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www.damtp.cam.ac.uk/user/mem/papers/LHCE/2.pdf19 Oct 2013: "# $ $ %& ' '! (# ) (# %. , , , , -. -. - - /10324052468789:2<;-= - - - > ,@? - - - - - -. -. -. -= -= -. -.A , , , , B B(C. ... D8EGF#. % H IJIH&. D8EGF#% % IJI $ , , , , - K= -= -. LNMPO ;. - -. - QA , , , , B B RSR- - - -. -. -T. VUXW Y Y H& H H, , , , -
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www.damtp.cam.ac.uk/user/mem/papers/LHCE/7.pdf19 Oct 2013: " # # $ $ $ $&% $ ' ( '' ' '' ' '' ' ),.-'' ' ( '' ' ( '' ' '( ' / / ' '0 $ $ $ $ 1/ '32 '"4. 11 576 ' ' ' '98. # # : # # ; # # < = >@?BADC9A"CFEHGHIJC. > ; < ; : < =? BADC9A"CFEHGHIKC 0 $ $ $ $ ' ' ' ' / L '( / 2 M5N5PORQTSUQVSXWY[ZXS. -/ ' '0 $ $ $ -
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www.damtp.cam.ac.uk/user/mem/papers/LHCE/v1.pdf19 Oct 2013: d T T T TV V V V V. b V VW V VX V V V V V VX VT e TgfV VX V V. ... h?h T T T TikjmlnjolEp [:q l VX VX b b VX Vc VX V r!s t. -
Mathematical Tripos Part II Michaelmas term 2007Further Complex…
www.damtp.cam.ac.uk/user/md327/fcm_5.pdf6 Mar 2013: b. Thus two linearly independent solutions of Legendre’s equation can be written, in the casewhen m is not an integer (so that the exponents at the origin do not differ ... a(a 1)b(b 1). c(c 1). z2. 2! 2. -
No many-scallop theorem: Collective locomotion of reciprocal swimmers …
www.damtp.cam.ac.uk/user/lauga/papers/23.pdf26 Jul 2013: b) Two dimers. We now consider the case of two dimersa and b. ... 482 2d3, 3a. V = ̄ab2 b1b1b2. ̄ba2 a1. a1a2 f a f b. -
Microstructural studies for rheology ◮ Micro & macro views ...
www.damtp.cam.ac.uk/user/hinch/teaching/nnfm/part7bhandout.pdf19 Aug 2013: Rotation of particles – rigid and dilute. Spheroid: axes a, b, b, aspect ratio r = ab. ... Averaged stress. σ = pI 2µE 2µφ[AE : 〈pppp〉. B(E 〈pp〉 〈pp〉E) CE FDrot〈pp〉]. -
REDUCED CONSISTENCY SAMPLING IN HILBERT SPACES Ben Adcock1, Anders ...
www.damtp.cam.ac.uk/research/afha/anders/AdcockHansenSampTA.pdf5 Oct 2013: Toquantify this, we consider the condition number κ(B) =‖B‖‖B1‖. The following lemma is also found in [2]:. ... Technical reportNA2010/07, DAMTP, University of Cambridge, 2010. [2] B. Adcock and A. -
Orientational order in concentrated suspensions of…
www.damtp.cam.ac.uk/user/lauga/papers/61.pdf26 Jul 2013: 3(b) denoting the 1=. ffiffiffiffiN. pisotropy. that is expected in our system. ... The case shown is for a puller swimmer (b 1) witha volume fraction / 0.01. -
Gauge Dynamics and Topological Insulators David Tong Back in ...
www.damtp.cam.ac.uk/user/tong/talks/gtop.pdf18 Jul 2013: B B. However, for our non-Abelian magnetic field, B B is simply a gaugetransformation. ... B. 2 ξi (k)0. (1.1). ψi =4. B. 2π. dk. 2πexp. -
REDUCED CONSISTENCY SAMPLING IN HILBERT SPACES Ben Adcock1, Anders ...
www.damtp.cam.ac.uk/research/afha/people/anders/AdcockHansenSampTA.pdf5 Oct 2013: Toquantify this, we consider the condition number κ(B) =‖B‖‖B1‖. The following lemma is also found in [2]:. ... Technical reportNA2010/07, DAMTP, University of Cambridge, 2010. [2] B. Adcock and A.
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