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28 Dec 2018: The code then calculates a new mesh by propagating the deformation throughout the.

18 Apr 2018: PHYSICAL REVIEW FLUIDS 3, 043601 (2018). Collective dissolution of microbubbles. Sébastien Michelin,1,2, Etienne Guérin,3 and Eric Lauga2,†1LadHyX, Département de Mécanique, Ecole Polytechnique, CNRS, 91128 Palaiseau, France. 2Department of

19 Jan 2018: x1. Finding LU is O(n3)but solving LUx = b for a new b is only O(n2). ... Need new direction v which does not reset u minimisation. f (xn αu βv) = f (xn) αu fn 12α2uT Au.

13 Dec 2018: The new inversion technique has been applied to an area covering the offshore sandbanks at Gt Yarmouth on the East Coast of the UK.

13 Apr 2018: Crew and A. de Salvio, Dialogues Con-cerning Two New Sciences (Macmillan, New York, 1914). ... 20] M. Abramowitz and I. A. Stegun, Handbook of MathematicalFunctions (Dover, New York, 1965).

19 Oct 2018: so nonlinear terms can produce new 23 M < n <43 M.

11 Oct 2018: We will seehowever that by adequately introducing new variables we can express it as a linear program.

13 Dec 2018: BAE Research Report, August 1995. 3 Kapp, D.A., and Brown, G.S.: ‘A new numerical method for roughsurface scattering calculations’, IEEE Trans.

13 Dec 2018: Mathematical modelling of shoreline evolu-tion, Proc. 16th Coast. Engrg. Conf., ASCE, New York, N.Y., p1163-1179. ... Coast. Struct. ’79,ASCE, New York, N.Y., p809-837. Wind, H.G., 1990. Influence functions, Proc.

19 Jan 2018: 3.6 Staggered grid – algorithm 4. New idea – a staggered grid with different variables at differentlocations.

13 Dec 2018: 3] Hsu, T-W., Ou, S-H & Wang, S-K., 1994. On the prediction of beach changes by a new 2-D empirical eigenfunction model, Coastal Engineering, 23, p255-270.

13 Dec 2018: lo] Mone P M and Feshbach H 1953 Methods of Zheoretical Physics I (New York: McGraw-Hill) [ll] Spivack M 1990 1 Acowf.

13 Dec 2018: Using the new Green’s function we can then derive extended forms of Eqs.4! ... 16Academic, New York, 1980! 2T. W. Dawson and J. A. Fawcett, ‘‘A boundary integral equation methfor acoustic scattering in a waveguide with nonplanar surfaces,’Acoust.

13 Dec 2018: 15A. Papoulis, Probability, Random Variables, and Stochastic Processes (McGraw-Hill, New York, 1981). ... 16A. Erd61yi, Tables oflntegral Transforms, I (McGraw-Hill, New York, 1954). 700 J.

13 Dec 2018: a new insight into the long-term spatial and temporal variations in coastline alignment. ... simplified solutions Proc. Comral Structue.es pp 809-36 (New York American Society of Civil Engineen).

10 Mar 2018: The remaining sixtypes define new transcendental functions and are given by the Painlevé equations. ... III. REDUCIBILITY AND FIRST INTEGRALS. The metrisable cases of PIII and PV do not define new transcendental functions but admit aquadrature and are

3 Aug 2018: shed new light on the physiology of gait control in flagellates,revealing its strongly nonequilibrium character.

13 Dec 2018: E. Wolf (Elsevier, New York, 1986). 5. A.G. Voronovitch, Wave Scattering from Rough Surfaces (Springer, Berlin, 1994). ... Nghiem-Phu, A new split-step Fourier algorithm, J. Acoust. Soc. Am. Suppl.

16 Jul 2018: At the end of a tum-ble, the motors return to their normal CCW state, the bundle reforms and the bacterium swims in a new direc-tion. ... E. coli in Motion. Biological and Medical Physics, Biomedical Engineering. Springer-Verlag New York (2004).

13 Dec 2018: implemented by a bounded operator. The proof constructs this operator. explicitly and hence yields a new and slightly more informative proof for nest.

20 Jul 2018: tions and theoretical analysis presented below. are new and worthy of being described as. ... cating how quantitative principles can be used. to derive new insight into phenomena.

4 Feb 2018: so nonlinear terms can produce new 23 M < n <43 M.

25 Oct 2018: No oscillations but lots of damping. Need new idea. 3. Total Variation Diminishing. ... No spurious oscillations with new minima and maxima. Preserves the monotonicity of a section of the solution.

5 Feb 2018: x1. Finding LU is O(n3)but solving LUx = b for a new b is only O(n2). ... Need new direction v which does not reset u minimisation. f (xn αu βv) = f (xn) αu fn 12α2uT Au.

