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20 Jun 2011: 1B), where η is the viscosity, and the distance betweenthe forces (24, 25). ... 38. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

7 Apr 2021: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... N =. 0. which should clearly be an integer. The quantisation (3.24) due to a background magnetic field.

26 Jun 2024: in (1.24) because E = (0,0,E) lies parallel to the side of the torus, not perpendicular. ... Instead, both (1.23) and (1.24) are best thought of as integrating the 2-form Fµν over.

27 Feb 2018: Resource-explicit models of bacterial mutualismscompare well with experiments in which mutualists are wellmixed [5,6,23,24].

19 Oct 2013: Another importantwave activity measure is given by the pseudomomentum vector,. p = kA =h′ u′. ... Because of the ray-invariance of absolute frequency we have that |kA| = |kB | asympto-tically.

6 Jul 2020: Cobalt yielded an intrinsic rema-nent magnetization of $ 500 kA/m. Other magnetic materials, such asparamagnetic iron oxide, could be utilized with a stronger magneticfield. ... Mater. 24, 811–816 (2012). 7H. Ceylan et al., “Mobile microrobots for

13 Nov 2010: of the complexes (18, 85), probe local molecular conformations of DNA by use of specific anti- bodies (55), and follow protein-nucleic acid interactions in buffer (24).

4 Oct 2010: The effective charge of the particle is[1,2,24]. Zeff ef. kB T. ... Steinbock, G. Stober, U.F. Keyser, Biosens. Bioelectron. 24 (8) (2009) 2423.[24] John C.

28 Oct 2006: 1.7.13 Aide Memoire. 24. 2 Partial Differential Equations 25. 2.0 Why Study This? ... You should be able to do example sheets 1/2/3/4 after lectures 6/12/18/24 respectively.

23 Jul 2009: 1 ) , ( 2. 2 ) ; and for the case ka 4 1 and a general form of P by Batchelor (1983). ... pO as r / a c o , (3.24). and P-D;Vp = ikD,.P on r = 2a.

2 Sep 2012: T̂ = N̂. 24. The curvature is the rate of rotation of T̂ about B̂, and. ... Comparison of Eqs. 21–24 reveals that2 =1. 2 22 and 3 = , where is the angle between.

30 Oct 2010: kA 3 B A. ‡. 2/meG. 0‡/kBT , kB 3 A B. ‡. ... the applied force, the loadingrate varies as the molecule is stretched and Equation 17 cannot be used directly(22, 24).

19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret

27 Nov 2011: Geneproduct. Function ormotor component. Size(kDa). Copies permotorb. Operonclassc. FlgA Assembly of P-ring 24 2. ... Elements of the stator must beanchored to this framework somewhere, or torque cannot be delivered to theflagellar filament (24).

18 Oct 2019: non-negative, because. n = nhn|ni = hn|N |ni = hn|A†A|ni = kA|nik2 0 (3.11). ... 24 –. appreciable, then, to reasonable accuracy, all the terms that contribute to (3.31) oscillate.

7 Apr 2017: k. , sin a 1 (24) = - t v " 1 , 3 0 9 " l o g n a t '. Soll W g l e i e h W sein, so f o l ... g t d u r c h G l e i c h s e t z e n v o n (23) u n d (24).

7 Apr 2021: ai bj = 2 ij (3.24)? is sometimes referred to as the dual lattice. ... 91 –. The condition (3.24) can also be stated as the requirement that.

31 Jul 2008: 9.3.9]:. u0(t) = 1, u1(t) =3t 5t3. 24, u2(t) =. 81t2 462t4 385t61152. , ... 9.6.24]. Kν (νz) =1. 2. eνφ(v) dv, φ(v) = z cosh v v.

24 Feb 2020: Received 20 November 2019; revised manuscript received 5 February 2020; accepted 5 February 2020;published 24 February 2020). ... The 8 central flagella generate thrust while the 24 peripheralones are tilted by β 30 and generate both thrust and rotation.

10 Apr 2011: 23). (24). H.N.W. Lekkerkerker I Curvature elasticity o f charged monolayers 325. ... 2 6 ) - ( 2 8 ) to order 1/(Ka) 2 the following expression for the surface potential:.