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23 Jul 2009: with the three shape constants. a = $ ( B 2 - B 1 ) , /3 = # ( B , B l ) and y = 4B3. ... At O ( B ) , the variation in q5 a t O( 1) drives harmonic oscilla- tions, i.e.

31 Jul 2009: 1, 367. LUMLEY, J. L. MAIJGREN, B. Molecular aspects of the drag-reduction phenomenon. ... MANDELBROT, B. B. 1974 Intermittent turbulence in self-similar cascades : divergence of.

27 Jul 2009: Plansangkate. where x j, j = 1, 2, 3, are local coordinates on B. ... s = b(y)eu3α and n = αx. for some b = b(y) = 0.

10 Nov 2009: FIG. 1. Concentration profile vs normalized height z / H for particles of batches A a, B b, D c in the cell having a cross section 10 10 cm2, and C ... FIG. 2. Time evolution of the velocity fluctuations w open symbols and the concentration gradient ad /

10 Jul 2009: away from the (collapsed) numerical results. and secularity is averted at order O(β1) if T0 B 0, whence B = B(T1) and. ... B(T ) ={. 1 T. 24β. }1/2. (5.2). Thus, for T 1,.

10 Jul 2009: a) Gravity acts on the fundamental mode to create the firstharmonic in (b). ... b) Capillary pressure gradients act to create the phase-shifted first harmonicin (c).

3 Sep 2009: Bernard, B. Hambrecht, P. Lugan, D. Clement,L. Sanchez-Palencia, P. Bouyer, A. ... Rev. Lett. 101 (2008)080401. [65] Th. Anker, M. Albiez, B. Eiermann, M.

14 Jul 2009: 2 = y e x - i B y , y = e y - - B x , 1. ... 0.05 1 b B 0.05. 0 0.02 0.04 0.06 0.08. (b) 0.04.

24 Aug 2009: 3A(sin4 8, sin 24,) - 2(A - B)(sin28, sin 24,)}, of, = of. = ... A , B, F, 211, would not be related to the particle aspect ratio in 6he manner described for spheroids.

13 Jul 2009: As a model problem we take. %(x) = U_[l - exp( -x/b)], (1). ... As indicated above, to make the calculation tractable we shall, however, assume that b B a so that the flow is almost unidirectional almost everywhere and lubrication methods can be employed.