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Mathematical Tripos, Part IB : Electromagnetism, Dr Natalia Berloff…
www.damtp.cam.ac.uk/user/ngb23/EM/Chapter1.pdf16 Jan 2009: n E|. =1. ǫ0σ (23). nE|. = 0. (24). b). Let S carry current density s per unit length (charge crossing unit length in S in unittime). -
Mathematical Tripos, Part IB : Electromagnetism 3 Steady electric ...
www.damtp.cam.ac.uk/user/ngb23/EM/Chapter3.pdf29 Jan 2009: 24. Recall Section 1.6: A is not unique, because we can transform the vector potential according to. -
CURRICULUM VITAE Name Nilanjana Datta Profession Affiliated Lecturer…
www.damtp.cam.ac.uk/user/nila/cv0809.pdf26 Apr 2009: 24) D. Bruss, N.Datta, A. Ekert, L.C. Kwek and C. Macchiavello, Multipartite entangle-. -
Existence and Newtonian limit of nonlinear bound states in ...
www.damtp.cam.ac.uk/user/dmas2/public_ps/ed.pdf15 Oct 2009: 2ψ22) 2me2N Φ21. (e2N 1)2. 2me2Nψ22 4. rΦ1ψ2. = O(1),. (1.24). ... To see this, observe that by (1.24) and the preceding remarks, the equationF(l,Q,N, Φ1,ψ2; 0) = 0 amounts to. -
Twistor theory and differential equations
www.damtp.cam.ac.uk/user/md327/jphysa09.pdf17 Sep 2009: It has been developed over the last30 years by the Oxford school of Penrose and Atiyah with the crucial early input from Ward[24, 25] and Hitchin [10, 11] and further ... Sächs. Akad. Wiss. Leipzig, Maths. Nat. Kl 69 262–77[24] Ward R S 1977 On -
Digital Object Identifier (DOI) 10.1007/s00220-009-0861-xCommun.…
www.damtp.cam.ac.uk/user/md327/DP09.pdf27 Jul 2009: 4.25)We now consider the reduction of the system (4.23),(4.24). Theorem 1.1 arises as acorollary of Proposition 4.2. ... to a coupled system whichincludes the Z3 two dimensional Toda chain [24] as a special case. -
PII: 0377-0257(91)87016-Q
www.damtp.cam.ac.uk/user/hinch/publications/JNNFM40_323.pdf13 Jul 2009: Lipscombe, R. Kennings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85 [l]). ... References. 1 G.G. Lipscomb, R. Keunings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85-96. -
The millennial atmospheric lifetimeof anthropogenic CO2 David Archer…
www.damtp.cam.ac.uk/user/mem/archer-carbon-tail08.pdf30 Aug 2009: 2007) 24–26% 40%(Ridgwell and Hargreaves 2007) 34%(Montenegro et al. 2007) 52%. ... Ambio 24(6):376–378Torn MS, Harte J (2006) Missing feedbacks, asymmetric uncertainties, and the underestimation of future. -
Chlamy_science_full
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Polinetal09.pdf31 Jul 2009: www.sciencemag.org SCIENCE VOL 325 24 JULY 2009 489. REPORTS. on. July. ... 24 JULY 2009 VOL 325 SCIENCE www.sciencemag.org490. REPORTS. on. July. 24,. -
IOP PUBLISHING FLUID DYNAMICS RESEARCH Fluid Dyn. Res. 41 ...
www.damtp.cam.ac.uk/user/ngb23/publications/fdr09.pdf3 Sep 2009: V|ψ|2 dx = ψ2u v, (24). where v =. V dx, and by ψ the wavefunction of the bulk: ψ ψ as r. ... For thequartic term in the expression for the energy, we write using equation (24). -
Noise and Synchronization in Pairs of Beating Eukaryotic Flagella ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/GoldsteinPolinTuval09.pdf16 Oct 2009: An estimate of the hydrodynamic coupling between twoidealized flagella [24] is est ’ rRL. ... E.Goldstein, Science 325, 487 (2009). [24] T. Niedermayer, B. Eckhardt, and P. -
Effective dynamics for solitons in the nonlinear Klein Gordon ...
www.damtp.cam.ac.uk/user/dmas2/public_ps/dl_final.pdf15 Oct 2009: Theorem 8 ([24]) If the nonlinearity satisfies the conditions given in 1.3.2 then (POS) is true. ... 24). The stabilityis in the same sense as in the previous theorem, see [17] for full details. -
VOLUME 80, NUMBER 4 P H Y S I ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysRevLett.80.704.pdf10 Jul 2009: For the same trial as in Fig. 5, this constantB is found to be20.90 and 24.29 for the large andsmall angle sides, respectively. -
http://journals.cambridge.org Downloaded: 31 Jul 2009 IP address:…
www.damtp.cam.ac.uk/user/hinch/publications/JFM66_1.pdf31 Jul 2009: SZAN-IAWSKI, A. 1972 Arch. Mech. 24, 555. TANNER, R. I. 1971 J. -
Buoyancy driven miscible front dynamics in tilted tubesT. Séon,a! ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_17_031702.pdf8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex, 05, France. ... Rev.Fluid Mech. 24, 21 s1992d. 12F. Viana, R. Pardo, R. Yanez, and J. -
Instability of a high-speed submerged elastic jet
www.damtp.cam.ac.uk/user/hinch/publications/JFM288_311.pdf14 Jul 2009: 0.24 1. 0.18. (T 0.12. 0.06. 0 a. FIGURE 2. The growth rate 0 = aci as a function of wavenumber CI for the varicose mode of a ... The dashed curves are contours of pressure. 0.24. 0.18. 0 0.12. -
98PA207
www.damtp.cam.ac.uk/user/hinch/publications/PRSLA455_3201.pdf10 Jul 2009: The displacements xn as a function of position along theline, n, at different times t = 13.5, 24.5, 35.2, and 45.7. ... The different symbols are different times: , t = 13.5; , t = 24.5; , t = 35.2; ,t = 45.7. -
PII: 0377-0257(93)80029-B
www.damtp.cam.ac.uk/user/hinch/publications/JNNFM50_161.pdf13 Jul 2009: Denn, J. Non-Newtonian Fluid Mech., 24 (1987). 85-96. 6 P.J. Coates, R.C. -
persescribeericalma- trulyinedwith CPUwith iodicpen-la-tua- ize of…
www.damtp.cam.ac.uk/user/hinch/publications/JFG000957.pdf10 Jul 2009: 1 O f 11/3! (24). Figure 3 shows the settling velocity for a simple cubic arrayspherical particles as a function off 1/3. ... It can be seen that thenumerical results, obtained by considering the finite size ofparticles, yield close agreement with the -
Buoyant mixing of miscible fluids in tilted tubesT. Séon, ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_16_L103.pdf8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex 05, France.
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