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  2. Two-axis unicycle simulation and control

    https://www.hep.phy.cam.ac.uk/~lester/teaching/PartIIIProjects/2011-NickStenning-REPORT-final-version.pdf
    1 May 2014: 2 sin χ 2AD sin χ/C cos χC cos χ 4AB/C cos χ. ... See Appendix B for the full equations of motion. NB: cξ = cos ξ and sξ = sin ξ.
  3. DIFFERENTIAL GEOMETRY EXAMPLES 2 P.M.H. Wilson, Lent 2014…

    https://www.dpmms.cam.ac.uk/study/II/DifferentialGeometry/2013-2014/dg14.2.pdf
    4 Feb 2014: φ(s,v) = α(s) r(n(s) cos v b(s) sin v)where n = n(s) and b = b(s) are the normal and binormal vectors of α. ... 9. Consider a surface of revolution parametrized by φ : (0, 2π) (a,b) R3, whereφ(u,v) = (f(v) cos u,f(v) sin u,g(v)).
  4. Weighted frames of exponentials and stable recovery of…

    www.damtp.cam.ac.uk/research/afha/anders/2DNonuniformSamplingArXiv13May14.pdf
    31 May 2014: The weighted framebounds A,B > 0 satisfy. A 2 e2πδB1d,. B e2πδB1d < 2. ... ω B(ω̃), |f̂(ω)| |f̂(zω̃)|. Since also µω = meas(V E. ω.
  5. pnas201217998 3276..3281

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2013GuestD.pdf
    6 Feb 2014: S = b cos θ tan γffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi1 cos2θ tan2γ. p ; [2]. ... cos γA1cos γB1. =cos γA2cos γB2. [21]. must be satisfied to enable stacking.
  6. 4 The Heat Equation Our next equation of study ...

    www.damtp.cam.ac.uk/user/dbs26/1BMethods/Heat.pdf
    4 Nov 2014: as. Θ(0, t) = Θ0 A cos (2πt/tD) B cos (2πt/tY) (4.30). – ... We can solve these as. X(x)T(t) =[a sin(. λx) b cos(.
  7. ANALYSIS II—EXAMPLES 1 Mich. 2014 Please email comments, corrections…

    https://www.dpmms.cam.ac.uk/study/IB/AnalysisII/2014-2015/14sheet1.pdf
    20 Oct 2014: 4. Let (fn) be a sequence of real-valued continuous functions on a closed, bounded interval [a,b], and. ... m=1 mam cos mx. (b) Show that f(x) =. m=1 am sin mx defines a continuous function on [π,π], but that the seriesm=1 mam cos mx need
  8. p250

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/250.pdf
    28 Jan 2014: 5. Define.  . . . . cos/cos/ 2. 2220 1. ... 2006). Acta Mat., 54, 1297-1306. Kachanov, M., Sevostianov, I. and Shafiro, B.
  9. Part IA Engineering Mathematics: Lent Term 2.5cm Convolution 0.1cm…

    www-sigproc.eng.cam.ac.uk/foswiki/pub/Main/1AMathematics_2013/IAMaths_Sections5_8_2014.pdf
    12 Feb 2014: f (t) = a0. n=1. (an cos(nt) bn sin(nt)). =. n=1. ... f (t) = a0. n=1. (an cos(nt) bn sin(nt)). =eπ eπ.
  10. November 2014 EPL, 108 (2014) 34003 www.epljournal.orgdoi:…

    www.damtp.cam.ac.uk/user/lauga/papers/100.pdf
    5 Nov 2014: When small-amplitudewaves propagate along ex, the surface of the cylinder is de-scribed by r̂ = [h(s, t) b cos φ]ey b sin φez sex and the. ... p̃ ηωh̃i cos θAK1(kr)ũr h̃ωi cos θ[αArkK1(kr) BK2(kr) CK0(kr)]ũθ h̃ωi sin θ[BK2(kr)
  11. 28 Nov 2014: f ′′cot θf ′6f =A cos θ B. (2.14)Together with the particular solution, the full solution is then ψ = cr3(at bt3 1)for t =cos θ. ... The function H(ν) is plotted for cone angles in figure 1(b).
  12. Arbitrary–order trigonometric Fouriercollocation methods for…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2014_03.pdf
    23 Oct 2014: ui(0) = sin( πxi. b. ), u′i(0) =. π. b. gd(xi) cos. ( ... b. gd(xN ) cos. ( πxNb. ))T,. (39). where U (t) denotes the N -dimensional vector with entries ui(t) u(xi, t),.
  13. Noname manuscript No.(will be inserted by the editor) Numerical ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_09.pdf
    22 Dec 2014: eπ2. sinh(π) j = 0,. j cos( jt)sin( jt)π2. j21. j Z+. ... a = 0, b = π, (t [0,π],q(t) = 20 cos(2t)), α1 6= 0, β1 6= 0, α2 = β2 = 0,.
  14. 5 The Wave Equation Waves are extremely common in ...

