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23 24 25 26 270 0.5 1 1.5 cross-sectional ...
www.damtp.cam.ac.uk/research/fluidshr/files/pictures/baffle.pdf19 Mar 2020: 23 24 25 26 270. 0.5. 1. 1.5. cross-sectional view side-view. -
Berry Groisman - Teaching
www.damtp.cam.ac.uk/user/bg268/11 Mar 2020: Berry Groisman. Further Complex Methods - Lent 2020. (Please, keep checking this page as it will be updated throughout the course. Material is examinable unless explicitly stated otherwise.). E-1: Analytic Continuation by Taylor series: Natural -
Dr Matthew Wingate - Lecture notes
www.damtp.cam.ac.uk/user/wingate/Notes/2 Jun 2020: 14. Interacting model - distributed 12 Nov 2008, corrections 24 Nov 2008. ... 17. Lower critical dimension - distributed 24 Nov 2008. -
Course: Numerical Analysis - Applied Functional and Harmonic Analysis
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/23 Nov 2020: Time, location: Online. This is a Part II course in numerical analysis given in Michaelmas term 2020 that contains 24 lectures. ... Lecture 16:Lecture 17:Lecture 18:Week 7:. Lecture 19:Lecture 20:Lecture 21:Week 8:. Lecture 22:Lecture 23:Lecture -
IB lecture notes on fluid dynamics (second year at Cambridge)
www.damtp.cam.ac.uk/user/mem/FLUIDS-IB/24 Jul 2020: Michael McIntyre (mem at damtp.cam.ac.uk),Silver Street, Cambridge CB3 9EW. Last updated 24 July 2020. -
Professor Nigel Weiss FRS (1936-2020)
www.damtp.cam.ac.uk/user/gio10/now.html22 Jul 2020: Professor Nigel Weiss FRS (1936-2020). Nigel Weiss, who died on 24 June 2020 after a fall at his home, was born on 16 December 1936, in South Africa. -
Dr A. Hansen Mathematical Tripos Part II: Michaelmas Term ...
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/b15.pdf29 Oct 2020: 19 on the Example Sheets). Method 3.24 (The spectral method for evolutionary PDEs) We consider the problemu(x,t). ... û′n(t) = π2n2ûn(t). n ΓN (3.24). Its exact solution is ûn(t) = eπ2n2t ĝn for n 6= 0 and we set û0(t) = 0 due to -
LUCIDITY PRINCIPLES supplement (index)
www.damtp.cam.ac.uk/user/mem/papers/LHCE/lucidity-supplem-index.html8 Jan 2020: McIntyre 1999. Last updated 24 Oct 2016. -
Mathematical Tripos Part II: Michaelmas Term 2020 Numerical…
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/b00.pdf6 Oct 2020: 24. The QR algorithm. Convergence of the first column and the bottom row. -
DYNAMICS SIGNIFICANT FOR CHEMISTRY
www.damtp.cam.ac.uk/user/mem/papers/ECMWF/ecmwf05.html9 Jan 2020: page 24 of the abovementioned Appendix III of the supplementary material for the Summer School), and in this paper with Tim Palmer written at a time when the idea was controversial. -
Stress-Induced Dinoflagellate Bioluminescence at the Single Cell Level
www.damtp.cam.ac.uk/user/gold/pdfs/lunula.pdf6 Jul 2020: action potential—which arises from nonlinear, excitabledynamics—analysis of the flashes [24] indicates a timecourse much like that of two coupled capacitors chargingand discharging on different timescales. ... exactly [24], thus enabling a global fit -
The much-neglected Second Normal Stress Difference
www.damtp.cam.ac.uk/user/hinch/talks/SecondNSDb.pdf24 Sep 2020: September 24, 2020. 1. What are normal stresses? In simple shear u = (γy, 0, 0), the stress tensor is. -
Dr A. Hansen Mathematical Tripos Part II: Michaelmas Term ...
