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24 Feb 2012: E.J. Hinch, 24 February 2012. E.J. Hinch — Curriculum Vitae. 1968 B.A.

3 Oct 2012: Department of Applied Mathematics. and Theoretical Physics. Goldstein Lab. Teaching. DAMTP Summer School on Fluid Dynamics of Sustainability and the Environment. Supplementary Reading (Biological Physics). The following is a collection of primary

27 Aug 2012: h. 1. 992. 24:3. 13-3. 58. D. ownl. oade. d fr. ... u. R. ev. F. luid. Mec. h. 1. 992. 24:3. 13-3.

24 Sep 2012: September 24, 2012. 1. Complex fluids. What & where? tooth paste, soup, ketchup, synthetic fibres,. ... Normal stress (tension in streamlines) = shear stress γτ. 24. Tension in streamlines.

19 Oct 2012: Instead, we adopt a new approach by adapting aclosure of Hinch and Leal [24] to d 2, yielding. ... G. Woodhouse and R. E. Goldstein (unpublished).[24] E. J. Hinch and L.

19 Dec 2012: 24 • • 25. οργανώθηκε η κοινωνία μας τα τελευταία 40 χρόνια, αφετέ-ρου δε, της πληθώρας ευτελών μηνυμάτων που, με τη βοή-θεια Μέσων Μαζικής

20 Jun 2012: 24. Stabilisation of jets. Newtonian Jet. Non-Newtonian Jet (200ppm PEO). Hoyt & Taylor 1977 JFM.

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.

27 Dec 2012: 22]. Recent experimental evidence [24] is consistentwith the hypothesis of orbit flexibility and hydrodynamiccoupling as a possible origin of flagellar synchronization.At the same time, synchronization of an isolated pair is ... Custom-made rotation

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.

15 Oct 2012: Aspects of fermions in magnetic AdS geometries. have been previously discussed in [20, 21, 22, 23, 24].

23 Jan 2012: The explicit expressionfor 8 is given by (5.24) and is linear in the highest derivative y(7). ... Springer, Berlin (1995)24. Hitchin, N.: Complex manifolds and Einstein’s equations, in Twistor Geometry and Non-Linear systems.

3 Sep 2012: ThethroatdiameterD exhibitsanintriguingcrossover. R94 Invited Article. Figure 7. Collapse of the Möbius strip ‘throat’ [24]. ... c) Caustic visible from highly curvedsurface after the collapse of the Möbius strip surface [24].

16 May 2012: Furthermore, weknow that Eqs. (3.14) and (3.15) are equivalent to (3.24). ... Eqs. (3.14) and (3.15)are equivalent to (3.24). The integrability conditions force δ0 = 0.

13 Feb 2012: The reconstructed arc lengthscluster tightly around 24:50 0:05 cm (inset histogram), demonstrating the accuracy of the image processing and analysismethodology.

3 May 2012: 2. ]. 24. More termsMatching: main body region. Main body=. c2n3.

5 Sep 2012: 7.1. A new scheme of Dirichlet series for particular systems of the form(24). ... Byletting z = P 1y, the system (24) is equivalent to a transformed dynamical system.

22 Mar 2012: here some of them, [1, 7, 10, 11, 18–21, 23, 24, 26–28, 32, 33]. ... J. Phys. A 24(24),. 5751–5762 (1991). http://stacks.iop.org/0305-4470/24/575131. Ralston, A., Rabinowitz, P.: A First Course in Numerical Analysis, 2nd edn.

2 Sep 2012: 15 OCTOBER 2010. 168101-2. surface [23], as well as a particular case of the ‘‘squirmer’’model [24]. ... Natl. Acad. Sci. U.S.A. 103, 8315. (2006).[24] J. R. Blake, J.

19 Sep 2012: Materials and MethodsLive Imaging. Females were fattened on yeast for 16–24 h at 25 C. ... 24. Wolff K, Marenduzzo D, Cates ME (2012) Cytoplasmic streaming in plant cells: the roleof wall slip.

2 Sep 2012: 2Program in Applied Mathematics, University of Arizona, Tucson, Arizona 85721, USA(Received 23 December 2003; published 24 August 2004). ... Rev.Lett. 71, 3975 (1993). [24] P. N. Segre, E. Herbolzheimer, and P.

27 Aug 2012: 23). From (22) and (23)PJL. For a given power P and frequency / , equation (24) gives a maximum value ofuwhen ,X. ... the observed value is 24/14.

10 Oct 2012: Therefore, (3.24) follows.The term Q1 is estimated using the bound. |Q1| = G. ... Fiα(λF) >= A Fiα (F) and the estimation (in. the spirit of (3.24)).

3 Sep 2012: 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

2 Sep 2012: On time scales shorter than , effects associ-ated with spatiotemporal correlations in Q [23] intervene.For a drop [24] or a film [22] of size L, the tails will be cutoff ... Tu, Phys. Rev. E 64, 011902. (2001).[24] G.V. Soni et al., Biophys.

