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9 Feb 2004: b 2004 to 131.111.8.96. Redistribution subject to AIP. ns. ’. the. ... The dotted line comes from theasymptotic theory of Sec. V B.b!

18 Jan 2007: G. Worster. (a). (b). (c). 12 cm. (b). (b). (a)(d). (c). ... dz= kl. d2T. dz2 b(T T). (2.3). 72 S. S. L.

30 May 2006: 8 ). ( 4. 8 b ). = 0 (n-reven), (4 8 c ) and Fnr = t w ' q s ,. , g , , r B B / ( b r - b n ). (,4.9). We again suppress the argument. ... 4.10 b ) N ( - )" 23(nw cosh [)-$ sin ( w cosh inn - &I-) sen(?).

30 May 2006: I n the former case. g ( t , y ) (Bt1-l (B-,O), (3.22). ... For B B 1 l,he penetration depth f L / N is much less than the actual depth H , and the critical height varies inversely with B.

7 Aug 2008: a dashed line, is the computational domain, shown in (b). (b) A schematic of the. ... 5(b). Wehave applied the same numerical method to predict the values of.

26 Apr 2006: where. B"B(j, hi)"! hi. Jpej2@4erf(j/2). (35). Eq. (34) is the transcendental equation determin-ing the eigenvalue j. ... Since gH is independent ofhiand B is expressed in closed form, we can calcu-.

7 Aug 2008: a dashed line, is the computational domain, shown in (b). (b) A schematic of the. ... 5(b). Wehave applied the same numerical method to predict the values of.

26 Mar 2023: b) As above, but for a two-dimensional geometry ( 3). 10 % of T. ... b), (b) the height above the input point, h(0, t), scaled by L2 and (c) the aspectratio of the current γ (height over length) as functions of dimensionless time

26 Sep 2011: d T / - d S < z. (5a,b) G = - z z f l d z. ... The Chemical. R u b b e r Co., 1263 pp.

21 Nov 2014: Using (2.14a,b) to evaluate P1 and P2 in (2.11), we obtain. ... its asymptotic value isdependent on all the parameters M, B, D and XF.