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13 Jul 2009: Downloaded 13 Jul 2009 to 131.111.16.20. Redistribution subject to AIP license or copyright; see http://pof.aip.org/pof/copyright.jsp.

13 Jul 2009: Downloaded 13 Jul 2009 to 131.111.16.20. Redistribution subject to AIP license or copyright; see http://pof.aip.org/pof/copyright.jsp.

8 Jul 2009: Experiments were performed in glass-wall vessels of dif-ferent cross sections 20 20 cm2, 10 10 cm2, and4 10 cm2 but filled with the same fluid height of 40 cm. ... The line indicates the best linear fit.The different cross sections presented are 20 20

20 Sep 2009: in 2026 (20% growth against 14% growth in England). Projected growth second highest in English regions. ... 3.0. -2.0. -1.0. 0.0. 1.0. 2.0. 3.0. 4.0. 5.0. 20. 01.

16 Sep 2009: Roads : 20% ‘SLOAP’ : 40FAR : 0.4Off-street parking: 100%. • ... Roads : 20 % ‘SLOAP’ : 0FAR : 0.4Off-street parking: 100%. •

20 Sep 2009: b. illio. n. 0. 10. 20. 30. 40. 50. 60. 70. ... 12. -80.0% -70.0% -60.0% -50.0% -40.0% -30.0% -20.0% -10.0% 0.0%. City of London.

20 Jan 2009: 20. 7. Perfectly conducting planes are positioned at z = 0 and z = a.

20 Sep 2009: MPDB2008. •20,000 <250 employee. companies in Eastern Region. •Part of national economy.

24 Feb 2009: t f2/t. 02. IC 2009, runout – p.20/59. Duration of flow, T. ... 0 5 10 15 20 25(RR0)/R0. 0. 1. 2. 3. 4E.

3 Sep 2009: Published July 20, 2009. Chaotic matter waves formed by perturbing a Bose-Einstein condensate may provide a valuable laboratorysetting for understanding many different kinds of quantum-fluid turbulence. ... Magalhães and V. S. BagnatoPhys. Rev. Lett. 103

20 Jan 2009: 20. a) Parallel-plate capacitor (two metal surfaces of areas A held a distance a apart.) Find thecapacitance.

16 Jan 2009: 2 1. c22. t2. ). E = 0, (20). where the wave speed c is given by.

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.

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.

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

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.

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.

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: 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