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10 Apr 2011: The expression forz, assuming wemay locally approximate actin as a cylinder@20# an addi-tional 1/2 in the denominator is neglected! ... Ott, and R. Goldstein, e-prin. cond-mat/9703244.@20# E. Guyon, J.-P. Hulin, and L.

10 Apr 2011: SwimmingFig. 2 was imaged at 20 magnification on a NikonTE2000U inverted microscope with an analog charge-coupled device CCD camera Sony XC-ST50, 30 fps,written to videotape, and digitized for ... RAPID COMMUNICATIONS. 030901-2. distances associated with

10 Apr 2011: 2] H. C. Berg and E. M. Purcell, Biophys. J. 20, 193 (1977).[3] J. ... Dombrowski et al. (to be published).[20] Somewhat similar patterns appear on agar substrates;.

10 Apr 2011: A. Barker, J. Chern. Phys. 20, 1526 (1952). 6G. N. Malcolm and J. ... TPP). The observation of narow bandwidth (20 cm -I) in IR spectra lead them to con-clude that the migration ofinner hydrogen atoms (see Fig.

14 Dec 2011: 86.4 cm dia.;. rotation. 20 rad/s (!). PV map and. dye map. ... Myers, and. Swinney,. Nature 1989. 86.4 cm dia.;. rotation. 20 rad/s (!). PV map and. dye map. near-identical. This is clearly. a strong jet:.

10 Apr 2011: Tin turn, modifies the relationship between the averagelocity U and the pressure so, for smallk, Uxx , px [20]. ... Tomotika, Proc. R. Soc. London A150, 322 (1932).[20] D. T. Papageorgiou, Phys.

14 Feb 2011: 0.381034 0 20 0 175.5 15.5 -0.482245 0.660473 0 21 0 183.5 15.5 -0.462795 0.842154 0 22 0 191.5 15.5 ... 5 -0.316616 0.961643 0 18 1 159.5 23.5 -0.375886 0.745553 0 19 1 167.5 23.5 -0.470441 0.734931 0 20 1

14 Feb 2011: 0.636345 0 20 0 175.5 15.5 0.080699 0.479536 0 21 0 183.5 15.5 0.141456 0.437615 0 22 0 191.5 15.5 ... 5 0.746923 0.732502 0 18 1 159.5 23.5 0.773595 0.728511 0 19 1 167.5 23.5 0.839741 0.578563 0 20 1

10 Apr 2011: a5. 20. cossvtd. 1 L 24s4 2 6ad sinsvtd 1 O sL 4d ,ytorque. ... Schliwa, J. Cell Sci.109,509 (1996). [20] R. E. Goldstein and S.

10 Apr 2011: a cell with some-thing like 20 nm resolution: it is unbelievablychock full of objects! ... I was stunned: how couldsomething so small 20 µm be so complex,and how did all the parts communicate witheach other?

10 Apr 2011: S0031-9007(98)0624. PACS numbers: 87.10. e, 02.40. – k, 03.40.Dz, 36.20.Ey. dts. ... F. Edwards,The Theory of PolymerDynamics(Oxford University Press, New York, 1986). [20] G.

20 Jan 2011: U = (1 e2τ c2), (2.20)where c is a local function on M independent of τ. ... Solution (3.2) can be obtained as an analytic continuation of the Kastor–Traschencosmological black holes [20].

10 Apr 2011: At eachlight intensity, the organism was stimulated with 20 periodsbefore the recording began, and the response was recorded for. ... For each viscosity andpopulation, we measured ωr for 20 colonies. Details of the Mathematical Model.

10 Apr 2011: 4) with artificially produced chemical wavescontrollable shape and velocity [20], complementaryrecent experiments with fixed gradients [21] and timvarying uniform concentrations [10]. ... Prost, Nat. (London) 370, 447 (1994).[20] R. H. Austin (private

10 Apr 2011: a) Growthvelocity vc versus pH, using CO2 partial pressure in the caveatmosphere of 3 104 atm, a temperature of 20 C, (i) Ca2of 100 ppm and volumetric fluid flow Q 2 ... For a more precisecomparison, we extracted the contours of 20 stalactitesby a

10 Apr 2011: Vt Czr. Vss 11. zrs 3 rss? fs. (4). The second term of (4) is nonzero [20] when the filamentis both out of elastic equilibrium f fi 0 and either ... Rubinow, J. Fluid Mech. 44, 705 (1976).[20] The writhe-tracking term is rs 3 rss?

10 Apr 2011: b) Enhancement of fluxthrough a circular region near the cell wall due to fluid flow for various valuesof the Péclet number (0, 10, 20, 50,. , ... Wink M (1993) J Exp Bot 44:231–246.20. Martinoia E, Maeshima M, Neuhaus HE (2007) J Exp Bot

10 Apr 2011: This suggests that the formation of a cenis not simply a characteristic of a subpopulation of cebut rather is determined in part by cell-cell interactio[20]. ... 20] P. M. Glazer and P. C. Newell, J. Gen. Microbiol.125, 221(1981).

