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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.

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.

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

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.

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.

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: 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

13 Jul 2009: Fluids, 20 (1977) 5280. 19 A.B. Metzner and A.D. Metzner, Rheol. ... Acta, 9 (1970) 174. 20 E. Biigen, J. de MI%., 12 (1973) 375.

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.

21 Jul 2009: Viscous effects increase the height of the floating disk by 20% even at a Reynolds number of 50. ... 2. We observe that the viscosity increases h / p : by typically 20% from the high.

21 Jul 2009: S. Bhatt. 0.20 I '. 0.18 I I I. I. 0.16. ... with a numerical evaluation. The small-k result over-estimates the value by 20 % by k = 0.1.

8 Jul 2009: For silicon oil with viscosity µ = 20 Pa s and acrylicbeads with diameter 0.58 mm, the settling time was d/VS = 0.27 s and the coefficientswere found to be. ... h. )Θ. 2(2Θ 1) Θ. 4 tan χcg (Θ 1). ). (4.20). The first term on the right-hand side is

13 Jul 2009: 2.0. 1.5. 1.0. 0.5. 010 15 20 25 30. Ca = 0. ... Trajectories terminate at (20,x2,x3), where. (x2,x3) are marked with. 3. 2.

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.

23 Jul 2009: 0 = 20' when X = 3 and the reversing turn starts from 0 = 70' when X = 3. ... 1.60. < 1.40 C. e z. 6 1.20 - I / x 1 / K.

24 Aug 2009: 3.20). (3.21). (3.22). subject to the matching conditions. go = 0, U, = 0, = [(I -i)/24] a$,/& at z = 1. ... 14 0 0.04 0.08 0.12 0.16 0.20. - 0.2. - 0.4 a. -

8 Jul 2009: The study is performed in a 4-m-long transparent tubewith an internal diameter d = 20 mm that can be tilted to all. ... FIG. 2. Color Images of the normalized relative fraction of light fluidobtained at different tilt angles = 0 , 20 , 40 , 60 , 75, and

31 Jul 2009: 10. 8. 6. 4. 2. I I I I I 0 4 8 12 16 20. ... 20 - 4. 0 4 8 12 16 20. Y l D FIQIJRE 4.

8 Jul 2009: 20. 15. 10. 5. 0 1 2 3 0 2 4 6 8 10. ... 0 5 10(R – R0)/R0. 15 20 25. ES/(. mSgR. 0)E.

20 Mar 2009: 2009 Macmillan Publishers Limited. All rights reserved. << /ASCII85EncodePages false /AllowTransparency false /AutoPositionEPSFiles true /AutoRotatePages /None /Binding /Left /CalGrayProfile (Dot Gain 20%) /CalRGBProfile (sRGB IEC61966-2.1)

10 Jul 2009: S0031-9007(97)05092-8]. PACS numbers: 47.11. j, 02.70.Pt, 47.20.Cq, 68.10. – m. ,. aher. al. lst,. ln,ed. gesngr-n. ffy.dutof. Inviscid pinchoff is ... With these numerical valueof A, B, and a, the three terms in the Bernoulli equa-tion (1) become in

23 Jul 2009: p E { ( T - 6,O) e(3fT cos 2 8 , 2 f ( T - 6 ) sin 20) O ( e 2 ) } , in which changes in the internal pressure have been ruled out at ... R ( 0 , z ; e ) = R,(z) [ 1 e f ( z ) cos 20 O(e2)].

10 Jul 2009: and22. No pre-stretch was applied. The best fit of the adjustable parameter is L1 = 20. ... i ) (in Pa) as a function of time (in s) for the case L1 = 20.

8 Jun 2009: 1. advection part ( f A): t. Ω. u dV. Γu(u n) dS = 0 (20). ... 4.5. 5. 5.5. 0 10 20 30 40 50 60 70 80.

30 Aug 2009: in the literature from 20–60%, remains airborne for athousand years or longer. ... For comparison, the IPCC business-as-usual scenario (SRES A1B). 0%. 10%. 20%.

13 Jul 2009: a’=20 11-022-633. E.J. Hinch / J. Non-Newtonian Fluid Mech. 54 (1994) 209-230 211. ... 14. In Fig. 20 we have plotted ,uextNb4/pR4(t), which the above estimates give as k,/12k2.

13 Jul 2009: a = 0.62 (stress Y -“.38) for 4 = 20. ... References. 1 R. Keunings, J. Non-Newtonian Fluid Mech., 20 (1986) 209-226.

30 Nov 2009: 8. 7. 6. 5. 4. 3. 2. 1. 0. 10 20 30 40 50. ... Compared to the case of largem, more. 16. 10 20 30 40 50.

21 Jul 2009: This corresponds to particle Reynolds numbers in the range from 0.009 to 0.20, and the ratio of the sphere radius t o the pipe diameter a in the range

21 Jul 2009: 20, 111. ECKSTEIN, E. C. , BAILEY, D. G. & SHAPIRO, A.

17 Sep 2009: Penrose transform. In 1969, Penrose gave a formula for solutions to the wave equation inthe Minkowski space [20]:. ... Phys. 8 345–66[20] Penrose R 1969 Solutions of the zero-rest-mass equations J.

21 Jul 2009: We may then put. m = (2 - 20)/(1- 20) where D = E(0)/2X,. ... King and D.F. James, J. Chem. Phys., 78 (1983) 4749-4754. 20 G.

10 Jul 2009: fluctuations and hydrodynamdiffusivity with the size of the numerical box,@14 –17,20#. ... For each case studied, dynamic simulations were made foto 20 realizations with different initial configurations.

24 Aug 2009: equation (14); ---- , equation (15); --- , equation (1 6 ). Calculated values from Brenner & Weiss- man ( 1 9 7 2 ) : 0, o / D = 20; 17, w / D = 40. ... It can be seen t h a t the numerical results for w / D = 20 and o / D = 40 are satisfactorily tending

8 Jul 2009: 5. Energy budgetThe initial potential energy in the tall column is E0 =. 12πgr20 h. 20 (axisymmetric) and. 12gr0h. 20 (planar). If one were to use the shallow-water equations to describe ... E/E0Eq/E0Dµ/E0Dq/E0(EiEq – Dµ – Dq)/E0. 15 20 25 300 5 10

15 Oct 2009: mN. )Φ1. ψ2r. 2rψ2 F1 = 0, (1.20). 2mψ2. Φ1r. F2 = 0, (1.21). ... the function u in (1.4)), and(eliminating ψ2 between (1.20)-(1.21)) the function Φ1 approaches ϕ, a solution of the Newton-Schrödingersystem (1.4).

8 Jul 2009: Experiments are performed in a longsL = 4 md perspextube of internal diameterd= 20 mm, with a sliding gate inthe middle, that can be tilted at anglesu from 0 to ... More quantitative results are obtained by recording witha digital camera images of the