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On the mechanisms of icicle evolution
www.damtp.cam.ac.uk/user/gold/pdfs/icicles_jfm.pdf10 Apr 2011: FT = kT. z. z=0. = kTL. Ra1/5θ ′(0). h(x), (2.20). ... 0.5 1.0 1.5 2.0 2.5 3.00. 5. 10. 15. 20. 25. -
DAMTP 2010/NA04 Beyond symmetric Broyden for updating quadratic…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2010_04.pdf13 Apr 2011: and y+. 4=. (20. ), (3.4). 8. with t = 4, θ = 0 and v = xk1 = xk = y1. , ... 5000 and n 20, but,for n = 10, the norms ‖Ek‖F become of the magnitude of computer roundingerrors in the difference 2Qk2F. -
P H Y S I C A L R ...
www.damtp.cam.ac.uk/user/gold/pdfs/necking.pdf10 Apr 2011: Adjacent wires have the samelength, from top to bottom: kFL 0, 10, 20, 40, 70, 105, and140. ... Kassubek, J. Bürki, and H. Grabert,. Phys. Rev. Lett. 83, 4836 (1999).[20] F. -
Optical metrics and projective equivalence Stephen Casey,* Maciej…
www.damtp.cam.ac.uk/user/md327/CDGW_file.pdf28 Apr 2011: Carter, and J. P. Lasota, Gen.Relativ. Gravit. 20, 1173 (1988). [4] S. -
Broken particle-hole symmetry in critical fluids Raymond E.…
www.damtp.cam.ac.uk/user/gold/pdfs/broken_particle_hole.pdf10 Apr 2011: The effective Hamiltonian in Eq. (20) has odd (and momentum dependent) terms just like those in the simpli-fied field-theoretic model Eq. ... 20) onto the field-mixing operator. For this purpose, we note on general grounds and independent of the -
Emergence of Synchronized Beating during the Regrowth of Eukaryotic…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/GoldsteinPolinTuval11.pdf30 Sep 2011: 2Department of Global Change Research, Mediterranean Institute for Advanced Studies (CSIC-UIB), E-07190 Esporles, Spain(Received 20 June 2011; published 30 September 2011). ... 30 SEPTEMBER 2011. 148103-4. 20] S. Takada and R. Kamiya, Cell Motil. -
Model for phase equilibria in micellar solutions of non ...
www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_84_3367.pdf10 Apr 2011: 00. 2Xt/J - t/JI(1 - t/J) - L (Bt/JnIBt/J)/nM = 0 (20) n=1. ... 3. (a) Micelle size distribution for; = 0.08, M = 20, E = 0.85, and q = 3. -
Generalized sampling and the stable and accuratereconstruction of…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_12.pdf22 Nov 2011: f fn,m‖R (1 θ2. )‖f Qnf‖R c(2 θ)θ2|||f Qnf|||, (2.20). and thatκ(A). ... 12. The estimate (2.20) for ‖f fn,m‖ holds with the stronger assumption (A2′). -
Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments…
www.damtp.cam.ac.uk/user/gold/pdfs/trapping.pdf10 Apr 2011: We note from the solution (Eq. 20) that each modegkdecays independently and exponentially with time. ... 0.485ỹ; yk2(0). 20.012ỹ, where we defineykn [ 0. 1 da y0kn, in analogy toEq. -
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...
www.damtp.cam.ac.uk/user/gold/pdfs/wigner_jphysa.pdf10 Apr 2011: k. )x̂nk(p̂mx̂k). (20). Here, we have used the notation x̂ = x and p̂ iη/x, together with the identity proven byMcCoy [23] (see also appendix B). ... Interscience)[19] Fröhlich H 1967 Physica 37 215–26[20] Fröhlich H 1973 Riv.
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