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14 Feb 2011: 0.0635388 0.532321 0 23 0 199.5 15.5 -0.0986939 0.69175 0 24 0 207.5 15.5 -0.419911 0.673265 0 25 0 215.5 ... 1 199.5 23.5 -0.0742271 0.746095 0 24 1 207.5 23.5 -0.236922 0.781727 0 25 1 215.5 23.5 -0.319311 0.835675

10 Apr 2011: 24 APRIL 2009. 0031-9007=09=102(16)=168101(4) 168101-1 2009 The American Physical Society. ... 1) may be reduced, in rescaled coordinates r r=hand t tF=h2 with h R, to [24].

10 Apr 2011: 15 OCTOBER 2010. 168101-2. surface [23], as well as a particular case of the ‘‘squirmer’’model [24]. ... Natl. Acad. Sci. U.S.A. 103, 8315. (2006).[24] J. R. Blake, J.

10 Apr 2011: www.sciencemag.org SCIENCE VOL 325 24 JULY 2009 489. REPORTS. on. July. ... 24 JULY 2009 VOL 325 SCIENCE www.sciencemag.org490. REPORTS. on. July. 24,.

10 Apr 2011: J. Colloid Interface Sci. 1981, 81, 531-535.(24) Adler, P. M. J. ... Scale bar is 2 mm. Letters Langmuir, Vol. 21, No. 24, 2005 10917.

10 Apr 2011: 24 OCTOBER 2008. 178102-3. [Fig. 4(b)] is dominated by a 1= dependence, leading to avery strong 3 scaling as the amplitude of the streamfunction approaches zero. ... G. Bessoth, A. J. deMello, and A. Manz, Anal. Commun. 36, 213 (1999).[24] J.

10 Apr 2011: An estimate of the hydrodynamic coupling between twoidealized flagella [24] is est ’ rRL. ... E.Goldstein, Science 325, 487 (2009). [24] T. Niedermayer, B. Eckhardt, and P.

10 Apr 2011: 24). 232 A I Pesci et al. where we have used the notation i /xi. ... The equationof motion for u can be recast in the form (24) by taking its gradient and then replacing.

10 Apr 2011: xj ij4s 1 Gas 2 1jsss. (10). Numerical solution [24] of (10) yields a critical valueac 8.9G [confirming dimensional analysis of Eq. ... Mod. Phys. 65, 851. (1993).[24] W. H. Press, W. T. Vetterling, S.

10 Apr 2011: sequences, or, alternatively, specified endpoint positions or lateral constraints, can be explored to ex-amine the internal relaxation rates of the intrinsic curvaturesand the long-time dynamics of buckled shapes 24. ... Soc. Edinburgh, Sect. A: Math. 99,

10 Apr 2011: Using magnetic beads [24], the flagellummay be rotated, permitting full examination of flagellarresponses to fluid drags and applied torques. ... J. 74, 1043 (1998).[23] D. Coombs, Ph.D. thesis, University of Arizona, 2001.[24] T.

10 Apr 2011: With small modifications,this experiment can include baroclinic effects, providing asimple model to address mixing in oceanic flows, such asgravity currents along undersea canyons [24]. ... R. Powers, Phys. Rev. E 69, 061910 (2004).[24] R. H. Kase, J.

10 Apr 2011: Moreover, the torsion dynamicis problematical at inflection points, wherek 0. The curve dynamics can be drastically simplified butilizing Hasimoto’s transformation [24] relating vortexfilament motion to the nonlinear Schrödinger equatioDefine the

10 Apr 2011: This and oobservations (e.g., of slow stress relaxation [24]) stronsuggest a dominant dissipative mechanismwithin the fila-ment, characterized by a very much largerzr. ... Chem. Phys.70, 2991. (1979); J. M. Schurr, Chem. Phys.84, 71 (1984).[24] J.

10 Apr 2011: The wires of [23, 24]are of finite length and attached to electrodes at either end. ... Our results may also be relevant to explain the observed stability of gold wires with largerradii [23, 24].

28 Apr 2011: 6] T. Levi-Civita, Ann. Math. 24, 255 (1896).[7] V. Koisak and V.

30 Sep 2011: CR strain CC124 [12] was grown axenically in tris-acetate-phosphate medium [11] in a growth chamber(Binder, Germany) set to 24 C and a cycle of 16 h lightat 100 ... Nikaido, J. Cell Sci. 109, 57 (1996). [24] M. A. Silverman and M.

