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

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

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.

31 Jan 2012: ij. 12. ′′ij 18. ′′′ij. (24). Clearly therefore χij is equivalent to the positive Gij under the arbitrariness ex-pressed by (16).

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 G. Woodhouse and R. E. Goldstein (unpublished).[24] E. J. Hinch and L.

27 Jul 2012: the various coefficients appearing in (3.24), (3.25) depend on the dimensionless couplingsgi. ... 2 112Rφ2, but this may be compensated at zero loop order in (3.24).

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.

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.

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].

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.