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29 Jan 2009: Apply Ampére’s law. C. B.dr = µ0I (20). to the plane needle shaped contour C shown, in the limit δ 0 for finite (small) l.

28 Sep 2009: Math. Letters 9(5), (1996), 27-33. 20. D. Stuart, “Minimal periods for solutions of some classical field equations”, SIAMJournal of Mathematical Analysis, 27(4), (1996), 1095-1101.

3 Sep 2009: µ = W0ψ2(1γ)0 V0ψ. 20. (10). The hydrostatic pressure of the system is found as. ... Fluid Dyn. Res. 41 (2009) 051403 N G Berloff. 0 20 40 60 80 1000.

13 Jul 2009: Increments between the bulk streamlines are 20 times the increments between the recirculating streamlines. ... Non-Newtonian Fluid Mech., 20 (1986) 11-29. 4 R.E. Evans and K.

26 Apr 2009: 3, 473–485, June 2006; e-print: quant-ph/0410034. (20) N.Datta, Multiplicativity of Maximal p-Norms in Werner-Holevo channels for 1 p 2: quant-ph/0410063.

13 Jul 2009: o 1. lO 20 30 50. lOO 200 500 600 700 800. ... flux boundary conditions (equations (2.20) and (2.21) in that paper) are incorrect, appar- ently because of algebraic errors incurred in the process of finding the limiting forms of the

27 Jul 2009: To testthis conjecture Loftin, Yau and Zaslow (LYZ) [20] aimed to prove the existence of themetric of Hessian form1. ... The ASDYM equations with these reality conditions are. Fzw = 0, (4.20)Fzz̄ Fww̄ = 0.

10 Jul 2009: F 13. Comparison of finger widths for 10 % and 20 % offset sinks, with γ 310%.10 % offset case is at t 22.3575. ... 10 % and 20 % offset sinks, with γ 310%. Numerical simulations of sink flow in the Hele-Shaw cell 549.

13 May 2009: m c)nn! vn, (3.20). for the same values of m. This gives. ... 2z. [(α β)z ǫ1 ǫ2]2 4z2z. , (4.20). where = αβz ǫ1β ǫ2α.

13 Jul 2009: Downloaded13Jul2009to131.111.16.20.RedistributionsubjecttoAIPlicenseorcopyright;seehttp://pof.aip.org/pof/copyright.jsp. and Mazur for that case of a channel of width of 10 particlediameters. ... 2237Phys. Fluids, Vol. 8, No. 8, August 1996 Brief