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19 Oct 2013: In the absence of specific information about the vertical profile of Maxwell stressesBrBφ at the periphery, there is an undetermined function ofz in the problem. ... In the example shownα was chosen, purely on Occam’s-razor grounds, to makethe

26 Jul 2013: 2uS2(xS0 , t). (6). 1It includes inparticular: secondandn-thorderfluid, allOldroyd-like models (upper-convected Maxwell, lower-convected Maxwell,corotational Maxwell, Oldroyd-A, Oldroyd-B, corotational Oldroyd,Oldroyd 8-constant model,

20 May 2013: An Example in d=11. d=11 dimensional Maxwell coupled to a massless Dirac fermion.

19 Aug 2013: I a retardation time λ2. Special cases. I Maxwell UCM λ2 = 0.

19 Oct 2013: namo action, is held down in magnitude, by the dynamo’s turbulent Maxwell. ... ably assume that it will act to reduce shear through the Maxwell stresses.

19 Oct 2013: Rather, the tachocline circulation must be driven. mainly by the Reynolds and Maxwell stresses interior to the convection zone,.

26 Jul 2013: The experimental values ofG′(ω) and G′′(ω) are fitted to a generalized Maxwell model,26 G′(ω) =. Ni =1(gi λ. 2i ω. 2)/(1 λ2i ω2)and G′′(ω) =

26 Jul 2013: 3). The polymeric stress τ p is then assumed to be governed by the upper-convected Maxwell equation:. ... the polymeric relaxation time, λ) toa characteristic time scale of the flow system (1/$), and appears in the dimensionless momentumequation and

26 Jul 2013: Fig. 19.1 Interpretation of the (Maxwell–Navier) sliplength λ. face the rate of strain tensor is different from the normalderivative of the tangential component of the flow so allthe terms ... The possibility of gas slip was first intro-duced by

21 Mar 2013: 20 CHAPTER 1. INTRODUCTION. Maxwell equations which can be seen to describe an arbitrary number of dy-. ... in both sets of coordinates. Solutions of the Einstein-Maxwell equations of Kastor-Traschen correspond to.

26 Jul 2013: A. Model. In the Oldroyd-B model, the polymeric stress, p satis-fies the upper-convected Maxwell equation. ... to the Maxwell model, i.e., of a dashpotof viscosity p in series with a spring of constant kp = p /. It is reasonable to consider two different

26 Jul 2013: Thisrelation was first proposed by Navier (1823) for liquids and was also rigorouslyderived by Maxwell (1879) in the case of gases, with a slip length of the order of themean free

4 Oct 2013: But the wave equation also has genuinely fundamental significance inother areas: for example in electromagnetic theory, Maxwell’s equations imply the theelectromagnetic potentials must satisfy the wave equation in regions free

3 Feb 2013: The ratchets mimic Maxwell’s demon, but there is no con-flict with thermodynamics due to the nonequilibrium nature ofliving systems.

20 Dec 2013: Reall. 2.7. TENSORS. the idea that the Maxwell field in special relativity is described by a tensor.

26 Jul 2013: PHYSICS OF FLUIDS 17, 103102 2005. Brownian motion near a partial-slip boundary: A local probeof the no-slip condition. Eric Laugaa. Division of Engineering and Applied Sciences, Harvard University, Cambridge, Massachusetts 02138. Todd M. Squiresb.

7 Jan 2013: The ratchets mimic Maxwell’s demon, but there is no con-flict with thermodynamics due to the nonequilibrium nature ofliving systems.