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10 Apr 2011: 3). vs T = - l/Ka• Recall that this expression refers to the formulation in Eq. ... I(K1,K2 ,Ka) =! Ko+ In Tria,) exp[L: Keff(l- Oa,a /)] , (lJ) (16).

20 Sep 2011: ω 6= 0 so ω defines a Killing vector Ka.Killing identity Ka RabKb = 0, where Rab = gab/4. ... M|K|2gd4x = 1. 4. M|K|2gd4x. Therefore Ka = 0 and our assumption was wrong.

10 Apr 2011: 2 6 ) - ( 2 8 ) to order 1/(Ka) 2 the following expression for the surface potential:. ... 1 2 ( q - 1) 1 ( q - 1)2(2q 1) 3 3 , (29) = 2 l n ( p q) Ka p q ( K a ) 2 p q.

10 Apr 2011: Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments. Chris H. Wiggins, D. Riveline,# A. Ott,# and Raymond E. Goldstein. Department of Physics, Princeton University, Princeton, New Jersey 08544 USA; #Institut Curie, Section de

10 Apr 2011: Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments. Chris H. Wiggins, D. Riveline,# A. Ott,# and Raymond E. Goldstein. Department of Physics, Princeton University, Princeton, New Jersey 08544 USA; #Institut Curie, Section de

20 Jan 2011: 2.12)Consider a complex tetrad of 1-forms. Ka = i(α̂AβA′ αAβ̂A′ ), Xa = α̂AβA′ αAβ̂A′ , Za = αAβA′. ... We now use(2.16) to find. φAB = 2|K|2 KA′B AA′. (1.

1 Sep 2011: On Lp-boundedness of the L2-projectoronto nite element spacesA. Yu. Shadrin1. IntroductionIn [Sh] we proved that, for p suciently close to 2, the Lp-norm of the L2-projector P onto the space S of polynomial splines of order k on a knot-sequence is

1 Sep 2011: TO KA-SAETSQ PORQDKA POLIGARMONINOSTI (g) = @(f)=@xj, TO, POSKOLXKU OPERACIQ DIFFERENCIRO-WANIQ SOHRANQET TOT PORQDOK, IMEEMr2(g) = 0; = m1 1 2m1 = m:pREDLOVENIE 1a0, A S NIM I SLUAJ 1a)

5 Aug 2011: Although the strong correlationsuggests an almost constant and linear relationship, it actually appears as ifthe earliest part of the record (before about 650 ka) had lower mixing ratios(both absolutely and ... a) The last interglacial and methane. The

26 Nov 2011: Part III: Biological Physics (Michaelmas, 2011) R E Goldstein (26/11/11). Examples Sheet #3. 1. Nonlinear Diffusion. For the nonlinear diffusion equation Ct = D(CpCx)x, where p and D. are strictly positive constants, show that the self similar

10 Apr 2011: RAPID COMMUNICATIONS. PHYSICAL REVIEW E AUGUST 1997VOLUME 56, NUMBER 2. Elastohydrodynamic study of actin filaments using fluorescence microscopy. D. Riveline,1 C. H. Wiggins,2 R. E. Goldstein,3 and A. Ott1,1Laboratoire PhysicoChimie Curie,†

10 Apr 2011: Tem- perature is T = - l/Ka, normalized to the critical coupling of the Ising model.

6 Jul 2011: 38. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

10 Apr 2011: PACS: 87.17.d; 87.16.Ka; 05.45.a; 46.70.De. Keywords: Supercoil; Growth; Elastic filaments; Filamentous bacteria.

10 Apr 2011: 0.6. xc. 0.5 ---- --------Xc«Mn)a CXl)---------. 0.4. 0.4 0.5 0.6. ka T lu.

1 Sep 2011: i j is js s, |i| :=. s. is. The following lemmas will be used frequently (see [Ka], pp.

20 Jun 2011: 38. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

27 Nov 2011: THE ROTARY MOTOR OF BACTERIALFLAGELLA. Howard C. BergDepartment of Molecular and Cellular Biology, Harvard University, 16 DivinityAvenue, Cambridge, Massachusetts 02138; email: hberg@biosun.harvard.edu. Key Words Escherichia coli, motility,