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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: Each 24 mm3 18 mm image was obtained by subtracting twsuccessive images taken 30 sec. ... Mikhailov, Foundations of Synergetics I(Springer-Verlag, New York, 1994). [24] J. Buck, Q.

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: minimize overestimation of the trap stiffness. The calibration images were. reduced to remove optical and electronic noise (23) using Image J (24). ... for more details). The effective bending modulus found using. this fitting procedure is 42 24 pN mm2.

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.

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

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.