16 Nov 2018: and a New Classification TheoryNovel Algorithms, Impossibility Results and Computer Assisted Proofs.

31 Dec 2018: frozen out. 3.2.4 Max Planck (1858-1947). “A new scientific truth does not triumph by convincing its opponents and. ... We can express this in. terms of our new favourite functions (3.27) as.

19 Oct 2018: to our continuum model (whatwe later call the ‘indirect chemotactic index’) and new phenomenology along withit.

11 Jan 2018: PHYSICAL REVIEW FLUIDS 2, 123101 (2017). Bundling of elastic filaments induced by hydrodynamic interactions. Yi Man,1, William Page,2 Robert J. Poole,2 and Eric Lauga1,†1Department of Applied Mathematics and Theoretical Physics, University of

26 Jan 2018: So we can regard(1.45) as defining a new kind of ensemble for the system S in which its temperature,rather than its energy, is held fixed.

26 Apr 2018: Reply. The course is about about how to start coding something you understand (and about some ofthe pitfalls), not about teaching new material. ... left of the ‘Editor’ window,followed by Save As.13 A new window should appear with a default File Name

3 Apr 2018: the isolated integrable vorticesof [22] while q = 1/3 gives rise to a new solution and completes thelist of integrable models under the class we consider.

19 Oct 2018: so nonlinear terms can produce new 23 M < n <43 M.

13 Dec 2018: E. Wolf (Elsevier, New York, 1986). [5] A.G. Voronovitch, Wave Scattering from Rough Surfaces (Springer, Berlin, 1994). ... Nghiem-Phu, A new split-step Fourier algorithm, J. Acoust. Soc. Am. Suppl.1 77 (1987) S101.

13 Dec 2018: 2] Y. He, P. Li, J. Shen, A new spectral method for numerical solution of theunbounded rough surface scattering problem, Journal of ComputationalPhysics 275 (2014) 608–625. ... 11] D. A. Kapp, G. S. Brown, A new numerical method for

23 Jan 2018: 13. The complex case contains no essential new ideas as compared to the real case, and issummarised here: Let B be Hermitian, then. ... Then addthe remaining I V 1 lines between the various vertices to restore the complete graph; eachaddition creates a

11 Oct 2018: 3.6 Staggered grid – algorithm 4. New idea –. a staggered grid with different variables at differentlocations. ... 3.6 Staggered grid – algorithm 4. New idea – a staggered grid with different variables at differentlocations.

11 Nov 2018: and a New Classification TheoryNovel Algorithms, Impossibility Results and Computer Assisted Proofs.

19 Jul 2018: J. Math. 85 (1963) 79–94.16. D. Moraru, ‘A new construction of anti-self-dual four-manifolds’, Ann.

13 Dec 2018: Kapp & G.S. Brown, A new numerical method for rough surface.

14 May 2018: 6.56). – 127 –. These diagrams tell us nothing new about the vertex; they’re already part of the exact elec-. ... x0 y0)4|x y| =. Zd4p. (2)4eip(xy). |p|2 (6.83). so we can combine the non-local interaction with the transverse photon propagator

1 Nov 2018: When we move an object around, we expect to find it in a new place. ... In other words, conjugating the X (component!) operator by U (a) gives a new operator.

13 Dec 2018: wy0y1 dx = 0.) Hence, to estimate λ1 we proceed asbefore but choose our new trial function y1 trial in such a way that it is orthogonal to our previous bestapproximation y0

13 Dec 2018: Then anew surface h2 can be reconstructed with the new sur-face wave φ2. ... A new split-step fourier algo-rithm for solving the parabolic wave equation with rough surfacescattering.

31 Dec 2018: something small. To emphasise this, it is common to make up some new notation8. ... T. Given some reference state O, this allows us to define a new.

25 Jul 2018: 2. In an idealized scenario, the reorientingtumbles result in unbiased new directions, uniformly chosen from the unit sphere, but this is not typicallythe case. ... One might also argue for the opposite: after a full tumble(or a series of persistent

12 Feb 2018: expect our eective action will contain infinitely many new self–interactions of x. ... Non–locality is generally bad news in physics: the equations of motion we’d obtain.

16 Aug 2018: However these new couplings perform no further role and aretherefore not introduced here. ... 4.33). This gives rise to new consistency conditions by requiring the finiteness of.

24 Jul 2018: An example is shown later in 9. Effects and benefits of the new principles. ... The subsampling pattern forthe new CS approach is the the one used in Fig.

16 Jun 2018: He talked about the loosening of thinking (Lockerungdes Denkens) that lets us see things in new ways. ... E. McIntyre 2016: Jupiter’s unearthly jets:A new turbulent model exhibiting statistical steadiness with-out large-scale dissipation.

13 Dec 2018: New York. Bailard, J.A., 1984. A simplified model for longshore sediment.