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5 Sep 2012: 49) , and open 3D bulk suspensions (7, 18,24, 25), bacteria were confined in closed microfluidic chambers to. ... 6. Berg HC (1997) Motile behavior of bacteria. Phys Today 53:24–29.7.

19 Jan 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J.

2 Sep 2012: 1B), where η is the viscosity, and the distance betweenthe forces (24, 25). ... 38. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

2 Sep 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J.

2 Sep 2012: Phys Rev Lett103:1981103. 15. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions. ... Phys Rev Lett 105:188101. 24. Oliver JK, Willis BL (1987) Coral-spawn slicks in the great barrier reef:

2 Sep 2012: Kachar & Reese 1989; Lichtscheidl & Balu ka 2000).Nevertheless, ‘relatively little is known about the biogene-sis, dynamics, maintenance, and inheritance of the organelleitself’ (Powell & Latterich 2000). ... al. 1999); and (v) thatthe actin

2 Sep 2012: solution to (24) subject to the boundary conditions is(Carslaw and Jaeger, 1959). ... computations. Fig. 2. The radial distribution function R0(r) for the parameter valuesP 1, N 8 , and Q 24.

2 Sep 2012: T̂ = N̂. 24. The curvature is the rate of rotation of T̂ about B̂, and. ... Comparison of Eqs. 21–24 reveals that2 =1. 2 22 and 3 = , where is the angle between.

27 Jul 2012: the various coefficients appearing in (3.24), (3.25) depend on the dimensionless couplingsgi. ... Thus we find. 2χei = Yi Ui iβjUj 12 (Vij Sij )βj θai ka. =

10 May 2012: 24. 2.2 Inverse scattering transform for KdV. 252.2.1 Direct scattering. 272.2.2 Properties of the scattering data. ... dx. 24. Figure 2.1: Sine–Gordon Kink. Kink. x. Note that the Sine–Gordon equations didn’t enter the discussion at this stage.