFILLMENT DIV, 2 HUNTINGTON
142 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
459 89992422 57614458 49016001 61447131 111114169
460 68770425 52728075 102422498 66381878 32391149
461 134477335 53221357 9929643 59492217 69681001
462 99223832 142688208 94600872 91658572 54857943
463 117365867 69323123 49588888 109970172 101670714
464 142688209 121603296 94652379 96449138 99938010
465 112825758 114905670 86802042 121339042 104794914
466 82674909 72096791 93668384 90513335 142688210
467 23060767 63731466 109033408 76303716 31384453
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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727 93329429 95967319 6199670 1785176 105872066 6325196
728 65361295 71941152 4307928 23120502 54053395
729 149068110 4811016 99953572 59859908 132156782
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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774 129596740 120782555 51131244 65361295 41141868
775 4307928 21555860 23120502 563068 120721875 142813985
776 135942402 4811016 86224873 57621419 85506488
777 89860062 44796632 51381285 132156779 156192450
778 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