12 Sep 2012: In a preliminary work [23, 24] we explored some mor-phological aspects of the fracture profiles obtained inplane-plane debonding experiments performed with gran-ular adhesives (crushed sand in an acrylic ... Van Damme, Fractals 1, 968 (1993).24. H. Van

2 Sep 2012: On the other hand, recent advances frommicron-scale magnetically actuated tails [24] to syntheticmolecular rotors [25] now allow fabrication of arrays ofactive tails that can stir up the fluid. ... 2007); Small 4, 111 (2008).[24] R. Dreyfus et al.,

16 Jul 2012: λ1 1270.9 1103.4 1100.7 1099.8 1189.8λ2 26.39 48.24 46.37 44.92 28.13. ... 24] K. Frick, P. Marnitz, A. Munk, Statistical Multiresolution Estimation for Variational Imaging:With an Application in Poisson-Biophotonics, J.

2 Sep 2012: 24 OCTOBER 2008. 178102-3. [Fig. 4(b)] is dominated by a 1= dependence, leading to avery strong 3 scaling as the amplitude of the streamfunction approaches zero. ... G. Bessoth, A. J. deMello, and A. Manz, Anal. Commun. 36, 213 (1999).[24] J.

22 Mar 2012: Evolving ideas of the stationary phase approximation [24], ourmethodsrequire explicit availability of more terms in the asymptotic expansion, leadingto the assumptions of non singularity of the matrix Aω and smoothness of ... 637–655. 24. E. M. Stein,

2 Sep 2012: The data wedisplay in this article are for a dimensionless gap size / R= 0.24. ... 24. Assuming all balls are far apart, we again use the Oseenmodel, Eq.

2 Sep 2012: Onemilliliter of 24-h stock was added to 50 ml of TB and incubated for18 h. ... O. (1992) Annu. Rev. Fluid Mech. 24, 313–358.12. Hillesdon, A. J., Pedley, T.

6 Mar 2012: 24. More termsmain body. With h = c2n/3H,. (H Hxx )x = c2n/3G c(2n1)n/3. ... 24. More termsMatching: transition regions. Transition regions=. h0 h2 h3 h4 h5.

3 Sep 2012: 24). So, by substituting (24) into (23), we have that. (P2M2)P1M1ϕ2 lBM2.

2 Sep 2012: 4 A), representing either depletion or waste, alsoprovide spatially and temporally extended signals for the presenceof a colony, perhaps significant for intercolony communication, asin sexual induction (23) and quorum sensing (24), ... Michod, R. E. (2004

28 Feb 2012: 3.24) 2B2A4 2[(. κ2 2) 2. ]BA3 2 2. (κ2 2. ... Nevertheless, from (3.24) the Re 0 limit is observedto be consistent with (3.12) obtained for Re = 0 and M = 1.

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: 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.

21 Oct 2012: 2. ]. 24. More termsMatching: main body region. Main body=. c2n3.

20 Oct 2012: 3 Consistent reconstructions and oblique projections. We now consider the consistent sampling technique of [23, 24, 28, 55, 57]. ... An analysis of consistent reconstructions, which we shall recap and extend in 3.3, was given in[23, 24, 28].

2 Sep 2012: Rev. Fluid Mech. 24,313 (1992). [2] A. Einstein, Ann. Phys. (Leipzig) 17, 549 (1905).[3] P.

2 Sep 2012: A macroscopic scale model of bacterialflagellar bundlingMunJu Kim, James C. Bird, Annemarie J. Van Parys, Kenneth S. Breuer, and Thomas R. Powers. Division of Engineering, Brown University, Box D, Providence, RI 02912. Edited by Howard C. Berg,

2 Sep 2012: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11.

2 Sep 2012: 1B), where η is the viscosity, and the distance betweenthe forces (24, 25). ... sions. Chem Phys 375:557–567.24. Batchelor GK (1970) The stress system in a suspension of force-free particles.

17 Apr 2012: 21:. 22:. 23:. 24:. 25:. 26:. 27:. 28:. 29:. 30:. 31:.

2 Sep 2012: O. Kessler, Annu. Rev. Fluid Mech. 24,313 (1992). [2] N. A.

2 Sep 2012: 24,313 (1992). [2] W. F. Paxton et al., J. Am. Chem.

2 Sep 2012: Lipidmembranes do behave as two-dimensional f luids and can sup-port shear (24). ... Cole L, Orlovich DA, Ashford AE (1998) Fungal Genet Biol 24:86 –100.7.

2 Sep 2012: Rev. Fluid Mech. 24,. 313 (1992).[3] X.-L. Wu and A. Libchaber, Phys.

2 Sep 2012: reinhardtii). Similar confine-ment can also occur in biofilms and in cellular transport near freesurfaces (24, 25), as well as in thin, mucous layers over ciliatedepithelia, such as line the human ... Phys Rev Lett 105:188101. 24. Oliver JK, Willis BL