Search

2 Dec 2014: correlated across multiple scales. In the first instance wecan derive a scalar measure a via a detrended fluctuationanalysis to characterize an individual time series [24], asfollows. ... Lodha, and M. Schroda, Plant J. 52,286 (2007). [24] C.-K. Peng, S.

24 Dec 2014: Emacs Lisp List. Last updated: Wed Dec 24 11:36:00 2014. 1270 entries. ... Sat 24 Jun 2006. Update ell.el to point to ELL at Cambridge.

23 Jun 2014: Theoptimal stroke pattern of Purcell’s finite three-link swimmerwas found by Tam and Hosoi [23], who then went on toconsider optimal gaits for the green alga Chlamydomonas[24]. ... Rev. Lett. 98, 068105 (2007).[24] D. Tam and A. E. Hosoi, Proc.

23 Oct 2014: 7, 13, 22–24, 33, 34, 39]. We consider the quadratic in-variant Q = qT Dp of (1). ... u(h) = p0 hk. l=1. blf (vl),. (24). where h is the stepsize, cl, bl, l = 1, 2,. ,

29 Aug 2014: 24–26]. In this case, thepropulsion, which is impossible to achieve in an isotropicmedium, is enabled by the presence of a wall which breaksthe symmetry of the nearby environment. ... sinh(n 1/2)(α β). [e(n1/2)α sinh(n 1/2)β. e(n1/2)β sinh(n 1/2)α

4 Sep 2014: µJµ5 =1. 24 16π221N3/2 N1/2. Rµνρσ Rµνρσ (3.5). For us, N1/2 = 0 and N3/2 = 1. ... The. distinction between rigid and gravitational theories was stressed, in particular, in [24]).

26 Mar 2014: g., velocity statistics (20–22) andpressure (23)] show starkly different behavior––see, e.g., therecent reviews (24, 25). ... Phys Rev Lett 82(24):4831–4834.9. Kobayashi M, Tsubota M (2005) Kolmogorov spectrum of superfluid turbulence:.

9 Nov 2014: 2. (φ. t. φ. t+ c2φ φ. )dV (5.24). 24For simplicity, I’ll only consider real–valued functions here.

22 Apr 2014: This hypothesis isconfirmed by numerical simulations performed using Brakke’sSURFACE EVOLVER [24] and shown in Fig. ... We useSURFACE EVOLVER [24] to analyze the system behavior,illustrating the results with θE = π/2 and 3π/4.

24 Dec 2014: Emacs Lisp List. Last updated: Wed 24 Dec 2014 11:36:00 GMT.