Search

2 Sep 2012: 2Program in Applied Mathematics, University of Arizona, Tucson, Arizona 85721, USA(Received 23 December 2003; published 24 August 2004). ... Rev.Lett. 71, 3975 (1993). [24] P. N. Segre, E. Herbolzheimer, and P.

27 Aug 2012: 23). From (22) and (23)PJL. For a given power P and frequency / , equation (24) gives a maximum value ofuwhen ,X. ... the observed value is 24/14.

10 Oct 2012: Therefore, (3.24) follows.The term Q1 is estimated using the bound. |Q1| = G. ... Fiα(λF) >= A Fiα (F) and the estimation (in. the spirit of (3.24)).

3 Sep 2012: See the article by Howard Berg, PHYSICSTODAY, January 2000, page 24.) The effect is not un-like a corkscrew pulling itself through the cork of awine bottle, except that the flagellum

12 Sep 2012: In a preliminary work [23, 24] we explored some mor-phological aspects of the fracture profiles obtained inplane-plane debonding experiments performed with gran-ular adhesives (crushed sand in an acrylic ... Van Damme, Fractals 1, 968 (1993).24. H. Van

2 Sep 2012: On time scales shorter than , effects associ-ated with spatiotemporal correlations in Q [23] intervene.For a drop [24] or a film [22] of size L, the tails will be cutoff ... Tu, Phys. Rev. E 64, 011902. (2001).[24] G.V. Soni et al., Biophys.

2 Sep 2012: On the other hand, recent advances frommicron-scale magnetically actuated tails [24] to syntheticmolecular rotors [25] now allow fabrication of arrays ofactive tails that can stir up the fluid. ... 2007); Small 4, 111 (2008).[24] R. Dreyfus et al.,

16 Jul 2012: λ1 1270.9 1103.4 1100.7 1099.8 1189.8λ2 26.39 48.24 46.37 44.92 28.13. ... 24] K. Frick, P. Marnitz, A. Munk, Statistical Multiresolution Estimation for Variational Imaging:With an Application in Poisson-Biophotonics, J.

22 Mar 2012: Evolving ideas of the stationary phase approximation [24], ourmethodsrequire explicit availability of more terms in the asymptotic expansion, leadingto the assumptions of non singularity of the matrix Aω and smoothness of ... 637–655. 24. E. M. Stein,

2 Sep 2012: 24 OCTOBER 2008. 178102-3. [Fig. 4(b)] is dominated by a 1= dependence, leading to avery strong 3 scaling as the amplitude of the streamfunction approaches zero. ... G. Bessoth, A. J. deMello, and A. Manz, Anal. Commun. 36, 213 (1999).[24] J.

2 Sep 2012: The data wedisplay in this article are for a dimensionless gap size / R= 0.24. ... 24. Assuming all balls are far apart, we again use the Oseenmodel, Eq.

2 Sep 2012: Onemilliliter of 24-h stock was added to 50 ml of TB and incubated for18 h. ... O. (1992) Annu. Rev. Fluid Mech. 24, 313–358.12. Hillesdon, A. J., Pedley, T.

6 Mar 2012: 24. More termsmain body. With h = c2n/3H,. (H Hxx )x = c2n/3G c(2n1)n/3. ... 24. More termsMatching: transition regions. Transition regions=. h0 h2 h3 h4 h5.

3 Sep 2012: 24). So, by substituting (24) into (23), we have that. (P2M2)P1M1ϕ2 lBM2.

2 Sep 2012: 4 A), representing either depletion or waste, alsoprovide spatially and temporally extended signals for the presenceof a colony, perhaps significant for intercolony communication, asin sexual induction (23) and quorum sensing (24), ... Michod, R. E. (2004

28 Feb 2012: 3.24) 2B2A4 2[(. κ2 2) 2. ]BA3 2 2. (κ2 2. ... Nevertheless, from (3.24) the Re 0 limit is observedto be consistent with (3.12) obtained for Re = 0 and M = 1.

2 Sep 2012: solution to (24) subject to the boundary conditions is(Carslaw and Jaeger, 1959). ... computations. Fig. 2. The radial distribution function R0(r) for the parameter valuesP 1, N 8 , and Q 24.

2 Sep 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J.

20 Oct 2012: 3 Consistent reconstructions and oblique projections. We now consider the consistent sampling technique of [23, 24, 28, 55, 57]. ... An analysis of consistent reconstructions, which we shall recap and extend in 3.3, was given in[23, 24, 28].

2 Sep 2012: Rev. Fluid Mech. 24,313 (1992). [2] A. Einstein, Ann. Phys. (Leipzig) 17, 549 (1905).[3] P.