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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-.

22 Jun 2009: PETRVM MAXWELL DAVIES. RPHEUS is said to have charmed wild beasts and stayed fast-flowing rivers with his Thracian lyre. ... I present to you. Sir PETER MAXWELL DAVIES, C.B.E. Honorary Fellow of Homerton College, Composer and Conductor, Master of the

3 Dec 2009: 1 Abstracting from a substantial literature, a useful summary of the ways in which poverty is variously defined and measured is given by Maxwell (1999 ). 2 For further discussion of these ... combine these approaches leads to logical incoherence, and

7 Jul 2009: 8 Propertius III 2 1–2. PETRVM MAXWELL DAVIES. ORPHEUS is said to have charmed wild beasts and stayed fast-flowing rivers with his Thracianlyre. ... I present to you. Sir PETER MAXWELL DAVIES, C.B.E.Honorary Fellow of Homerton College, Composer and

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

19 Oct 2009: 5The electric field E and magnetic field B of Maxwell’s equations contain only “physical”degrees of freedom, in the sense that every mathematical degree of freedom in an electromag-netic

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).

25 Nov 2009: tion were followed by the reassignments of velocities from the Maxwell.

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

8 Aug 2009: The Maxwell–Calladinerelation (see Calladine 1978) reads as. m Z s C3jKbK6; ð2:1Þwhere b is the total number of bars and j is total number of joints in thestructure.

28 Apr 2009: Perfect decisions in a two-person game. Say we have two players, called Maxwell and Minny - Max and Minfor short.

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

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

25 Nov 2009: John T. Maxwell III. Name type ambiguity: more evidence against gazetteers 15. •

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 Apr 2009: Perfect decisions in a two-person game. Say we have two players, called Maxwell and Minny - Max and Minfor short.

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.