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  2. 19 Jul 2010: S. T U R N E R ET AL. T A B L E 1. ... B. Relatedfigures. 3, 4, 5, 6. A2. A2, A3. A2. 11, 12B1.B2.
  3. combine-new-not-indented-6.18

    www.phase-trans.msm.cam.ac.uk/2007/QinBo_Thesis.pdf
    7 Jun 2010: another coordinate system B, which satisfies:. [B; u’] = (B S B) [B; u]. ... A; u] = (A J B) [B; u] and [B; u’] = (B J A) [A; u’].
  4. 24 Mar 2010: 10. 002. 0.00. 5. nes. timat. ed M. ISE. (b). 100 200 500 1000 2000. ... 10. 5. 05. 0.01. 0.02. 0.03. 0.04. (b) Gaussian mixture classification.
  5. The Stiffness of Tensegrity Structures S.D. GuestDepartment of…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2011b.pdf
    22 Jun 2010: Tensegrity B (b.i and b.ii) for varying valuesof ε = t/AE. ... Pugh, A. (1976). Introduction to Tensegrity. University of California Press.,Berkeley. Roth, B.
  6. ANALYSIS II (Michaelmas 2010): EXAMPLES 2 The questions are ...

    https://www.dpmms.cam.ac.uk/study/IB/AnalysisII/2010-2011/anII_ex_2010_2.pdf
    1 Nov 2010: B}. Show thatif A and B are both closed and one of them is bounded then A B is closed. ... b) Is the space R[0, 1] of integrable functions on [0, 1], equipped with the uniform norm, complete?
  7. report.dvi

    www.phase-trans.msm.cam.ac.uk/2003/delrome.report.pdf
    7 Jun 2010: Is the final generation or has accuracy been met? Selection. 8 &. B! "! $. (. =%. >-@. >@. =%? %. > @ >B@. ... B. > B /@ &111. '111 C. &111. 2.
  8. An introduction to Kato's Euler systemsA. J. Scholl to ...

    https://www.dpmms.cam.ac.uk/~ajs1005/preprints/euler.pdf
    29 Jan 2010: X. Then hai: (X=B; [N]H) 7! (X=B; [aN]H) is an automor-phism of YH. ... 7!(X=B; [aN]H;z).Recall also [18, (9.4.1)] that the eN pairing denes a morphismeN : YH!
  9. Invpend.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2010_05.pdf
    4 May 2010: p′0,0 =. (. 0 1k b. ). p0,0, p0,0(0) = x(0),. ... b. b. lθ(t). y(t). 1. Figure 4: The inverted pendulum. The top position, corresponding to θ = 0, isunstable, but can be rendered stable by adding a fast vertical
  10. 7 Jun 2010: OP?:>OTU>YV=9?:=9UhJ=s_=aaJLMzC>=aMLaHLOPeg=9CvOPU)c<dQRbJS=aHkbl;<>OPMc<dQIbJL=9H%>HN=9MN=9UhJSMJS<b=?B=sJS<>ADC>M ... AVU5ZoQIMn=s¤i>EPQIOPUb=9C>HN=aDOPAVbMLETtIlÛrbHLOPUbYÎJS<>=0Ub=s¤DJWJSOT?B=BMNJS=a}];OßÞ C>HSQZ7MQRHLegAVUFGHLAV?
  11. An exact theory of nonlinear waves on a Lagrangian-mean flow

    www.damtp.cam.ac.uk/user/mem/andrews-mcintyre-glm-jfm78.pdf
    22 Jul 2010: Further properties of J and K j j. Appendix B. Derivation of theorem I. ... v?,, = (v,tF (v,jF q , t , m,i = (v,$ q , i 9 (2.4u, b ). B(x, t ) = x E(X, t ) , (2.6). (vii) The mapping (2.2)
  12. c h r i s t ’s c o ...

    https://alumni.christs.cam.ac.uk/file/2010-Magazine.pdf
    13 Oct 2010: L i b r a r y P r o j e c t. ... . S e n i o r M e m b e r s.
  13. (M16-revision)

    www.phase-trans.msm.cam.ac.uk/M16/M16-revision.pdf
    7 Jun 2010: Nis the total number of atoms and x the fraction of B atoms. ... 2, BB bonds 12 zNax2 and A–B bonds zNa(1 x)x. where z is the co–ordination number.
  14. werhist-main.2.eps

    mi.eng.cam.ac.uk/~mjfg/thesis_ckr21.pdf
    10 Jun 2010: frequency cepstral features. xtd =. 2. B. B. b=1. log(mtb) cos. (. ... πd. B(b 0.5). ). (2.4). where xtd is the dth cepstral coefficient for tth frame.
  15. Spatial pattern formation and polarization dynamics of a…

    www.damtp.cam.ac.uk/user/ngb23/publications/spinor-josephson.pdf
    27 Jun 2010: In such a basis, a full 2. PHYSICAL REVIEW B 81, 235302 2010. ... with the analogous equation for R following by replacingL R and B B.
  16. HIGH STRENGTH AND GOOD DUCTILITY OF BULK NANOSTRUCTURED META-STABLE…

    www.phase-trans.msm.cam.ac.uk/2005/LINK/154.pdf
    7 Jun 2010: The second process (Fig. 1(b)) was designed to refine the grain size further through the recrystallization of reversed austenite deformed by warm rolling. ... 4 (b). But the homogeneity of the grain sizes seems to be decreased compared with the grains
  17. �� ������ �� � ���� ��� � ���� � ...

    www.phase-trans.msm.cam.ac.uk/2005/titanium.Wei.JMST.2005.pdf
    7 Jun 2010: 4:-= >? #0! @:. ;! < : '::A :A:' =! $$0! @:. ;( < : :: = >>@! $0BB?:. ;B < :9/ : $$ : -, C: ::2 =! 0! (:. ; < :: :- :" $ :: &: :' :D=! ... 0@? >:. ;E < A: :' :6: A:= >B 0(! :. ;? < A: :' :6: A: 6:: = >(0E! @(:. ;@ < 9 , '= >@ % 4?:. ;> <
  18. THE HESSIAN OF A GENUS ONE CURVE TOM FISHER ...

    https://www.dpmms.cam.ac.uk/~taf1000/papers/g1hessians.pdf
    25 Nov 2010: Our choice of (a : b) now forces γ to be a scalar matrix. ... 2t S2st2 S3t. 3. adj(s(adj A) t(adj B)) = a2As3 aT1s2t eT2st.
  19. 7 Jun 2010: Then, Eq.(2) is modified to the following equitation,. surf b b p p a a fE (A A A ) V= ε ε ε. ... Fig.1 OM microstructure, (a) and (b) and SEM microstructure, (c) and (d) of theternary steel.
  20. 7 Jun 2010: Ü ª£ b=@n tij!tnehu21  u[4305)687 o!Ü µ nzehm|g»x3bdc!lgil|elÓgicºmgiegc!{. ... n lgipnemgÅPehw!u3bdm|Àl|bn cfÀehu¡kehsbbd»Pl|w!bdj!tio7o!b à Õ!
  21. UNIVERSIDAD COMPLUTENSE DE MADRID FACULTAD DE CIENCIAS FÍSICAS…

    www.phase-trans.msm.cam.ac.uk/2004/CMisc/Caballero.pdf
    7 Jun 2010: APÉNDICE B………………………………………………………………………… B/1-9. APÉNDICE C………………………………………………………………………… C/1-10. Introducción. 1. Introducción. La

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