Search

26 Jul 2013: J. Elfring and E. Lauga Phys. Fluids 24, 072102 (2012). Equation (14) was derived by Howe,11 and restated in English by Gillette and Dyson,12 to havea solution. ... C. Dyson, “Stability of fluid interfaces of revolution between equal solid circular

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

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.

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

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.

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

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

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