Search

29 Dec 2023: Preprint typeset in JHEP style - HYPER VERSION. Statistical PhysicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,.

25 Sep 2015: FL47CH15-Goldstein ARI 1 December 2014 20:34. Green Algae as ModelOrganisms for BiologicalFluid DynamicsRaymond E. GoldsteinDepartment of Applied Mathematics and Theoretical Physics, Centre for MathematicalSciences, University of Cambridge,

10 Nov 2017: rspa.royalsocietypublishing.org. ReviewCite this article: Atiyah M, Dunajski M,Mason LJ. 2017 Twistor theory at fifty: fromcontour integrals to twistor strings. Proc.R.Soc.A 473: 20170530.http://dx.doi.org/10.1098/rspa.2017.0530. Received: 1 August

17 Jul 2024: A gluing operator for the ambitwistor string. KA Roehrig, D Skinner. –

14 Feb 2005: Part II Statistical Mechanics, Lent 2005. Prof. R.R. Horgan. February 14, 2005. 1 Statistical Mechanics. 1.1 Introduction. The classical and quantum dynamics of simple systems with few degrees of freedomis well understood in that we know the

2 Sep 2012: 38. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

10 Apr 2011: 0.6. xc. 0.5 ---- --------Xc«Mn)a CXl)---------. 0.4. 0.4 0.5 0.6. ka T lu.

15 Jan 2024: Show that the phase shifts δl obey. tanδl =jl(ka). nl(ka). 4. ... Show that the phase shifts obey. tanδl =q jl(ka)j. ′l(qa) k j.

27 Jul 2007: K bb Ka = 12ηKa. Thus K is automatically geodesic, and if it is pure then its trajectories are parameterizedby an affine parameter.

17 Apr 2021: Preprint typeset in JHEP style - HYPER VERSION. Statistical PhysicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,.

3 Apr 2018: Vortices, Painlevé integrability andprojective geometry. Felipe ContattoQueens’ College. This dissertation is submitted for the degree of Doctor of Philosophy. Department of Applied Mathematics and Theoretical Physics. University of Cambridge.

12 Aug 2016: Representing the resonance between the modes @n,o,ka and by the label (n, k,, k,,), the solid circles represent (n, 1,l) resonances; the solid squares (n, 2,2) resonances;

25 Aug 2022: Preprint typeset in JHEP style - HYPER VERSION. F́ısica Estad́ıstica. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences. Wilberforce Road,. Cambridge, CB3 OBA, UK.

29 Jul 2007: Ka = αAβ̂A′ α̂AβA′ is a Killing vector, and deduce the form of themetric.

3 Oct 2008: Natural Sciences Tripos, Part IB. Michaelmas Term 2008. Mathematical Methods I. Dr Gordon Ogilvie. Schedule. Vector calculus. Suffix notation. Contractions using δij and ǫijk. Re-minder of vector products, grad, div, curl, 2 and their

1 Sep 2011: i j is js s, |i| :=. s. is. The following lemmas will be used frequently (see [Ka], pp.

7 Jan 2013: Phys Rev Lett 105(16):168101. 17. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

31 May 2023: Preprint typeset in JHEP style - HYPER VERSION Lent Term, 2017. Applications of Quantum MechanicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical

28 Sep 2009: respectively. These parameters ka and krare determined as the best fit parameters to the measurement. ... As parameters of the contact angle model, mda= 107, e = 90, mdr = 77, ka = 9.0 10.

28 Nov 2013: J. Fluid Mech. (2013), vol. 737, pp. 205–231. c Cambridge University Press 2013 205doi:10.1017/jfm.2013.559. Stability of columnar convection in a porousmedium. Duncan R. Hewitt1,†, Jerome A. Neufeld1,2,3 and John R. Lister1. 1Institute of

10 Apr 2011: RAPID COMMUNICATIONS. PHYSICAL REVIEW E AUGUST 1997VOLUME 56, NUMBER 2. Elastohydrodynamic study of actin filaments using fluorescence microscopy. D. Riveline,1 C. H. Wiggins,2 R. E. Goldstein,3 and A. Ott1,1Laboratoire PhysicoChimie Curie,†

5 Aug 2011: Although the strong correlationsuggests an almost constant and linear relationship, it actually appears as ifthe earliest part of the record (before about 650 ka) had lower mixing ratios(both absolutely and ... a) The last interglacial and methane. The

28 Oct 2006: This. isa. super. vis. or’. sco. py. ofth. enote. s.It. isnot. tobe. dis. trib. ute. dto. studen. ts. Natural Sciences Tripos: IB Mathematical Methods I. Contents. 0 Introduction i. 0.1 Schedule. i. 0.2 Books. ii. 0.3 Lectures. ii. 0.4 Printed

1 Sep 2011: On Lp-boundedness of the L2-projectoronto nite element spacesA. Yu. Shadrin1. IntroductionIn [Sh] we proved that, for p suciently close to 2, the Lp-norm of the L2-projector P onto the space S of polynomial splines of order k on a knot-sequence is

1 Dec 2023: T R A N S P O R T P H E N O M E N A A N D F L U I D M E C H A N I C S. On two-phase modeling of dewatering pulp suspensions. Daniel T. Paterson1 | Tom S. Eaves2 | Duncan R. Hewitt3 | Neil J. Balmforth4 |. D. Mark Martinez1. 1Department of Chemical

1 Sep 2011: TO KA-SAETSQ PORQDKA POLIGARMONINOSTI (g) = @(f)=@xj, TO, POSKOLXKU OPERACIQ DIFFERENCIRO-WANIQ SOHRANQET TOT PORQDOK, IMEEMr2(g) = 0; = m1 1 2m1 = m:pREDLOVENIE 1a0, A S NIM I SLUAJ 1a)

