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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).

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

22 Jan 2009: eg = 2πN, N = 1, 2, 3,. Maxwell equations = U (1) gauge theory.

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

8 Jul 2009: used a 2 fs integration time step and covalent bonds involvinghydrogen atoms were constrained with SHAKE.30 All simulationswere performed at 300 K; initial velocities were randomly assignedfrom a Maxwell-Boltzmann

28 Nov 2009: Appendix A1 : Electromagnetism. Prof. M.A. Thomson Michaelmas 2009 476. (Non-examinable) In Heaviside-Lorentz units Maxwell’s equations in the.

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.