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19 Oct 2018: Funct. Mater. 2010, 20, 2430.[5] M. García, J. Orozco, M. Guix, W. ... 2017, 49, 511.[19] J. L. Anderson, Annu. Rev. Fluid Mech. 1989, 21, 61.[20] W.

30 Nov 2018: B. Calculation of the elastic strains. To calculate the deformation gradient, we make the Kirch-hoff “hypothesis” [20], that the normals to the undeformedmidsurface remain normal to the midsurface in the ... 20] B. Audoly and Y. Pomeau, in Elasticity

13 Dec 2018: metres 400. 200. 0. -200. - 4 0 0 o 10 20 30 40 50.

18 Apr 2018: The nature and properties of the dissolved species,and the physical exchange on the surface of the bubble, are the main distinguishing features betweenvapor and gas bubbles [8,20]. ... 2 sinh(n 12. )η. , (20). with η = η1 η2 (see details in Appendix B

13 Dec 2018: 20). where Xl = 12 (xl1 xl). The last subintegral with singularitycan be approximated by. ... Then everything turns to be knownin Eq. (20) except the discrete ψ′(Xl).

27 Feb 2018: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom. (Received 19 December 2017; published 20 February 2018). ... 0 10 20 30Time t. 0.0. 0.1. 0.2. 0.3. 0.4. 0.5.

18 Nov 2018: Zworski [20, 21]. Introduction Schrödinger and PDEs Discrete operators Numerical Examples Conclusion Definitions.

27 Nov 2018: form, where the cell velocity scales linearlywith chemoattractant gradient, the KS model can lead toinfinite concentrations in finite time [20]. ... Note that the Péclet number isthen Pe = 1/Dc 2.5. For faster-swimming organisms, suchas marine bac0teria

11 Jan 2018: rts (. I 12. rs rs. ) vs 1. 2(rss rs rs rss ) (rt v), (20). ... 0. 10. 20. 30. Bu=2. Bu=30. Bu=60. (a). (b. ( )(c).

1 Nov 2018: can be written as20. U (a) = 1 i a P O(a2) (4.20). ... Plugging (4.20) into the defining equation (4.18) for the translation operator we find.