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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.

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.

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.

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 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 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: 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.

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.

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)

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.

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%.

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.

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.

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.

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

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).

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.

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

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.

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)].

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.

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.

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.

19 Sep 2009: 2. 3. t. y(t) 0 5 10 15 20 25. 2. ... 20,0)pr,0. Moreover. L[p1,0] = 0L[p2,0] = 3bp0,0p21,0L[p3,0] = 6bp0,0p1,0p2,0 bp31,0. We can easily work out the initial values.

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

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

14 Jul 2009: E = π. 0. π/20. [L{Γ}ge(φ,θ; Γ). ]2sin θ dθ dφ. ... 20 L. C. Nitsche and E. J. Hinch. more vigorously than they are thrown back toward the centreline.

10 Jul 2009: a!, b!, c! Spatiotemporal diagrams obtained ford5 20 mm at asame density contrast At. ... Tube diameterd5 20 mm. The slope of the dashelines5 0.25 @see Eq.14!#.