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16 Jun 2023: mathrm{S}mathrm{I}mathrm{A}mathrm{M} mathrm{J}. mathrm{N}mathrm{U}mathrm{M}mathrm{E}mathrm{R}. mathrm{A}mathrm{N}mathrm{A}mathrm{L}. 2023 mathrm{S}mathrm{o}mathrm{c}mathrm{i}mathrm{e}mathrm{t}mathrm{y} mathrm{f}mathrm{o}mathrm{r}

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).

1 Dec 2023: 0.025 0.050 0.100 0.200. (a) (b). (c) (d ). (e) ( f ). 0.05. 0.10. 0.15. 0.20. 0.25. 0.30. 0.02. 0.01.

21 Jan 2023: 0-300. 0.6. 0. -200. (a) (b). (c) (d). 30. -20. -10. ... 20. 10. 0. 0. 100. 200. 300. 400cis. trans. FIG. 6.

22 Sep 2023: For reading comfort I recommend zooming in, usually Ctrl+ or Ctrl-Shift+, or Cmnd+ on Mac. This web page previewsby Herbert E. Huppert FRS. Foreword. by Herbert E. Huppert FRS. Michael Edgeworth McIntyre FRS has written a book wide in its

1 Dec 2023: J. Fluid Mech. (2016), vol. 790, pp. 173–204. c Cambridge University Press 2016doi:10.1017/jfm.2016.8. 173. Obstructed and channelized viscoplastic flowin a Hele-Shaw cell. D. R. Hewitt1,2,†, M. Daneshi3, N. J. Balmforth2 and D. M. Martinez3.

1 Dec 2023: order of Q ' 200–710 m3 s1.Hence, given the range of b0, the dimensionless flux could lie anywhere betweenQ̃'2109–6.5103. ... till. These sizes varied significantly depending on the parameters,but for a typical simulation we used a domain 0 < r <

26 Jan 2023: 5.4.4 Chern-Simons Theory with Wilson Lines 192. 5.4.5 Eective Theories of Non-Abelian Quantum Hall States 200.

1 Dec 2023: J. Fluid Mech. (2020), vol. 883, A37. c Cambridge University Press 2019doi:10.1017/jfm.2019.888. 883 A37-1. Buoyancy-driven plumes in a layeredporous medium. Duncan R. Hewitt1,†, Gunnar G. Peng2 and John R. Lister2. 1Department of Mathematics,

1 Dec 2023: xp = 2Ra1/2. Figure 6. (a) vertical advective heat flux at the top boundary for Ra = 200 with boundarycondition BC 2 and aspect ratio L = 4.