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search results for `B b cos` |u:www.damtp.cam.ac.uk
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Invpend.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2010_05.pdf4 May 2010: eη cos ωt = I0(η) 2. m=1. Im(η) cos mωt, (4). ... Alternatively, if wedefine the potential. H(p,q) = 12p2. g. cos q σ. -
An exact theory of nonlinear waves on a Lagrangian-mean flow
www.damtp.cam.ac.uk/user/mem/andrews-mcintyre-glm-jfm78.pdf22 Jul 2010: Further properties of J and K j j. Appendix B. Derivation of theorem I. ... v?,, = (v,tF (v,jF q , t , m,i = (v,$ q , i 9 (2.4u, b ). B(x, t ) = x E(X, t ) , (2.6). (vii) The mapping (2.2) -
Problems and prospects in the theory of gel electrophoresis of DNA
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/electrokinetics/zimm.pdf18 Nov 2010: The concept in a more relaxed form. 176 B. H. Zimm and S. ... 1987) and by Jonsson et al. (1988). 188 B. H. Zimm and S. -
REVIEW OF SCIENTIFIC INSTRUMENTS VOLUME 75, NUMBER 9 SEPTEMBER ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/optical_tweezers/neuman-block.pdf28 Oct 2010: The net force on the bead is to the right, in the directionintensity gradient, and slightly down.(B) To form a stable trap, the ligmust be focused, producing a three-dimensional ... B. Trapping laser. The basic requirement of a trapping laser is that it -
USING STANDARD SYSTE
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/electrokinetics/viovy.pdf4 Oct 2010: Irreversible trapping 8534. Trapping of rigid particles 854. B. Polyelectrolytes with nonlinear architectures 8551. ... In waterat room temperature, l B is of the order of 0.7 nm.
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