10 Apr 2011: We found that tubes would begin growing within 20 min if theinitial value of r was 0.08 – 0.16. ... 20. Bigham, J. M. & Touvinen O. H. (1985) in Planetary Ecology, eds.

10 Apr 2011: 2005; 74, 031915 2006.20 T. B. Liverpool and M. C. Marchetti, Phys. ... 3.65 3.7 3.75ρ0. 0. 5. 10. 15. 20. 25. L. ρc.

10 Apr 2011: Colloid Surface A 323:123–131. 20. Turitsyn KS, Lai L, Zhang WW (2009) Asymmetric disconnection of an underwater airbubble: Persistent neck vibrations evolve into a smooth contact. ... RevMath Pures Appl 4:5–20. 25. Călugăreanu G (1961) Sur les

10 Apr 2011: carteri(18–20), fluid inertia is negligible and the flagella-induced flowis a direct measure of the flagellar activity. ... Proc Natl Acad Sci USA 103:8315–8319. 20. Drescher K, et al.

10 Apr 2011: An examination of the 20 amino acids found in living matter reveals that their mass is typically100 Da. ... them is 109/(2 104 2000 s) 20 s1, as shown in (b), andwhich roughly corresponds to the experimentally established value.

10 Apr 2011: V. carteri was synchronized in 20-ml test tubes with airbubbling, standard Volvox medium (33), and homogeneous coolwhite light [1,000 footcandles (1 footcandle 20.76 lx)]. ... C. & Purcell, E. M. (1977) Biophys. J. 20, 193–219.26. Keller, E.

10 Apr 2011: We consider themotion of colonies within a noninteracting ‘‘ideal gas’’model [20] which, despite its simplicity, gives satisfactoryagreement with the experiment; the fluid is unbounded, theswimmers are confined to a rectangular ... Drescher, K.

10 Apr 2011: limy0. mh′(x′) = ψ(x),. limy0. mh′′(x′′) = ψ (x) (20). and the density ρ can be easily verified to be given by ρ = ψ ψ. ... Mod. Phys. 20 367–87[7] Feynman R 1951 An operator calculus having applications in quantum electrodynamics Phys

10 Apr 2011: 4d and movie 4. The downward plume’s velocity isabout 10 – 20 m / s. ... See also movie5 in 20. SOKOLOV et al. PHYSICAL REVIEW E 80, 031903 2009.

10 Apr 2011: However, the shapes of the fingers, their remarkablywell-defined widths between 20 and 50 m, and their depen-dence on the substrate temperature were not obtained explic-itly in this earlier ... In order to observe the instability, 1.7 For amagnetic field

10 Apr 2011: A. Chandrasekaran et al., Nat. Biotechnol. 26, 107. (2008).20. V. Soundararajan et al., Nat. ... The dashed vertical line represents theintrinsic frequency difference observed in cell models (20).

10 Apr 2011: Recently Szleifer et al. [20] presented a statistical thermodynamic theory to explain the decrease of the bending elastic modulus upon replace- ment of a fraction of the long chains by shorter ... Electrolyte concentration (M). 0.01 0.02 0.05 0.10 0.20

10 Apr 2011: mU 20 /V0) 1) we can define the following dimensionless quantity, the Shelleynumber:. ... We do so by using the canonical change of variables givenby (20), so that.

23 Feb 2011: σ/N vs t/N2 (Rouse). Short times finite. 0.1. 1. 0 5 10 15 20.

14 Feb 2011: 0.301235 0 20 0 175.5 15.5 -0.143051 0.450492 0 21 0 183.5 15.5 -0.33389 0.431915 0 22 0 191.5 15.5 ... 5 0.043539 -0.014242 0 18 1 159.5 23.5 -0.0134359 0.0919865 0 19 1 167.5 23.5 0.0627316 0.147985 0 20 1

14 Feb 2011: 0.13211 0 20 0 175.5 15.5 0.0666464 0.365959 0 21 0 183.5 15.5 0.177715 0.638453 0 22 0 191.5 15.5 ... 5 0.150711 -0.150862 0 18 1 159.5 23.5 -0.00791379 -0.0660623 0 19 1 167.5 23.5 -0.0513637 0.10727 0 20 1

14 Feb 2011: 1.05988 0 20 0 175.5 15.5 0.624214 0.942312 0 21 0 183.5 15.5 0.538496 0.913936 0 22 0 191.5 15.5 ... 5 -0.10752 0.847604 0 18 1 159.5 23.5 0.152793 0.950005 0 19 1 167.5 23.5 0.393126 0.969928 0 20 1

14 Feb 2011: 0.151468 0 20 0 175.5 15.5 -0.930939 -0.0264941 0 21 0 183.5 15.5 -1.04152 0.133211 0 22 0 191.5 15.5 ... 5 -0.877919 -0.188921 0 18 1 159.5 23.5 -0.812542 -0.215161 0 19 1 167.5 23.5 -0.792198 -0.278359 0 20 1