    www.damtp.cam.ac.uk/user/dbs26/1BMethods/Wave.pdf
    9 Nov 2014: 2. V (t) =µπ2c2. 4L. n=1. n2[An cos. (nπct. L. ) Bn sin. ... m=1. i=1. [Cmi cos mθ Dmi sin mθ] cos(kmict) Jm(kmir). (5.32).
  15. D15a.dvi

    www.damtp.cam.ac.uk/user/examples/D15a.pdf
    14 Oct 2014: obtain:. Φ(ϕ) = A sin(λϕ) B cos(λϕ),. with positve constants A, B. ... Aλrλ Bλr. λ) sin(λϕ) (Cλrλ Dλr. λ) cos(λϕ). E0 F0 ln(r).
  16. Part III: Biological Physics (Michaelmas, 2014) R E Goldstein ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/BiologicalPhysics201415_Examples2.pdf
    13 Oct 2014: b) Now consider an almost ideal FJC with N monomers of type a. ... Show that these can be written as. W(n)(x) = A cos(k(n)x) B sin(k(n)x) D cosh(k(n)x) E sinh(k(n)x) ,. and
  17. 29 Aug 2014: û% |r =1 = K cos(nθ ). . 0. cos φ cos θ sin φ. ... Thus, the previous equations canbe put in the form. s û% = K cos φk.
  18. Weighted frames of exponentials and stable recovery of…

    www.damtp.cam.ac.uk/research/afha/people/anders/2DNonuniformSamplingArXiv13May14.pdf
    31 May 2014: The weighted framebounds A,B > 0 satisfy. A 2 e2πδB1d,. B e2πδB1d < 2. ... ω B(ω̃), |f̂(ω)| |f̂(zω̃)|. Since also µω = meas(V E. ω.
  19. The Nonlinear Graviton as anIntegrable System � Maciej Dunajski ...

    www.damtp.cam.ac.uk/user/md327/dunajski_thesis.pdf
    6 Nov 2014: The Frobenius integrability condition yields. [X,Y ] = aX bY. for some a and b. ... 2.14). Let ΣA′B′ be the usual basis of SD two forms.
  20. The hydrodynamics of swimming microorganisms

    www.damtp.cam.ac.uk/user/lauga/papers/32.pdf
    9 Sep 2014: fprop = (ξ‖ ξ)u sin θ cos θ ex. (13)In addition, in order to generate a net propulsion from a. ... u(x, h(x, t)) = ht. ey = bω cos(kx ωt)ey , (21).
  21. PHYSICAL REVIEW E 89, 043011 (2014) Geometry and wetting ...

    www.damtp.cam.ac.uk/user/lauga/papers/88.pdf
    22 Apr 2014: dE. dα BγAL. (V. B. )2/3 [ 43C1 cos(θE )α. 1 13. ] ... B. Solving the problem. We start by rearranging Eq. (12) by differentiating onceto eliminate Ft , Fn, and M and obtain a third-order equationfor ψ ,. d3ψ. ds3+ γ cos θE. EI.
  22. Bifurcation in electrostatic resistive drift wave turbulenceRyusuke…

    www.damtp.cam.ac.uk/user/mem/oldftp/jeff-parker-numata-pp07.pdf
    13 Jul 2014: r = b. 21 162. b2 1/4 cos. 2,. i = 1. ... s = sinn. Lx n:even. cos nL. x n:odd , 16and the critical wavenumber is.
  23. PHYSICS OF FLUIDS 26, 071902 (2014) Dynamics of swimming ...

    www.damtp.cam.ac.uk/user/lauga/papers/92.pdf
    20 Jul 2014: indy =3 cos θ sin θ. 64π η1h3. [1 1. 2γ 2 1γ 2 1. ... 62). Using the same methodology as that described in Sec. IV B 2 and Appendix B, we get that,indy =. [,indy. ]0 cos2 θ ,x x cos θ sin θ ,x
  24. TH EJ OU RN AL OF CE LL BIO ...

    www.damtp.cam.ac.uk/user/sje30/papers/kishi2005.pdf
    14 Jun 2014: A and B) Neonatal diaphragmwas hybridized with probes for CD24 (A) or LL5 (B). ... Figure 7. LL5 is required for AChR clustering.(A) COS cells were cotransfected with GFP-LL5 plus control duplex VIII siRNA (left), LL5-RNAi#1 (center), or LL5-RNAi#2 (right
  25. 10 Sep 2014: χn = r nn. m=0P mn (μ)(cmn cos mφ c̃mn sin mφ). ... pn = r nn. m=0P mn (μ)(amn cos mφ ãmn sin mφ).
  26. Soft Matter and Biological Physics Raymond E. Goldstein and ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/Handout_SMB_131125.pdf
    10 Jan 2014: x =. Nn=1. b cos θN E[{θn}] = FbNn=1. cos θn. ... f cos θn f =Fb. kBT. =. [4π sinh(f). f. ]N.
  27. 24 Sep 2014: The product is exp iθ exp iφ =exp i(θ φ). (b) SO(2) =. {R(θ) =. (cos θ sin θsin θ cos θ. ): 0 θ 2π. }. ... 3.3.1 Lie Algebra of SO(2). g(t) =. (cos f(t) sin f(t)sin f(t) cos f(t).
  28. Statistical Field Theory R R Horganrrh@damtp.cam.ac.uk…

    www.damtp.cam.ac.uk/user/rrh/notes/qstat.pdf
    8 Dec 2014: P is an orthogonal matrix and has the form. P =. (cos φ sin φsin φ cos φ. ), cot 2φ = e2K sinh B. ... λr+ 00 λr. )(cos 2φ sin 2φsin 2φ cos 2φ. )(λr+ 00 0. )],
  29. D15e.dvi

    www.damtp.cam.ac.uk/user/examples/D15e.pdf
    9 May 2014: obtain:. Φ(ϕ) = A sin(λϕ) B cos(λϕ),. with positve constants A, B. ... Aλrλ Bλr. λ) sin(λϕ) (Cλrλ Dλr. λ) cos(λϕ). E0 F0 ln(r).

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