10 Apr 2011: minimize overestimation of the trap stiffness. The calibration images were. reduced to remove optical and electronic noise (23) using Image J (24). ... for more details). The effective bending modulus found using. this fitting procedure is 42 24 pN mm2.

10 Apr 2011: To this end, substitute the constitutive relation(22) into the moment balanceequation (24)tofind the forceF on a cross-section:. ... C3. s= ζRω3. (31). The unknown functionΛ(s, t) occurs inEq. (30)because the moment balanceequation (24)does not

10 Apr 2011: xnpm n,m. Bnm1. 2n. nk=0. (n. k. )x̂nk(p̂mx̂k), (21). which is the correspondence obtained by using the operator ordering rule first introduced byWeyl [24]. ... Natl Acad. Sci. USA 18 674–6[24] Weyl H 1927 Z. Phys.

26 Mar 2011: This was conjectured by Slepian [20]. Asecond proof of this result is in [24]. ... 24] H. Widom, On a class of integral operators with discontinuous symbol.

27 Nov 2011: Experiments were done at 24.0C and16.2C, with initial speeds indicating operation well into thehigh-speed, low-torque regime. ... Fig. 3. (a) Data from five bacteria at 24.0C were plotted on the same graph andmarked with different symbols (with the data

10 Apr 2011: 1 1 1 Tc- T t=.-A----A--= A (24). C (0) f3tPl (0) f3ctPl (0) Tc. ... J(r) = 21TV3 fer) , f>. (44). (45). where f = (1/4 )(r/a)4 - (1/24 )(r/a) 6 for r<2a, and f = 4/3 for r>2a.

10 Apr 2011: Each 24 mm3 18 mm image was obtained by subtracting twsuccessive images taken 30 sec. ... Mikhailov, Foundations of Synergetics I(Springer-Verlag, New York, 1994). [24] J. Buck, Q.

10 Apr 2011: 24! The Bessel functionK 0(r /Ae) cancels the logarithmic divergence of the ln(r) term of the inner solution. ... Seifert, Adv. Phys.46, 13 1997!@24# B. Alberts, Molecular Biology of the Cell, 3rd ed.

22 Nov 2011: Unlike with the latter, the estimates(22) and (24) both decrease as M1 increases. ... IEEE Trans. Signal Process., 57(8):2986–2997, 2009. [24] Y. C. Eldar and T.

14 Jun 2011: Received 24 November 2010; revised manuscript received 31 March 2011; published 14 June 2011). ... A two-phasemodel [24] exhibits the chaotic character of the collectivebacterial swimming.

10 Apr 2011: A 1981, 24, 2203. scaling law equation of state like that postulated by Mermin and Rehr, eq 3.2, with the revised thermal scaling field T t wh, to leading order ... E 1981,23, 6157. (24) Reatto, L.; Tau, M. Europhys. L e t t.

10 Apr 2011: As the lower values of viscosity ratio are approachthe boundary integral method eventually fails to consevolume.24 In Fig.

6 Jul 2011: Annu Rev Fluid Mech 24:313–358. 2. Aranson IS, Sokolov A, Kessler JO, Goldstein RE (2007) Model for dynamical coherencein thin films of self-propelled microorganisms.

10 Apr 2011: 92, No. 24, 1988 Letters. Bessel functions of ith order. Finally, with spherical symmetry one has.

25 Nov 2011: It considers a forcing term that is oscillatory in space. tu = 2x b sin ωx, (3.24). ... 2t cos ω xbeω2t sin ω,. 21. Figure 3.1: The solution of (3.24) for different values of ω.