7 Oct 2014: Anti-Self-Duality and Solitons. Prim PlansangkateTrinity College. University of Cambridge. Department of Applied Mathematics and Theoretical Physics. Faculty of Mathematics. Supervisor: Dr Maciej Dunajski. This dissertation is submitted for the

17 Jul 2024: KA Mizerski, HK Moffatt. – Geophysical & Astrophysical Fluid Dynamics. (2018).

17 Jul 2024: R Hložek, EEO Ishida, J Guillochon, SW Jha, DO Jones, KS Mandel, D Muthukrishna, A O’grady, CM Peters, JR Pierel, KA Ponder, A Prša, S Rodney, VA Villar. –

6 Oct 2014: Anti–self–dual fields. and manifolds. Moritz F. Högner. Trinity College. Dissertation submitted for the Degree of Doctor of Philosophy. October 2012. Abstract. Anti–self–dual fields and manifoldsMoritz F. Högner. In this thesis we study

7 Apr 2021: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... v(k) =Ca. sin(ka) = Ca. sineEa. t. The Bloch frequency is! =

6 Jul 2020: Cobalt yielded an intrinsic rema-nent magnetization of $ 500 kA/m. Other magnetic materials, such asparamagnetic iron oxide, could be utilized with a stronger magneticfield.

4 Oct 2013: if ψ = 0at r = a then Rnk(a) = Jn(ka) = 0 so for each n, ka = kni with i = 1, 2,.

18 May 2022: Elastohydrodynamic Synchronization of Rotating Bacterial Flagella. Maria Tătulea-Codrean 1,2 and Eric Lauga 1,1Department of Applied Mathematics and Theoretical Physics, University of Cambridge,. Cambridge CB3 0WA, United Kingdom2Collège de France

10 May 2012: INTEGRABLE SYSTEMS. Maciej Dunajski. Department of Applied Mathematics and Theoretical Physics. University of Cambridge. Wilberforce Road, Cambridge CB3 0WA, UK. May 10, 2012. Contents. 1 Integrability in classical mechanics 41.1 Hamiltonian

13 Mar 2019: δ(r a). Show that the phase shifts are given by. tan δl = kλa2[jl(ka)]. ... 2. 1 kλa2jl(ka)nl(ka). [Hint: The δ-function leads to two continuity conditions at r = a.

2 Sep 2012: Kachar & Reese 1989; Lichtscheidl & Balu ka 2000).Nevertheless, ‘relatively little is known about the biogene-sis, dynamics, maintenance, and inheritance of the organelleitself’ (Powell & Latterich 2000). ... al. 1999); and (v) thatthe actin

10 Apr 2011: Tem- perature is T = - l/Ka, normalized to the critical coupling of the Ising model.

30 Nov 2015: Mathematical Methods. University of Cambridge Part IB Mathematical Tripos. David Skinner. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge CB3 0WA. United Kingdom. d.b.skinner

10 Nov 2014: Part III: Biological Physics (Michaelmas 2014) R E Goldstein (06/11/14). Examples Sheet #3. 1. Nonlinear Diffusion. For the nonlinear diffusion equation Ct = D(CpCx)x, where p and D. are strictly positive constants, show that the self similar

10 Jan 2017: A linear functionon T given by κ = Ka(X)Ẋ a is called a first integral if dκ/dτ = 0 when (1.1) holds, or equivalently if.

5 Sep 2012: J R Soc Interface 8:1314–1331. 22. Kurtuldu H, Guasto JS, Johnson KA, Gollub JP (2011) Enhancement of biomixingby swimming algal cells in two-dimensional films. ... J EngMath 10:287–303. 58. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows

26 Feb 2014: 20131160, published 26 February 201411 2014 J. R. Soc. Interface Kirsty Y. Wan, Kyriacos C. Leptos and Raymond E. Goldstein Lag, lock, sync, slip: the many 'phases' of coupled flagella.

19 Jan 2012: detail, including a fluctuation-rounded stretch-coil transition of actin filaments. DOI: 10.1103/PhysRevLett.108.038103 PACS numbers: 87.16.Ka, 47.63.b, 83.50.Jf, 87.15.H.

5 Nov 2014: ψ1 = Re. [. n=1. ω. ka(n)NN(1 nky)e. nkyein(kxωt)]. (9). Notably, the flow described by eq.

4 Oct 2013: Its FT is easy to calculate:. f̃(k) =. aaeikx dx =. aa. cos(kx) dx =2 sin(ka). k. (41). so by the Fourier inversion theorem we get. ... 1. π. eikxsin ka. kdk =. {1 |x| < a,0 |x| > a.

14 Nov 2016: Part III: Biological Physics and Complex Fluids (Michaelmas, 2016)R E Goldstein (02/10/16). Example Sheet #3. 1. A forced particle. A microsphere of radius a and drag coefficient ζ is constrained to movealong the x-axis, and is acted on by an

10 May 2022: Elastohydrodynamic synchronization of rotating bacterial flagella. Maria Tătulea-Codrean1, 2 and Eric Lauga1, 1Department of Applied Mathematics and Theoretical Physics,. University of Cambridge, Cambridge CB3 0WA, United Kingdom2Collège de

27 Oct 2010: k CkA BkeMjtt0j1M ka bkeMjtt0jwhere C is a constant depending only on A and a.Proof. ... deningfn(t) = ka bk CkA Bkj(t t0)j M Z tt0 fn1(s)ds: (2.6).

8 Oct 2021: kA| ik  M k| ik for some fixed M > 0.