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26 Jul 2013: F (r ) = C1 Iλ(kr ) C2 Kλ(kr ), (24). ... Applying the condition that p̂ is finite at r = 0 to equation (24)eliminates Kλ as a solution for F.

26 Jul 2013: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11.

29 May 2013: Although very dif-ferent in size and composition, these systems are oftenjointly termed ‘‘active’’ fluids, for which there is now arange of continuum theories [12,14–24]. ... 2(d)] we observe the linear scaling z Exy=2,with 24 m being roughly

11 Nov 2013: un1 = un t. 24(9Fn1 19Fn 5Fn1 Fn2). NB uses 1 function evaluation per step – goodNB difficult to start or change step size t – badNB Stable t.

26 Jul 2013: 24–26 The second type of surface, less stud-ied, is one where the solid is the continuous phase, and theliquid/air contact occurs on isolated domains Fig. ... whose solution is. f xns, f yns =An, Bn. 1 s21/2 1 s 1 , 24.

26 Jul 2013: The first type of model, termed sublayer modeling, con-siders the dynamics of individual cilia, either theoretically ina simplified fashion,4,5 or numerically with all hydrodynamicinteractions.24,25 The study ... 1. Ln x0, t2. x0 tdx0. 24. For a given

26 Jul 2013: Typicalvalues for b range from $%1 for bacteria like E. coli,6 $0for Volvox and artificially created squirmers17,24,27 to $þ1for Chlamydomonas.19.

26 Jul 2013: We also plot in Fig. 3 the results ofour model for both surface coverage considered in the twoprevious studies: = 0.43 dashed line and = 0.68 solidline.24.

17 Jul 2013: second fluid withoutthe membrane [23,24]. ... 174, 381 (1987).[24] K.SugiyamaandM.Sbragaglia,J.Eng.Math.62,35(2008).[25] F. G. Woodhouse and R. E. Goldstein, J.

26 Jul 2013: minima in the free energy see Ref. 24 for a textbook treat-ment. ... Rev. E 76,. 061914 2007.24 M. Kardar, Statistical Physics of Fields Cambridge University.

26 Jul 2013: we employ insteadthe full non-local SBT [24] to study the hydrodynamics ofthe superhelical swimmers. ... Þ. hþðh. (Þð%Þ. j Uþ(Vj=V. ðj U((Vj=VÞð%. Þ. Aedes. notoscriptus. 0.24.

4 Oct 2013: n2π2 1. (24). On the other hand we had in a previous example the expression constructed from homo-geneous solutions:. ... ξ. (25). Now comparing eqs (24,25) and viewing ξ as a parameter and x as the independentvariable, we see that the equivalence of

4 Oct 2013: u,Av) = (Bu,v) (24). (as you can easily check using the property that (Bu)† = u†B†). ... 36) of the µn values.). 1B Methods 24. 2.5 Parseval’s identity and least square approximations.

26 Jul 2013: 4. Experimental Section. Reagents and Solutions: Cupric sulfate pentahydrate, nickel(II) chloride hexahydrate, nickel(II) sulfamate tetrahydrate, gold (Oro-temp 24 RTU RACK) and silver (1025 RTU @ 4.5 Troy/gallon) ... HeLa cells were plated 24 h earlier

26 Jul 2013: Other avenues of current active research in-clude the swimming dynamics of bodies in non-Newtonianfluid environments, such as the propulsion of spermatozoa inthe human female reproductive tract.24–29. ... studied spermatozoa of the seaurchin

16 Oct 2013: m=1. α(m)(t)δmn. = α(n)(t) , (1.24). reproducing (1.23) apart from renaming the indices. ... 24. Chapter 2. 2. Groups. This chapter contains the second set of syllabus items, together with a fewitems anticipating the third set:.

3 Feb 2013: Photosynthetically Active Radiation (Fluora; OSRAM) and 10 h in dark at 24 C.Cells were harvested during the exponential growth phase. ... animal and plant functions. Science 318(5848):245–250.24. Fujiu K, Nakayama Y, Iida H, Sokabe M, Yoshimura K (2011

26 Jul 2013: See the article by Howard Berg, PHYSICSTODAY, January 2000, page 24.) The effect is not un-like a corkscrew pulling itself through the cork of awine bottle, except that the flagellum

26 Jul 2013: a). Re 29, onset of local absolute instability at x 1:24 (b) Re 47,onset of linear global instability, (c) Re 100, (d) Re 175, (e)Re 235, (f) Re

26 Jul 2013: mental22 or locomotive processes.23,24. aDepartment of Physics, University of California San Diego, 9500 GilmanDrive, La Jolla, CA, 92093-0354.