Search

5 Dec 2007: J. Fluid Mech. (1986), vol. 161, p p. 449-492 Printed in &eat Britain. 449. Do Rossby-wave critical layers absorb, reflect, or over-reflect? By PETER D. KILLWORTH? A N D MICHAEL E. M c I N T Y R E Department of Applied Mathematics & Theoretical

17 Jan 2008: Mathematical Tripos: IA Vector Calculus. Contents. 0 Introduction i. 0.1 Schedule. i. 0.2 Lectures. i. 0.3 Printed Notes. ii. 0.4 Examples Sheets. iii. 0.5 Previous Comments, Comments on Comments and Style of Lectures. iii. 0.6 Books. iv. 0.7

29 Jan 2008: Thus the orthogonality conditions. d Tj F (xk1) = 0, j = 1, 2,. ,

3 Jul 2008: Adiabatic limit and the slow motion of vortices in a. Chern-Simons-Schroedinger system. Sophia Demoulini and David StuartCentre for Mathematical Sciences, Wilberforce Road, Cambridge, CB3 OWB, England. email:sd290@cam.ac.uk, dmas2@cam.ac.uk.

31 Jul 2008: If we consider the two following expansions:. h(t) =. j=0. aj tj, h(t) =. k=0. bk. (. t. 1 t. )k. , (8). which converge inside D, then it is true ... By using the first expansion in (8), it follows that. bk =. j=0. aj Bj,k, Bj,k =1. 2πi. Ct. tj(1 t)k1.

19 Nov 2008: Prove the results (a = |a|),. (i) [Ti , Tj ] = iijkTk ,. (ii) (aT)3 = a2aT ,. (iii) exp(iaT) = 1 iaT sin aa (aT)2 cos a1.

13 Jul 2009: 7’ = 7-- 70 - crm,. when C,[TJ] > 1. (5). ... 771e = [VIU %Jrll). (9) Taking as an example 0.5% master solution of Polyox with [TJ] = 2000 cm3/ gram and q. =

13 Jul 2009: With a streamfunction tj = r1 “f(0), th’ is no-slip boundary condition gives f(0) =f’(O) = 0.

13 Jul 2009: x(tj-(O)]=n6D,Ati=2D,t, (24). where the factor l/3 represents the variance of a random number chosen uniformly on [ - 1, 11.

21 Jul 2009: http://journals.cambridge.org Downloaded: 21 Jul 2009 IP address: 131.111.16.227. 3. Fluid Mech. (1993), vol. 256, pp. 3 4 3 4 0 1 Copyright @ 1993 Cambridge University Press. 343. Nonlinear drift interactions between fluctuating colloidal particles: