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1 Dec 2023: b,c) Marginal stability curves (σ =0, outlines)and regions of instability (σ > 0, shaded areas), for R = 3 and (b) Pe = 25, 200, 500 and(c) Pe=15, 20, 25.

25 Jan 2007: λsin. q̃ q2. , (4.1.4). 16. Cop. yrig. ht. 200. 7 U. ... M1x i[σ3, M2] = QM1. (4.3.18). 21. Cop. yrig. ht. 200.

26 Jul 2013: 440. D.L. egen. dre,. E.L. auga. and. J.M. agnaudet. Kn = 0 Re = 5 20 50 100 200 500 800. ... 1000.0. 0 0.5 1.0 1.5 2.0 2.5. 47.5. Kn. Re. Re = 200.

10 Jun 2024: J. Fluid Mech. (2024), vol. 988, A10, doi:10.1017/jfm.2024.223. Flow of an Oldroyd-B fluid in a slowly varyingcontraction: theoretical results for arbitraryvalues of Deborah number in the ultra-dilutelimit. Evgeniy Boyko1,†, John Hinch2 and Howard

18 Oct 2023: We use the geodesicicosahedron f3; 5þgð3;0Þ in standard notation [17], with 92total vertices, and take patches with N 58 to be repre-sentative of experimentally observed sizes (10–200

26 Jul 2013: In 1963,Rothschild measured the distribution of bull spermatozoaswimming between two glass plates (separation 200 m).The cell distribution was nonuniform, with a constantdensity in the center strongly increasing near the ... 48:3 15 m; when H 200 m,

13 Sep 2023: theory took over 200 years to discover; and it’s not at all clear what the relationship is.

2 Jan 2024: CEOS DCOR probe corrector.The microscope was operated at 200 keV with a beam current of 80 pA. ... TheSTEM convergence angle used was 25.5 mrad with HAADF detector inner andouter collection angles of 50 and 200 mrad, respectively.

25 Jan 2007: 200. 2 U. nive. rsity. of C. ambr. idge. Not. to b. ... Suppose the surface charge to be18. Cop. yrig. ht. 200. 2 U.

1 Dec 2023: 2 m3 s1, and the total volume over the 200 sduration to 4.95 m3. ... The resultingtime constant D was 18,200 s for BH19c, 25,000 s for BH19e and23,000 s for BH19g(e).