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12 Sep 2022: 23/36. What went wrong? 24/36. What went wrong? 24/36. Recall complexity of Karmarkar’s algorithm: 𝑂(𝑛3.5𝐿2 log 𝐿 log log 𝐿 ). Question: What happens with 𝐿 =?

22 Jul 2022: In particular, we refer the reader to work by Böttcher [14,24],Böttcher and Silbermann [22], Lindner [59, 61], Marletta [62], and Marletta andScheichl [63].

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).

29 Jan 2022: Wang et al., Sci. Adv. 8, eabk0685 (2022) 14 January 2022. S C I E N C E A D V A N C E S | R E S E A R C H A R T I C L E. 1 of 14. C O N D E N S E D M A T T E R P H Y S I C S. Order and information in the patterns of spinning magnetic micro-disks at

18 May 2022: Niedermayer, B. Eckhardt, and P. Lenz, Chaos 18,. 037128 (2008).[24] D.

18 Nov 2022: mpEDMD: First convergent Galerkin method! 24/34. Numerical examples. 25/34. Lorenz system: scalar-valued spec measሶ𝑥1 = 10 𝑥2 𝑥1 , ሶ𝑥2 = 𝑥1 28 𝑥3 𝑥2, ሶ𝑥3 = 𝑥1𝑥2.

7 Jul 2022: Eng. Sci.,1976, 31, 901–911. 24 S. Engelnkemper, M. Wilczek, S. V. ... Tcholakova, M. Vethamuthuand A. Lips, Surfactant Mixtures for Control of Bubble SurfaceMobility in Foam Studies, Langmuir, 2008, 24, 9956–9961.

3 Dec 2022: 2. Zd3r0 r0 J(r0) (3.24). Just as in the electric case, the multipole expansion continues to higher terms. ... 3.24),. B(r) =µ04. 3(m1 r̂)r̂ m1. r3. (3.30). Now we’ll consider how this aects the second dipole m = m2.

27 Mar 2022: Expand out all 24 terms and watch them cancel one by one.

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

16 Jun 2022: Û(t) = exp(itĤ) (24). which is sensibly called the time evolution operator.

23 Sep 2022: work in [24, 29, 42, 48, 49,66, 67].

29 Jan 2022: Thesis, University of. Kaiserslautern, Kaiserslautern, Germany, 2000.[24] L. Koens and E.

23 Mar 2022: 24 , 20 No. 3. 11 220 1 967 2 34242 0 14525 0 29392 1 66300. ... 23 ,- 11 116 2 004 2-33445 0 14525 0 30189 1P65503 25 ,, 24. ,

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.

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).

17 Sep 2022: to 1. 93.5. 2.24. 28. by M. atth. ew C. olbr. ... 93.5. 2.24. 28. by M. atth. ew C. olbr. ook. (mjc.

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).