14 Feb 2011: 1.00213 0 20 0 175.5 15.5 -0.056326 0.872868 0 21 0 183.5 15.5 0.056367 0.33225 0 22 0 191.5 15.5 ... 5 0.324436 0.964582 0 18 1 159.5 23.5 0.317599 0.97583 0 19 1 167.5 23.5 0.216859 1.01212 0 20 1

14 Feb 2011: 1.1349 0 20 0 175.5 15.5 0.321468 1.0736 0 21 0 183.5 15.5 0.386148 0.912148 0 22 0 191.5 15.5 ... 5 0.119709 0.762242 0 18 1 159.5 23.5 0.192348 0.99978 0 19 1 167.5 23.5 0.272276 1.12541 0 20 1

14 Feb 2011: 0.912465 0 20 0 175.5 15.5 0.478221 0.93301 0 21 0 183.5 15.5 0.380002 0.931476 0 22 0 191.5 15.5 ... 5 0.379722 0.724791 0 18 1 159.5 23.5 0.404805 0.660128 0 19 1 167.5 23.5 0.639609 0.801639 0 20 1

14 Feb 2011: 1.05099 0 20 0 175.5 15.5 0.46974 0.768858 0 21 0 183.5 15.5 0.381097 0.69793 0 22 0 191.5 15.5 ... 5 0.102586 1.12121 0 18 1 159.5 23.5 0.302539 1.09455 0 19 1 167.5 23.5 0.593112 0.92331 0 20 1

14 Feb 2011: 0.744591 0 20 0 175.5 15.5 0.270967 0.741916 0 21 0 183.5 15.5 0.21869 0.638322 0 22 0 191.5 15.5 ... 5 0.38091 0.813985 0 18 1 159.5 23.5 0.486496 0.694853 0 19 1 167.5 23.5 0.37697 0.687171 0 20 1

14 Feb 2011: 0.834156 0 20 0 175.5 15.5 0.344188 0.663663 0 21 0 183.5 15.5 0.233853 0.581521 0 22 0 191.5 15.5 ... 5 0.622901 0.938816 0 18 1 159.5 23.5 0.583384 0.858902 0 19 1 167.5 23.5 0.586658 0.615734 0 20 1

14 Feb 2011: 0.461786 0 20 0 175.5 15.5 0.356437 0.219798 0 21 0 183.5 15.5 0.235042 0.0493363 0 22 0 191.5 15.5 ... 5 0.431447 0.896386 0 18 1 159.5 23.5 0.45025 0.828354 0 19 1 167.5 23.5 0.723953 0.586477 0 20 1

14 Feb 2011: 0.445455 0 20 0 175.5 15.5 0.336337 0.267822 0 21 0 183.5 15.5 0.237421 0.0177448 0 22 0 191.5 15.5 ... 5 0.29934 0.560707 0 18 1 159.5 23.5 0.472969 0.627417 0 19 1 167.5 23.5 1.05941 0.524177 0 20 1

14 Feb 2011: 0.631629 0 20 0 175.5 15.5 0.0144695 0.435807 0 21 0 183.5 15.5 0.096276 0.307003 0 22 0 191.5 15.5 ... 5 0.261833 0.886844 0 18 1 159.5 23.5 0.497466 0.765129 0 19 1 167.5 23.5 0.603043 0.4535 0 20 1

14 Feb 2011: 0.246806 0 20 0 175.5 15.5 -0.0184821 0.200944 0 21 0 183.5 15.5 0.19374 0.275617 0 22 0 191.5 15.5 ... 5 0.15709 1.17497 0 18 1 159.5 23.5 0.11643 0.708492 0 19 1 167.5 23.5 0.347185 0.285254 0 20 1

14 Feb 2011: 0.43388 0 20 0 175.5 15.5 0.0337572 0.592916 0 21 0 183.5 15.5 0.233953 0.592298 0 22 0 191.5 15.5 ... 5 0.111855 0.659229 0 18 1 159.5 23.5 0.305167 0.595087 0 19 1 167.5 23.5 0.337357 0.607351 0 20 1

14 Feb 2011: 0.693216 0 20 0 175.5 15.5 0.014696 0.563245 0 21 0 183.5 15.5 0.0263186 0.489598 0 22 0 191.5 15.5 ... 5 -0.140485 0.779295 0 18 1 159.5 23.5 0.112082 0.615701 0 19 1 167.5 23.5 0.0560559 0.658591 0 20 1

14 Feb 2011: 0.137188 0 20 0 175.5 15.5 -0.108146 0.248575 0 21 0 183.5 15.5 0.235509 0.239217 0 22 0 191.5 15.5 ... 5 -0.351883 0.780339 0 18 1 159.5 23.5 -0.0519843 0.396896 0 19 1 167.5 23.5 0.0923328 0.24042 0 20 1

14 Feb 2011: 0.0787456 0 20 0 175.5 15.5 0.0468984 0.0264737 0 21 0 183.5 15.5 0.169941 -0.137999 0 22 0 191.5 15.5 ... 5 -0.120662 0.744875 0 18 1 159.5 23.5 0.114093 0.323688 0 19 1 167.5 23.5 0.192553 0.12101 0 20 1