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2 Sep 2012: 68). At t = t 2 let the new position of the b o u n d a r y be z = (t2); therefore 0[(t2) , t2]----0. ... Otherwise, a new guess for the b o u n d a r y position must be m a d e and the problem re-integrated from t = t.

2 Sep 2012: ica Educational Corporation, New York, 1966).[4] Sir J. Lighthill, Mathematical Biofluiddynamics(SIAM,. ... 18] L. Landau and L. Lifshitz,Theory of Elasticity(Pergamon,New York, 1986), p.

2 Sep 2012: Alberts et al., Molecular Biology of the Cell (Garland,. New York, 2002).[4] R. ... Bray, Cell Movements (Garland, New York, 2001), 2nded. [12] M. Fontes and D.

2 Sep 2012: Acad. Sci. U.S.A. 94, 11307 1997. 3H. C. Berg, E. coli in Motion Springer-Verlag, New York, 2004.4D. ... Rev. Fluid Mech. 9, 339 1977. 16S. Camalet and F. Julicher, “Generic aspects of axonemal beating,” New J.Phys.

27 Aug 2012: New York: McGraw Hill.PRTNOLE, J. W. S. (1957). Myogenic Rhythms. In Recent Advances in Invertebrate Physiology,.

28 Feb 2012: However, contemporary physicsresearch leads to a number of new and important computational challenges. ... Davis, P. J. & Rabinowitz, P. (1975), Methods of Numerical Integration, AcademicPress, New York.

2 Sep 2012: A. Shapiro and M.Dworkin (Oxford University Press, New York, 1997),p. 417.

5 Sep 2012: Some discussion and a numerical experiment areaccordingly carried out for the new Dirichlet approximation. ... Theorem 7.2. Denoting the truncation of the new Dirichlet series (30) by.

29 Apr 2012: Examples from twistor theory/algebraic geometry. Mixture of old and new: Classical invariant theory (Young, Sylvester),algebraic geometry, twistor theory (Penrose, Hitchin).

2 Sep 2012: To derive it, first wereparametrize the trajectory by the new phase variable ðÞ that makes the intrinsic phase velocity con-stant: 0ðÞ FðÞ=jR0ðÞj 2=T. ... 17] Y. Kuramoto, Chemical Oscillations, Waves, andTurbulence (Springer, New York, 1984).

2 Sep 2012: The new ele-ment in this configuration may be a steady attractive(orrepulsive) force between the two helices.

2 Sep 2012: Hoffmann (Springer-Verlag,New York, 1990); B. L. Partridge, Sci. Am. 246, No.

3 Sep 2012: This relaxation process is quite rapid, and is ultimately constrained by the topologyof the knot: the wire cannot self-intersect, but in its new equilibrium state makes contact withitself at several ... The wire then finds a new equilibrium, subject now

2 Sep 2012: Our hope isthat modern microscopy and imaging techniques. will produce novel insights into phase dynamics andinspire a new class of models that allow quantitativecomparisons between theory and experiments. ... Dworkin, eds.,Oxford U. Press, New York (1997

2 Sep 2012: Then, the director is randomized on the thin-ning spiral arm, which collapses and proliferates a cascadeof new defects.Thermal fluctuations.—We then introduce the ther-. ... Soc. 70, 303 (1971).[28] Y. Kuramoto, Chemical Oscillations, Waves, and.

2 Sep 2012: New microfluidic methods exploiting the rota-tional streaming paradigm may be of significant interest.

2 Sep 2012: Y.-T.,. Brokaw, C. J. & Brenner, C. (Plenum, New York), Vol.

2 Sep 2012: Bray, Cell Movements: From Molecules to Motility(Garland, New York, 2001), 2nd ed.

2 Sep 2012: The relationship between suspensions of microorgan-isms and of sedimenting particles takes on new signifi-cance in light of measurements of velocity fields aroundfreely swimming organisms [5], which emphasized that theStokeslet

22 Mar 2012: N. G. De Bruijn, Asymptotic Methods in Analysis, Dover Publications Inc., New York,1981. ... 535–562. 22. F. W. J. Olver, Asymptotics and special functions, in Computer Science and AppliedMathematics, Academic Press, New York, London, 1974.

2 Sep 2012: coli in Motion (Springer, New York, 2004).6. M.D. Manson, P.M. Tedesco, H.C. ... 23. B.A. Finlayson, The Method of Weighted Residulas andVariational Principles (Academic Press, New York, 1972).

22 Mar 2012: Numerical Mathe-matics and Scientific Computation. Clarendon, Oxford University Press, New York (1995). ... Dover, New York (2001)32. Vandewalle, S.: Parallel Multigrid Waveform Relaxation for Parabolic Problems.

2 Aug 2012: Φ′(Q)T p = q, suchthat K1 depends only on the new momenta. ... εH1 δ < 0,. consequently H0 pt > 0, and the new Hamiltonian to consider is.

19 Sep 2012: Curr Biol 7:468–478. 33. Karpova N, Bobinnec Y, Fouix S, Huitorel P, Debec A (2006) Jupiter, a new Drosophilaprotein associated with microtubules. ... Cell 134:843–853. 47. Berg HC (1993) Random Walks in Biology (Princeton Univ Press, Princeton,New

2 Sep 2012: Halvorson, H. O. &Monroy, A. (Liss, New York), pp. 221–256. 11.

17 Apr 2012: Wethen used knowledge of this system to suggest a new method for estimating membraneviscosities.