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11 - 20 of 27 search results for `B b cos`

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  2. Delivered by ICEVirtualLibrary.com to: IP: 129.169.110.8 On: Tue, 02…

    www-civ.eng.cam.ac.uk/geotech_new/people/bolton/mdb_pub/208.pdf
    2 Aug 2011: It can be shown that. D B sin cos eŁ tan. ... Dc B cos e tan. 2 cos =4 þ =2ð Þ sin =4 =2ð Þ (3).

  3. INSTITUTE OF PHYSICS PUBLISHING NONLINEARITY Nonlinearity 18 (2005)…

    www.damtp.cam.ac.uk/user/gold/pdfs/spin.pdf
    10 Apr 2011: B s =(. η2. 4 ζ 2. )1/2 [Bx sin ω By cos ω. ] ... s = η2. [sin θ sin ωx̂ sin θ cos ωŷ cos θ ẑ. ].

  4. Flows driven by flagella of multicellular organismsenhance long-range …

    www.damtp.cam.ac.uk/user/gold/pdfs/flagflows.pdf
    10 Apr 2011: In a coordinate system moving at the speed of the colony, theradial and polar velocities are ur U[(c x3)cos A(x, )]and u U[(d x3)sin B(x, )], ... B 254, 107–113.12. Berg, H. C. & Purcell, E. M. (1977) Biophys.

  5. An isoperimetric inequality for the Wiener sausage Yuval Peres∗ ...

    www.statslab.cam.ac.uk/~ps422/wienergafa.pdf
    26 Oct 2011: f0R(x) =1(x B(0,L cnε))cos(α(x))µ(C(L)). ,. where α(x) is the angle between π1(x) and (0,. ... f1R(x) =1(x π(C(ζ(0),ε)))cos(α(x))µ(C(ζ(0),ε)). and ξ(1) has density function given by. f1(x) =1(x

  6. NATURAL SCIENCES TRIPOS Part II Wednesday 19 January 2011 ...

    www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam11sol.pdf
    24 Jan 2011: 2. (2P1 cos(ωt ϕ) Q2. )py =. α. 2. (2P1 sin(ωt ϕ) P2. ... µ and WµWµ. The coefficients are. m2. λ[e cos α e′ sin α].

  7. INSTITUTE OF PHYSICS PUBLISHING NONLINEARITY Nonlinearity 14 (2001)…

    www.damtp.cam.ac.uk/user/gold/pdfs/quantray.pdf
    10 Apr 2011: as a Fourier series:. R(z) = R0(. 1. 0dq b(q) cos(qz φ(q)). ... Our aim is to expand up to second orderin the coefficients b(q) characterizing the deformation.

  8. Mathematical Tripos Part III 2007–08Fundamentals of Atmosphere–Ocean…

    www.damtp.cam.ac.uk/user/mem/III-NOTES/mcintyre-fund-atm-oc-dynamics-exs-4.pdf
    15 Jul 2011: ψ′ = Re. [. N 2H. f0 m sin(mH)eikx sin(ly) cos{m(z H)}. ]. ... ψ′ = Re[. eikx sin(ly){. B (t t0) cos(mz) C (z H) sin(mz)}]. ,.

  9. Topographical complexity of multidimensional energy landscapes Tamiki …

    https://www-wales.ch.cam.ac.uk/Telluride.papers/rlj_06_5.pdf
    13 Jan 2011: CP, Vi m. pbn,mVi log p b n , m V i , [5]. ... Berry RS, Elmaci N, Rose JP, Vekhter B (1997) Proc Natl Acad Sci USA.

  10. PHYSICS OF FLUIDS VOLUME 10, NUMBER 11 NOVEMBER 1998 ...

    www.damtp.cam.ac.uk/user/gold/pdfs/pinching.pdf
    10 Apr 2011: 2 ix1 (uku>2. ĥkeikx. 5 h̄1uĥ1uS 2 cos x1 f! 1 (uku>2. ... h x,t 5 0!5 h̄ 11 a cos x!, 0<x<2p. 58!

  11. examples.dvi

    https://www.hep.phy.cam.ac.uk/~thomson/partIIIparticles/examples/examples_2011_sheet_2.pdf
    24 Oct 2011: 1 cos θ2 (E3/E1)(1 cos θ). ]. whereθ is the angle through which the positron has scattered. ... b) The Lorentz invariant matrix element forπ µνµ decay is. Mf i =g2W.

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