Search

13 Jul 2011: just murky water, produces an initial sediment occupying over 30% of the volume, and how this weak fluffy sediment then compacts under its own weight over 24 hours.

14 Feb 2011: 0.0635388 0.532321 0 23 0 199.5 15.5 -0.0986939 0.69175 0 24 0 207.5 15.5 -0.419911 0.673265 0 25 0 215.5 ... 1 199.5 23.5 -0.0742271 0.746095 0 24 1 207.5 23.5 -0.236922 0.781727 0 25 1 215.5 23.5 -0.319311 0.835675

10 Apr 2011: 24 APRIL 2009. 0031-9007=09=102(16)=168101(4) 168101-1 2009 The American Physical Society. ... 1) may be reduced, in rescaled coordinates r r=hand t tF=h2 with h R, to [24].

10 Apr 2011: 15 OCTOBER 2010. 168101-2. surface [23], as well as a particular case of the ‘‘squirmer’’model [24]. ... Natl. Acad. Sci. U.S.A. 103, 8315. (2006).[24] J. R. Blake, J.

10 Apr 2011: www.sciencemag.org SCIENCE VOL 325 24 JULY 2009 489. REPORTS. on. July. ... 24 JULY 2009 VOL 325 SCIENCE www.sciencemag.org490. REPORTS. on. July. 24,.

10 Apr 2011: J. Colloid Interface Sci. 1981, 81, 531-535.(24) Adler, P. M. J. ... Scale bar is 2 mm. Letters Langmuir, Vol. 21, No. 24, 2005 10917.

10 Apr 2011: 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.

10 Apr 2011: An estimate of the hydrodynamic coupling between twoidealized flagella [24] is est ’ rRL. ... E.Goldstein, Science 325, 487 (2009). [24] T. Niedermayer, B. Eckhardt, and P.

10 Apr 2011: xj ij4s 1 Gas 2 1jsss. (10). Numerical solution [24] of (10) yields a critical valueac 8.9G [confirming dimensional analysis of Eq. ... Mod. Phys. 65, 851. (1993).[24] W. H. Press, W. T. Vetterling, S.

10 Apr 2011: sequences, or, alternatively, specified endpoint positions or lateral constraints, can be explored to ex-amine the internal relaxation rates of the intrinsic curvaturesand the long-time dynamics of buckled shapes 24. ... Soc. Edinburgh, Sect. A: Math. 99,

10 Apr 2011: Using magnetic beads [24], the flagellummay be rotated, permitting full examination of flagellarresponses to fluid drags and applied torques. ... J. 74, 1043 (1998).[23] D. Coombs, Ph.D. thesis, University of Arizona, 2001.[24] T.

10 Apr 2011: With small modifications,this experiment can include baroclinic effects, providing asimple model to address mixing in oceanic flows, such asgravity currents along undersea canyons [24]. ... R. Powers, Phys. Rev. E 69, 061910 (2004).[24] R. H. Kase, J.

10 Apr 2011: Moreover, the torsion dynamicis problematical at inflection points, wherek 0. The curve dynamics can be drastically simplified butilizing Hasimoto’s transformation [24] relating vortexfilament motion to the nonlinear Schrödinger equatioDefine the

10 Apr 2011: This and oobservations (e.g., of slow stress relaxation [24]) stronsuggest a dominant dissipative mechanismwithin the fila-ment, characterized by a very much largerzr. ... Chem. Phys.70, 2991. (1979); J. M. Schurr, Chem. Phys.84, 71 (1984).[24] J.

10 Apr 2011: 24). 232 A I Pesci et al. where we have used the notation i /xi. ... The equationof motion for u can be recast in the form (24) by taking its gradient and then replacing.

30 Sep 2011: CR strain CC124 [12] was grown axenically in tris-acetate-phosphate medium [11] in a growth chamber(Binder, Germany) set to 24 C and a cycle of 16 h lightat 100 ... Nikaido, J. Cell Sci. 109, 57 (1996). [24] M. A. Silverman and M.

10 Apr 2011: 0.947 1.422 0.380 0.589. 291.155 265.827 31.473 24.649 3.488 6.172. 3626.522 116.233 18.702 14.883 2.529

10 Apr 2011: To this end, substitute the constitutive relation(22) into the moment balanceequation (24)tofind the forceF on a cross-section:. ... C3. s= ζRω3. (31). The unknown functionΛ(s, t) occurs inEq. (30)because the moment balanceequation (24)does not

10 Apr 2011: xnpm n,m. Bnm1. 2n. nk=0. (n. k. )x̂nk(p̂mx̂k), (21). which is the correspondence obtained by using the operator ordering rule first introduced byWeyl [24]. ... Natl Acad. Sci. USA 18 674–6[24] Weyl H 1927 Z. Phys.

26 Mar 2011: This was conjectured by Slepian [20]. Asecond proof of this result is in [24]. ... 24] H. Widom, On a class of integral operators with discontinuous symbol.