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  2. Preprint typeset in JHEP style - PAPER VERSION June ...

    www.damtp.cam.ac.uk/user/tong/tasi/tasi.pdf
    24 Apr 2008: 1.4 The ADHM Construction 20. 1.4.1 The Metric on the Higgs Branch 23. ... 20 –. of the D(p 4)-brane [3, 5]. They are the same object!
  3. Mathematical Tripos: IA Vector Calculus Contents 0 Introduction i ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/VC_2000.pdf
    17 Jan 2008: whenever this limit exists. Remarks. • It follows from (1.20) and the definition of a partial deriva-tive (1.14) that. ... To derive (1.52) start from the definition of a directional derivative (1.20), and use the definition of.
  4. cowley.dvi

    www.damtp.cam.ac.uk/user/sjc1/papers/ictam2000/long.pdf
    25 Sep 2008: while the kinematic equation yieldsu = @x@t ; v = @y@t : (20)Van Dommelen & Shen (1980) made the key observation that (19) de-pends only on x and u, and hence that ... 19) and the rst of (20) can besolved independently of the equations governing y and v.
  5. ia-dyn-problems1.dvi

    www.damtp.cam.ac.uk/user/reh10/lectures/ia-dyn-problems1.pdf
    26 Feb 2008: 1 Two cyclists start 40 km apart and head towards each other, each going at a steadyrate of 20 km per hour.
  6. Worked ExampleA Ping-Pong Ball Bouncing on a Plane A ...

    www.damtp.cam.ac.uk/user/reh10/lectures/ia-dyn-handout11.pdf
    25 Feb 2008: l1 =2V 21 sin θ1 cos θ1. g=. 2eV 20 sin θ0 cos θ0g. = ... L =. n=0. enl0 =2V 20 sin θ0 cos θ0. g(1 e).
  7. Chapter 3 Dimensional Analysis 3.1 Power Laws It is ...

    www.damtp.cam.ac.uk/user/reh10/lectures/ia-dyn-chapter3.pdf
    26 Feb 2008: f (x1)f (x2). =f (αx1)f (αx2). 20. for any α. (If we changed our units of length from metres to centimetres, for instance, we would haveα = 100.).
  8. 5 May 2008 National Transport Information Incubator (NaTII) Enabling…

    www.damtp.cam.ac.uk/user/pvl/natii_publication.pdf
    13 Jun 2008: It focuses on:.  visual and simple.  the fact that the first 20% of effort gets 80% of the result.
  9. 1 Feb 2008: 0 10 20 30 40 50 600. 5. 10. 15. 20. ... 3è1V6ñEG;=1"J /. i>31Vð@6:v3EF<@> <Cç35è1ENêïé-DF;1þ:C>-A 17>1V6ð"õÂ651V;éDN35;zEF> :@>. 5. 0 10 20 30 400.
  10. Spontaneous Rotating Vortex Lattices in a Pumped Decaying Condensate…

    www.damtp.cam.ac.uk/user/ngb23/publications/polariton.pdf
    11 Aug 2008: AdaptingEqs. (4) and (5) for a rotating solution [20] gives. r r r Rr; (6). ... 15. 20. 25. 30. 35. µ. FIG. 3 (color online). Chemical potential as a function ofpumping spot size R.
  11. Condensation of Classical Nonlinear Waves in a Two-Component System…

    www.damtp.cam.ac.uk/user/ngb23/publications/2compCond.pdf
    7 May 2008: We note that in contrast to the kinetic equations pre-sented in [19] and [20] for the one-component case, Eq. ... 20] C. Connaughton, and Y. Pomeau, C.R. Physique 5 5, 91 (2004).[21] S.

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