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25 Jul 2008: Spheroid: axes a, b, b, aspect ratio r = ab. rod r > 1 disk r < 1. ... A B C. r r 22(ln 2r3. 2). 6 ln 2r11r 2.

30 Oct 2008: We add and subtractf(b),. I[f,g,θ] = f(b). b. a. g(sin[ωθ(x)]) dx. ... b. a. [f(x) f(b)]g(sin[ωθ(x)]) dx. = f(b). b. a. g(sin[ωθ(x)]) dx.

26 Jul 2013: b c d e. ii. iii. iv. Kn = 0. Kn = 0.2 Kn = 0.4 Kn = 0.5. ... Kn Kn/Knc. 1.00 10.00. (a) (b). CD. 0.2. 0. 0.4. 0.6.

22 Jan 2019: A B. B D. )(U. ωp. )=. (Z. H. )ωf l , (25). ... b) Plot of U vs the length of the fibers Lfib following Eq.

26 Jul 2013: V2 =¡ (1) (2) ¢ ¢ ¢ (n). ¢;. taking A = ¤ , B = B, Q = I, R = 2I and ¤ cl = ¡ ¤ ¤ , and applying the aboverelationships, it follows that (3.7 ... written in the form _À = ¤ À Bu, where the diagonal matrix ¤ contains theunstable eigenvalues

22 Jan 2018: b "arctan ðcos2 W þ q sin2 WÞR. 2ð1 " qÞsin W cos Wh! : ... Torques computedusing the analytical model (RFT, a) and the numerical model (SBT, b).

23 Nov 2023: a2 = b, a3 reproduces the group multiplication rules defining D3 S3 in (1.20). ... Conversely for n odd Z2 Dn D2n where the extra element ccommutes with a, b.

2 Oct 2017: b b- -. ( ). ( ). ( ) ( ). F y f f. Ay. w. y. wA. y. w. y. ... a, b) Dilute and dense suspensions of motile ellipseswithout hydrodynamical interactions (s = 0).

7 Mar 2013: On the other hand, the demand of re-1/2 1/2 1/2 1/2B (B B ) Bsources depends on the number of cells in the colony andthe total cells ... gb Bvif 1, v p 1,dc Cv. g gb B b Bv vif!

21 Feb 2022: T. B<0. B>01. 1. Figure 7:. m! B. Tas T! 1. ... move from any point B 6= 0 to any other point without suering.