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21 Jul 2009: The idea of a corrective pseudo-potential force was suggested independently by Rallison (1979), who used a much simpler approach based on Maxwell-Boltzmann thermodynamic equilibrium distributions in the full phase

31 Jul 2009: Hinch. Maxwell-Boltzmann distribution c cc exp ( - V / k T ). Using this distribution and equating the net flux to zero produces the result (1.1).

21 Jul 2009: 1987). The tensor a satisfies the upper convected Maxwell equation. v haa = y ,. is the upper-convected derivative of a, and h is the polymer relaxation time. ... The Oldroyd-B model contains both the upper-convected Maxwell fluid (ys = 0-.

28 Sep 2009: 36 pages. 2. Eamonn Long and David M.A. Stuart, “Effective dynamics for solitons in thenonlinear Klein-Gordon-Maxwell system and the Lorentz force law”, Reviews inMathematical Physics, 21 (4), (2009)

23 Jul 2009: As shown by Hocking (1973), who used a simple Maxwell-slip model to study the relative motion of rigid spheres in aerosols, actual physical contact between the solid surfaces can occur

10 Jul 2009: They then tested these fluids in a LFR. Now, for a Maxwell fluid with a single relaxation time, Bazilievsky, Entov and Rozhkow [1]have shown that in a LFR the radius

8 Jul 2009: This was demon-strated for instance by Rasmussen and Hassager [30], who carryout three-dimensional simulations of the creeping flow of anupper-convected Maxwell fluid described by an integral modelin a

23 Jul 2009: Then a t time t = 0 the probability distribution for the particle positions is Maxwell-Boltzmann with.

14 Jul 2009: In the case of inertia, unlike the variable diffusivity, the phenomenon is correct: when a Maxwell-Boltzmann distribution in phase-space is.

14 Jul 2009: http://journals.cambridge.org Downloaded: 14 Jul 2009 IP address: 131.111.16.227. J. Fluid Mech. (1996), t d 308, p p. 255-288 Copyright @ 1996 Cambridge University Press. 255. Computer simulations of polymer chain relaxation via Brownian motion. By