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27 Jan 2013: The rail pads andbearings are modelled as continuous resilient layers of stiffness ka and kb respectivelyper unit length [6]. ... G̃a = ka(Ỹ1 Ỹ2) (2.44). 18. 2.2. Modelling the track. The joining condition between the slab and tunnel invert results

28 Jan 2013: Vibration from underground railways. A dissertation submitted to the University of Cambridge. for the degree of Doctor of Philosophy. by. Mohammed Farouk Mohammed Hussein. Girton College. December 2004. To my parents. ii. Preface. The work described

10 Nov 2013: ka†k. )] O(N. 1/20 ). cf. quantum AF in spin-wave approximation. ... 2. (akak a. †ka†k. )]As with quantum AF, Ĥ diagonalised by Bogoluibov transformation:(.

22 May 2013: Theorem 4.2. The vector of mean hitting times kA = (kAi : i I) is the minimalnon-negative solution to the system of linear equations. {. ... 4.1). Proof. First we show that kA satisfies (4.1). If X0 = i A, then HA = 0, so kAi = 0.If X0 6 A, then HA 1, so

2 Jan 2013: Population Genomics of the Wolbachia Endosymbiont inDrosophila melanogasterMark F. Richardson1¤a, Lucy A. Weinert2, John J. Welch3, Raquel S. Linheiro1, Michael M. Magwire3¤b,. Francis M. Jiggins3, Casey M. Bergman1. 1 Faculty of Life Sciences,

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

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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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

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