Search

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: 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: 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: 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].

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: 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.

20 Jan 2011: American University ofBeirut, Beirut, Lebanon5 The Mathematical Institute, Oxford University, 24–29 St Giles, Oxford OX1 3LB, UK. ... Substituting (2.24) into (2.23) gives the system (2.18) for the1-forms ei.

10 Apr 2011: microscope stage at 24 C. ... See [3]. [16] J. Lighthill, Mathematical Biofluiddynamics (SIAM,Philadelphia, 1975). [17] Fiber density at 24 C in TB is 1.015 gcm3 from thesedimentation velocity y 29R2Drgh of fiber-ballstructures of

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: 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: 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: 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: 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

11 Dec 2011: Prolongation II. k (Jk1(S2(TU))) (Jk(Pr(U))) (ker σk) obstructions0 9 4 5 01 18 12 6 02 30 24 6 03 45 40 5 04 63 60 3

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.

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: 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: 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.

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,

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

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,

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.

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.

10 Apr 2011: 0.947 1.422 0.380 0.589. 291.155 265.827 31.473 24.649 3.488 6.172. 3626.522 116.233 18.702 14.883 2.529

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

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

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: 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.

14 Feb 2011: 0.0997679 0.0314839 0 23 0 199.5 15.5 0.155559 -0.167651 0 24 0 207.5 15.5 -0.00544606 -0.227898 0 25 0 215.5 ... 1 199.5 23.5 0.610019 0.125893 0 24 1 207.5 23.5 0.668408 0.386805 0 25 1 215.5 23.5 0.565238 0.810526

24 Aug 2011: on August 24, 2011rsif.royalsocietypublishing.orgDownloaded from. J. R. Soc. Interface (2011) 8, 1409–1417. ... 36 h. 12 h6 h 18 h. 24 h48/0 h. 42 h.

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: This argument is similar in spiritto that posed by Levinthal and Crane [24] in the con-text of DNA transcription. ... Hohenberg, Physica (Amster-dam) 56D, 303 (1992). [24] C. Levinthal and H.

10 Apr 2011: LabVIEW wasused to trigger the camera and control the LED light intensity time series.The temperature in the sample chamber was 24.5 0.5 C. ... Trends Cell Biol4:305–310. 24. Friedrich BM, Jülicher F (2007) Chemotaxis of sperm cells.

10 Apr 2011: The last term in Eq. 1 describesthe coupling to strain rate tensor E Exy = xvy yvx 21,24.Our further analysis shows that while this term has somequantitative effect, e.g., ... F. Edwards, The Theory of Polymer DynamicsClarendon Press, Oxford, 1988. 24 N.

10 Apr 2011: The electrostatic contribution was first determined by Odijk [24] and independently by Skolnick and Fixman [25] in the Debye- Hiickel approximation. ... 23). (24). H.N.W. Lekkerkerker I Curvature elasticity o f charged monolayers 325.

10 Apr 2011: J Fluid Mech 647:201–219. 24. Călugăreanu G (1959) L’intégral de Gauss et l’analyse des noeuds tridimensionnels. ... Jordan arcs and prescribed surfaces. Proc Natl Acad Sci USA 24:97–101.33.

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.

6 Jul 2011: 1B), where η is the viscosity, and the distance betweenthe forces (24, 25). ... sions. Chem Phys 375:557–567.24. Batchelor GK (1970) The stress system in a suspension of force-free particles.

10 Apr 2011: Onemilliliter of 24-h stock was added to 50 ml of TB and incubated for18 h. ... O. (1992) Annu. Rev. Fluid Mech. 24, 313–358.12. Hillesdon, A. J., Pedley, T.

10 Apr 2011: This canmodify significantly the rate of transport to an absorbing surface(24) and modify the hang time (25). ... 1976) Nature 259, 200 –201.24. Acrivos, A. & Taylor, T. D.

10 Apr 2011: 4 A), representing either depletion or waste, alsoprovide spatially and temporally extended signals for the presenceof a colony, perhaps significant for intercolony communication, asin sexual induction (23) and quorum sensing (24), ... Michod, R. E. (2004

10 Apr 2011: O. Kessler, Annu. Rev. Fluid Mech. 24, 313. 1992.5 C. Dombrowski, L. ... R. Soc. London, Ser. A 219, 186 1953;. 223, 446 1954.24 B.

10 Apr 2011: The ratio of theseadvective and diffusive terms, or equivalently the ratio of thediffusion time L2D to the advective time LU, then defines thePeclet number (24),. ... 23. Wu, X.-L. & Libchaber, A. (2000) Phys. Rev. Lett. 84, 3017–3020.24.

10 Apr 2011: barberi have a deriveddevelopmental programme and perform binary fissionto produce daughter colonies [13,23,24]. ... 36 h. 12 h6 h 18 h. 24 h48/0 h. 42 h.

10 Apr 2011: Therefore, we expect the MSC to describe fronpropagation at smalla if it applies at all [24]. ... 23] H. Lamb, Hydrodynamics(Cambridge University Press,Cambridge, England, 1993), 6th ed. [24] Preliminary numerical studies by D.

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.

14 Feb 2011: 0.656853 0.108999 0 23 0 199.5 15.5 0.708149 0.112969 0 24 0 207.5 15.5 0.908188 -0.0192405 0 25 0 215.5 ... 1 199.5 23.5 0.808678 -0.164453 0 24 1 207.5 23.5 0.955868 -0.206018 0 25 1 215.5 23.5 0.975417 -0.280142

10 Apr 2011: 2Program in Applied Mathematics, University of Arizona, Tucson, Arizona 85721, USA(Received 23 December 2003; published 24 August 2004). ... Rev.Lett. 71, 3975 (1993). [24] P. N. Segre, E. Herbolzheimer, and P.

10 Apr 2011: This progression along the “devel-opmental path” [24] can work on a global scale to breakthe symmetry of circular waves, either by competition witha postulated third wave [19], tuning of the ... 24] A. Goldbeter and L. A. Segel, Differentiation 17,