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  2. Dr David Stuart

    www.damtp.cam.ac.uk/user/dmas2/
    23 Nov 2012: Recent publications Effective dynamics for solitons in the nonlinear Klein Gordon Maxwell system and the Lorentz force law (PDF, 423KBytes).
  3. omg4.dvi

    www.damtp.cam.ac.uk/user/tong/statphys/omg4.pdf
    11 Jan 2012: Statistical Physics: Example Sheet 4. David Tong, March 2012. 1i. By examining variations in E, F , H and G, derive the four different Maxwell. ... Hint:You will need to use a Maxwell relation). iii. What is µJT for an ideal gas?
  4. 19 Jan 2012: Exercise: Derive equations (1) and (2). For the latter you will require the Maxwell relation. ... or E = uB Jσ. From Maxwell’s equations we then obtain the induction equation.
  5. N21b.dvi

    www.damtp.cam.ac.uk/user/examples/N21b.pdf
    31 Oct 2012: Using Cartesian coordi-nates, calculate the electric current density J given by the steady Maxwell equation B = µ0J.
  6. Holographic Dual of the Lowest Landau Level David Tong ...

    www.damtp.cam.ac.uk/user/tong/talks/hololll.pdf
    15 Oct 2012: 3. and the gauge fields dictated by a two-dimensional Maxwell action in curved space. ... and the gauge fields dictated by a two-dimensional Maxwell action in curved space.
  7. What Would Newton Do? David Tong Adams Society, November ...

    www.damtp.cam.ac.uk/user/tong/talks/newton.pdf
    9 Nov 2012: It was first published in a book by Maxwell, who gave credit to Hamilton.
  8. P H Y S I C A L R ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Hatwalneetal04.pdf
    2 Sep 2012: On approachingan orientationally ordered state, active suspensions with. 0031-9007=04=92(11)=118101(4)$22.50 . Maxwell-like viscoelasticity.
  9. VOLUME 84, NUMBER 13 P H Y S I ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/WuLibchaber00.pdf
    2 Sep 2012: Experimentally Py was foundto obey the Maxwell’s distribution, Py 2jyj. y20exp2 y.
  10. B6c.dvi

    www.damtp.cam.ac.uk/user/examples/B6c.pdf
    8 May 2012: to the functional I[A] =. (E2 B2)dxdt. (This gives two of Maxwell’s equations).16.
  11. Op#cal Conduc#vity from a Holographic La8ce Based on work ...

    www.damtp.cam.ac.uk/user/tong/talks/optical.pdf
    7 Jun 2012: and Maxwell field has twice the lattice wavenumber. For Nx grid points along the x-direction,a Fourier grid can only hope to resolve up to |kmax| Nx/2.
  12. Part II Applications of Quantum MechanicsLent 2012 Prof. R.R. ...

    www.damtp.cam.ac.uk/user/rrh/notes/aqm_notes_180112.pdf
    8 Mar 2012: Part II Applications of Quantum MechanicsLent 2012. Prof. R.R. Horgan. March 8, 2012. Contents. 1 The Variational Principle 1. 1.1 Estimating E0. 1. 1.2 Accuracy. 2. 1.3 Evaluation of 〈ψ|H|ψ〉. 21.4 Further Results. 3. 2 Bound States and
  13. PCE845.fm

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Pickard03.pdf
    2 Sep 2012: Second, ionic mobility is relatedto ionic diffusivity by way of the Einstein relation, which isvery general and should hold given only the applicabilityof Maxwell–Boltzmann statistics to the charged entity(Ashcroft &
  14. lectures2012.dvi

    www.damtp.cam.ac.uk/user/phh/mathbio/lectures2012.pdf
    6 Jun 2012: as Newton’s Second Law, Maxwell’s equations, the Schrödinger equations, which can be.
  15. doi:10.1016/j.physrep.2003.08.001

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/vansaarloos.pdf
    31 Oct 2012: Available online at www.sciencedirect.com. Physics Reports 386 (2003) 29 – 222www.elsevier.com/locate/physrep. Front propagation into unstable states. Wim van Saarloos. Instituut-Lorentz, Universiteit Leiden, Postbus 9506, 2300 RA Leiden, The

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