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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: 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.

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].

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.