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10 May 2022: 3. using a bispherical coordinate system [24–26]. These classical analytical results were later. ... Yamakawa kernel and matched asymptotics uses a larger prefactor of e3/24 [61].

10 May 2022: the proximal to the distal end of the filament13,24,41. ... Phys. Rev. E 98,. 042419, https://doi.org/10.1103/PhysRevE.98.042419 (2018). 24. Lee, W., Kim, Y., Griffith, B.

9 Nov 2022: Newtonian fluids, includingboth short-range and long-range hydrodynamic interactions,direct collisions, and Brownian motion (24, 28, 29, 31, 32,43, 44). ... 24) forNewtonian fluids to predict the size of the radius of curvatureusing the distribution of

18 May 2022: Rev. Fluid Mech. 24, 313–358 (1992). 8R. E. Goldstein, “Green algae as model organisms for biological fluid dynami-cs,” Annu. ... Miller, “Roles for motility in bacterial–host inter-actions,” Mol. Microbiol. 24, 1109–1117 (1997).

21 Oct 2022: 2.4.1 Noether’s Theorem 24. 2.5 Applications 26. 2.5.1 Bead on a Rotating Hoop 26. ... kinetic energy,. T(t2) T(t1) =i. Fexti dri. i 6=j. Fij dri (1.24).

16 Sep 2022: bit hole. First we’ll sort out some of the terms in (6.24), and then return to the 3-point. ... Our equation (6.24) for the correlation function has now. become. @Cij(r; t).

25 Aug 2022: Preprint typeset in JHEP style - HYPER VERSION. F́ısica Estad́ıstica. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences. Wilberforce Road,. Cambridge, CB3 OBA, UK.

16 Sep 2022: u = Ga and P =x a. 4r3(3.24). – 78 –. where G is the matrix. Gij =1. 8µ. ijr. xixjr3. The tensor G is known as the Stokeslet. ... right. Proof: First, we’ll check that the solution (3.24) obeys µr2u = rP everywhere.

30 Dec 2022: 1.2.4 Kramers Degeneracy 22. 2. Approximation Methods 24. 2.1 The Variational Method 24. ... ΘLΘ1 = L (1.24). – 19 –. We can also see how it acts on states.

21 Jul 2022: Received on 29 August 2019; revised on 10 April 2020; accepted on 24 June 2020].