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4 Mar 2016: ux0 þ rðtÞ; t uðx0; tÞþ rðtÞu xðx0; tÞ: (24). As the velocity field, the distance x and the displacement rare made dimensionless using n0x, k.

19 Oct 2016: This paper is based on an invited lecture given by Keith Moffatt at the 68th Annual Meeting of the APSDivision of Fluid Dynamics, which was held 22–24 November 2015 in

6 Oct 2016: 24. 2.2.4 Proof of the factorization theorem for SDP lifts. We now give a proof of Theorem 3.

11 Jan 2016: leakage rate predicted by (2.24) is then unphysical because there is no fluidabove the outlet to draw. ... Generally, this assumptionis invalid if the current delivers a smaller flux towards the outlet than is predicted toleak according to (2.24).

26 Nov 2016: φ(x, y) = (2 2x y) e2xy sin(2x y) (y 2) ex , (9.24).

1 Jun 2016: Received 2 December 2015; revised 13 April 2016; accepted 24 April 2016). ... 6 ms 12 ms 18 ms 24 ms. 2000. –2000. 2000.

30 Oct 2016: What is the physical meaning of Ψ in 3.1 and 3.24? ... What are the meanings of Ẋc and Ṙ in 3.24? 2.

21 Jan 2016: Although this issue has been quite widely recognized [24, 56, 60], there have been few attempts madethus far to extend the existing theory to infinite-dimensional models (see 1.4).

10 Feb 2016: ZΛZsΛ. ]1/2= 1. [d 22. γφ. ]δs (5.24). with γφ as in (5.16).

6 Nov 2016: VECTORS AND MATRICES 24 lectures, Michaelmas term. Complex numbersReview of complex numbers, including complex conjugate, inverse, modulus, argument and Arganddiagram. ... You should be able to do example sheets 1/2/3/4 after lectures 6/12/18/24

6 Oct 2016: 24. Translation of frequencies. We have:. f (x ) =. j.

3 Jun 2016: 24. where xj, j = 1, ,n are the zeros of a monic orthogonal polynomial Pωn (x) of degree non [0,b] with the complex weight function h(x)eiωg(x), b.

24 Oct 2016: There is a wide variety of problems that lack incoherence, a fact that has been widely recognized [2,6, 10, 11, 24, 25, 27, 33–36, 40], however, they instead posses

2 Oct 2016: Annu. Rev. Fluid Mech. 1995. 27: 169-93 Copyright 1995 by Annual Reviews Inc. All rights reserved. CONSTITUTIVE EQUATIONS FOR. POLYMERIC LIQUIDS. R. Byron Bird. Department of Chemical Engineering and Rheology Research Center, University of Wisconsin,

2 Oct 2016: KL ::::: - ( 1 /24)[2 (rods, length I), = - ( 1/3)c2 (disks, radius c). ... p = -kT[C-C'],. which gives the following when substituted into (24) and (27):.

12 Aug 2016: 1.24). The reader should note that the original geometry has been recovered in the limit ,u << 1. ... With no precession, (1.22)-( 1.24) is the normal mode problem for a uniformly-rotating basic state within a spheroidal container.

10 Nov 2016: The Evolution of Silicon Transport in Eukaryotes. Alan O. Marron,1,2 Sarah Ratcliffe,3 Glen L. Wheeler,4 Raymond E. Goldstein,1 Nicole King,5 Fabrice Not,6,7. Colomban de Vargas,6,7 and Daniel J. Richter5,6,71Department of Applied Mathematics and

28 Jan 2016:

21 Jan 2016: Although this issue has been quite widely recognized [24, 56, 60], there have been few attempts madethus far to extend the existing theory to infinite-dimensional models (see 1.4).

11 Jan 2016: T. P= Ta. P+ 5̄. ρg′c2. (24). Thus the conductive heat flux, qcond, may be expressed in terms ofthe adiabat and the potential temperature.