Search

5 Aug 2015: coli, with v 20 μm/s and τ 1 s, run 20 μm, but it can be considerably longer for otherbacteria [28]. ... 30, 235 (1971). [20] J. D. Murray, Mathematical Biology II Spatial Models andBiomedical Applications, 3rd ed.

22 Apr 2015: Fig. 6 shows thetrajectories of non-interacting pullers with a 0.8 swimmingtowards a sphere of size A 20. ... Fig. 8provides a general picture of the scattering dynamics, where wex the colloid size to A 20.

9 Nov 2015: We already have the Green’s function. solution to the homogeneous problem in (7.20), so we simply need to find a solution to. ... sin x. sin 1. 1. xf(ξ) sin(1 ξ) dξ (7.35). using the result (7.20). –

1 May 2015: Notice that higher temperatures induce unwantedcaramelization.20 The molten sugar is poured into a cylindrical Teflonmold (length 14 cm and inner diameter 2 cm) until it fills the entirebore volume (approximately ... Phys. Rev. E 2013, 87, 011003.(20)

30 May 2015: Forpolynomial reconstructions see [19] and [20]. IV. NUGS IN ONE DIMENSIONIn one dimension we take ZK R̂ to be the interval. ... Com-put. Phys., vol. 229, no. 3, pp. 933–946, 2010. [20] B.

31 Mar 2015: These satellites aretypically much smaller than the primary drop (20) and almostalways undesirable in applications (2). ... Nat Phys 5:697–702. 20. Collins RT, Harris MT, Basaran OA (2007) Breakup of electrified jets.

30 May 2015: Forpolynomial reconstructions see [19] and [20]. IV. NUGS IN ONE DIMENSIONIn one dimension we take ZK R̂ to be the interval. ... Com-put. Phys., vol. 229, no. 3, pp. 933–946, 2010. [20] B.

5 Feb 2015: Define some common functions for plotting.soma.rad <- 20/2 #20 um soma diameter.on.col <- "red"of.col <- "blue"show.on <- function(pts, main) {. symbols(pts, circles = rep(soma.rad,

9 Nov 2015: There are two real zeros.One is close to 0.2144 and the other is (up to 20 digits). ... V̇ CD̂V = F(t), U(0) = U0, (31) advectionnumv. 21. 25 20 15 10 5.

21 Jan 2015: The dimensionless form of the inequality (2.20) is. B < QF < Qmax BD1(1B). ... 1 20. 0.5. 1.0. 0 1 2 0 1 2 3.