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3 Dec 2022: 162r2c3|m̈|2 sin2 ẑ (6.24). – 150 –. Integrating over all space gives us the power emitted,.

22 Jul 2022: S̃l(λ) =. 0. eiλtSl(t)dt. (24). B. Collocation points and basis choice.

21 Feb 2022: 1.3.1 The Landau-Ginzburg Free Energy 24. 1.3.2 The Saddle Point and Domain Walls 26.

27 Mar 2022: 2 The Lagrangian Formalism. 2 The Lagrangian Formalism. When I was in high school, my physics teacher called me down one day after class and said, “You look bored, I want to tell you something interesting”. Then he told me something I have

29 May 2022: 2017 Schlumberger Chair for Mathematical Sciences, IHES, Bures-sur-Yvette, France SUPERVISION OF GRADUATE STUDENTS AND POSTDOCTORAL FELLOWS 1991 – 2020 24 PhD Students Completed (3 Princeton, 6 Arizona, 15 Cambridge): 5 ... 24. Geometrical and

3 Dec 2022: 2.2.3 General Charge Distributions 20. 2.2.4 Field Lines 23. 2.2.5 Electrostatic Equilibrium 24.

9 Nov 2022: III and IV. The setup of downward jets is relevant to range of biological situations,including a falling plume of a cell suspension, i.e., bioconvection [22–24]. ... Pedley, Bioconvection, Fluid Dyn. Res. 37, 1 (2005).[24] M. A. Bees, Advances in

9 Mar 2022: 24. Microstructure 1 – rotation. Jeffery (1922) found that rigid ellipsoids rotated with all of the vorticity ,. but only a fraction of strain-rate, a fraction r21r21. Hence non-affine slip, introduced

28 Nov 2022: capillary waves. (See the large k limit of (4.24).) This is to be expected: waves with. ... t+ u r! =. 1. 2r rP! ru r2u (5.24).

10 May 2022: 2.24). Notably, this expression can be simplified into. s0 =sb(rc) r s(.