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1 - 10 of 16 search results for KA :PC53 |u:www.damtp.cam.ac.uk where 0 match all words and 16 match some words.

  1. Results that match 1 of 2 words

  2. GRAVITY WAVE GENERATION BY VORTICAL FLOWS IN A ROTATING ...

    www.damtp.cam.ac.uk/user/mem/papers/SSREPLY/rupert-ford-thesis93.pdf
    19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret

  3. pnas201210548 1..6

    www.damtp.cam.ac.uk/user/gold/pdfs/ciliary_contact_plus_SI_online.pdf
    7 Jan 2013: Phys Rev Lett 105(16):168101. 17. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

  4. GRAVITY WAVE GENERATION BY VORTICAL FLOWS IN A ROTATING ...

    www.damtp.cam.ac.uk/user/mem/oldftp/rupert-ford-thesis93.pdf
    19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret

  5. doi:

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Hewitt-2013-1.pdf
    28 Nov 2013: J. Fluid Mech. (2013), vol. 737, pp. 205–231. c Cambridge University Press 2013 205doi:10.1017/jfm.2013.559. Stability of columnar convection in a porousmedium. Duncan R. Hewitt1,†, Jerome A. Neufeld1,2,3 and John R. Lister1. 1Institute of

  6. pnas201210548 1187..1192

    www.damtp.cam.ac.uk/user/gold/pdfs/ciliary_contact.pdf
    3 Feb 2013: Phys Rev Lett 105(16):168101. 17. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

  7. � ������� �� ����������������� ���������! "�#���%$ &���' …

    www.damtp.cam.ac.uk/user/mem/oldftp/polarcool.pdf
    19 Oct 2013: ó ö ëLë BnF í öJLFLö-K ëlê D[F é KÁ@ òóí ø ê @pöFWK5î ð ø¥FWJö5ñ ê¥ò ø¥KpF ý ñ êÒëLê û#ø¥K¿ö-Dî ê Dù0JöJK5î[Jö-î ... ïí K5î ê F ê¥ò D ë F é öF@ ò D ú J ó K5îF é KÄ@pö ð ë K ëÁò ùbF é K

  8. The decay of stabilizability with Reynolds number in a linear model…

    www.damtp.cam.ac.uk/user/lauga/papers/3.pdf
    26 Jul 2013: ¤ and compute a matrix F with components fij = cij =( i ¤j ).The minimal-energy stabilizing feedback controller is then given by u = KÀ , whereK = B ¤ F ¡1.

  9. ��������� ��� ����������������������� �����…

    www.damtp.cam.ac.uk/user/mem/oldftp/airsea-negvisc.pdf
    19 Oct 2013: J<6{4)01# "9#mI =9? : : "9#r=:; DJzG=x? 0- I?6,z#1 Kj BKj'Kä :6#(8º Jz0 G= 8G? ... 6'? ] BKj0G=>=# Kj Km'Kä :#I =º? :;81#G5#6: º#=>c0- "GG "(8º J= G= 0G=º# Km Kj'EKà :#c X8Ñ?

  10. §4 FLOWS WITH A FREE SURFACE Such flows are ...

    www.damtp.cam.ac.uk/user/mem/FLUIDS-IB/waves.pdf
    19 Oct 2013: iσζ̂ kA sinh kh = 0. and from the second (pressure) (). gζ̂ iσA cosh kh = 0. Regarding these as a system of two linear algebraic equations for the two unknown constants ζ̂

  11. flm563.dvi

    www.damtp.cam.ac.uk/user/mem/papers/RECOIL/remote-recoil.pdf
    19 Oct 2013: Another importantwave activity measure is given by the pseudomomentum vector,. p = kA =h′ u′. ... Because of the ray-invariance of absolute frequency we have that |kA| = |kB | asympto-tically.

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