27 Sep 2011: 2004) to identify missing intronsin poor gene models, and 3) Pfam (24.0) analysis (Finn et al.2008) to identify conserved functional domains in eachprotein (METE: PF01717, PF08267; METH:PF02965,PF02965,

1 Sep 2011: F0 = 1 < F2 =π2. 8< < 4. π< < F3 =. π3. 24< F1 =. π. 2. In this section we obtain a difference analogue of the Bohr-Favard inequality in theform. ... 1. 24. ]= 1. 325. 192. 1. α4. With α = 1 and α = 2, we obtain c4(πn ) =. 517192. = 2.6927, and c4

10 Apr 2011: simplifying assumptions (a), (b) above [24]. While our physical picture and conclusions aredifferent from theirs, we are indebted to them for emphasizing these issues. ... The late-time asymptotics have been studiedby Granek and Olami [24].). What is the

10 Apr 2011: f1. t+. dxdt. f1x. dpdt. f1p. (24). This symmetry is most apparent in the new variables, and translates into the fact thatequations (22) and (23) can be satisfied up to O(

10 Apr 2011: The identity22,23,24. exp[ -A3({P})]. = exp[ - A 3 ( {81M}) ]exp(f dr J(r) p (r») I J= 0' (2.22). ... f/Jc. where the N independent amplitude is. 1 (w) _ '24 [g2(X) p/2 1/2 -yk ()[ ()]1/2 gl X -g4 X.

1 Sep 2011: up to the sign we obtaina11 = a22 = k; a12 = 1:From (12.3) we have a21 = k1k1 k0k 10 = k2 1;i.e., A = (1)k1 24 k 1k2 1 k ... 24. 19. ConclusionIt is clear that the above MAPLE algorithm may help to verify de Boor's conjecture only for particularvalues m.

30 Sep 2011: CR strain CC124 [12] was grown axenically in tris-acetate-phosphate medium [11] in a growth chamber(Binder, Germany) set to 24 C and a cycle of 16 h lightat 100 ... Nikaido, J. Cell Sci. 109, 57 (1996). [24] M. A. Silverman and M.

10 Oct 2011: and. 2β.αβ.β. = 2|α||β|. cos θ Z (1-24). Taking the product we find that 4 cos2 θ Z. ... 24. The Cartan subalgebra H can be taken to be the traceless diagonal matrices; there aren(n 1) roots associated with the Ei,j for i ̸= j.

10 Apr 2011: 2 Ok5k1. 0ka!0# kk4. e2k4t (24). Evaluating the first few integrals, we find forh# k, h# k1. ... A 5zL4. tk1. 24 (54). whereas the rodlike treatment implies (from Eq.

10 Apr 2011: V R! 26aa0. 5. R6. 24! Expressing this result in terms of the electric polarizabilvia. ... Thus the van deWaals potential assumes the form. V R! 24.

10 Apr 2011: Bt/JI= M , (24) t/JI Bt/J t/J(Mn). and a further differentiation then gives. ... 4. Clearly, a steepest-descent approximation should be valid for that part of the distribution near the region of the mini-mum at n 'Z 24.

5 Aug 2011: N2 ratio of the atmosphere [24]. ... Science 309, 1714–1717. (doi:10.1126/science.1115193). 24 Manning, A. C. & Keeling, R.

6 Oct 2011: 1 7 X 102 1.60 2. 2 5 2.92 3.24 3.59 9. ... 6 2 X 1 0 -1 1.10 1.24 1. 3 7 X 1 0 1 3.

2 Nov 2011: Generalized sampling and infinite-dimensionalcompressed sensing. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd,

3 Dec 2011: Generalized Sampling: Extension to Frames and Inverse andIll-Posed Problems. Ben Adcock Anders C. Hansen † Evelyn Herrholz ‡ Gerd Teschke‡. Abstract. Generalized sampling is new framework for sampling and reconstruction in

10 Apr 2011: a. Dd!1/2. h F pln 0.56/h!G1/2. 3.24! B. Energy of a straight-lamina model. ... detail elsewhere in the context of clorelated models,22–24,26,27,30we do not repeat them here.

10 Apr 2011: 2 Ok5k1. 0ka!0# kk4. e2k4t (24). Evaluating the first few integrals, we find forh# k, h# k1. ... A 5zL4. tk1. 24 (54). whereas the rodlike treatment implies (from Eq.

10 Apr 2011: PHYSICS OF FLUIDS 17, 083101 2005. Stalactite growth as a free-boundary problemMartin B. ShortDepartment of Physics, University of Arizona, Tucson, Arizona 85721. James C. BaygentsDepartment of Chemical and Environmental Engineering and Program in