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/sh03.pdf9 Nov 2020: criterion. So, you need also to prove that ρ(D1(AD)) > 1.]. 24. ... Further, show that if one Jacobi iteration isperformed, then u3,3 = 23/24 occurs, which is the estimate of u(1/2,1/2) = 9/8. -
Active rotational dynamics of a self-diffusiophoretic colloidal motor
www.damtp.cam.ac.uk/user/lauga/papers/172.pdf5 Feb 2020: motor surface.22 Active rotational motion hasalso been studied for Janus motors with a coupling of electro-chemical forces to fluid flow23 or under an external field such asgravity,24 nonspherical ... dy:. (24). The integral in eqn (24) may be evaluated -
Hydrodynamic model for Spiroplasma motility
www.damtp.cam.ac.uk/user/lauga/papers/181.pdf8 Sep 2020: 24) and βh = 1/2, and furthersubstituting into Eq. (50) gives access to the asymptotic solution for the swimming speed as(. ... 24]. When viewed as a run-reverse motionwith rotational diffusion, a change in the reversal rate modifies the mean path length -
solidstate
www.damtp.cam.ac.uk/user/tong/aqm/solid1.pdf11 Nov 2020: 1.5 Spin in a Magnetic Field 22. 1.5.1 Spin Precession 24. ... qg = 2n with n 2 Z (1.24). This is the famous Dirac quantisation condition. -
Selectively controlled magnetic microrobots withopposing helices
www.damtp.cam.ac.uk/user/lauga/papers/176.pdf6 Jul 2020: In a given frequency range, this motionleads to a stable forward propulsive force.24,25 An example response,called the step-out profile, is illustrated in Fig. ... Mater. 24, 811–816 (2012). 7H. Ceylan et al., “Mobile microrobots for bioengineering -
Numerical Analysis - Part II
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/Lect_8_slides.pdf15 Oct 2020: This, however,does not mean that its numerical modelling is easy. 13 / 24. ... 23 / 24. Stability using Fourier analysis. The Fourier analysis (for Cauchy problem) provides. -
DOI 10.1140/epje/i2019-11854-3 Regular Article Eur. Phys. J. E (2019) …
www.damtp.cam.ac.uk/user/lauga/papers/163.pdf6 Jul 2020: 24). For many ions in water atroom temperature, the diffusivity is approximately Ds 109 m2 /s [33]. ... 24), we can integrate eq. (59) directly to obtainthe following result for the non-reacting model:. -
Part III Applications of Differential Geometry to Physics, Sheet ...
www.damtp.cam.ac.uk/user/md327/PartIII_geom_2.pdf20 Jan 2020: 24 = 1 and find its. degree. By calculating Tr((dg g1)3) at the point on S3 where x4 = 1,or otherwise deduce that the formula. -
Irreversible hydrodynamic trapping by surface rollers
www.damtp.cam.ac.uk/user/lauga/papers/174.pdf6 Jul 2020: magnetic,5 electrostatic,18 or hydrodynamic forces.24 In recentyears, synthetic swimmers actuated by external fields, chemicalfuels or bacteria have been attracting attention and been employedsuccessfully for the transport of cargo ... 23 See ESI†.24 A. -
2. The Integer Quantum Hall E↵ect In this section ...
www.damtp.cam.ac.uk/user/tong/qhe/two.pdf5 Oct 2020: by (1.24). With the Landau levels filled, the current in the x-direction is. ... But we know from (1.20) and (1.24) that these harmonic oscillator states are. -
PII: 0377-0427(89)90022-8
www.damtp.cam.ac.uk/user/ms100/PAPERS/JCAM89.pdf2 Feb 2020: Since. and. ux= [ rx i&r] exp(W,. 24 xx = [ 2irx+, rxx i+,,r - (x)2r] exdih. ... U, = 24, e,_, Sl_le,_2. S,‘e,. Now, for kc n define r&= (AZ)-2e,, and #k= ,S$#Q_, and put 4, = (AZ)-2e,_,. -
On the existence of stable and accurate neural networks ...
www.damtp.cam.ac.uk/user/mjc249/pdfs/NN_colbrook10.pdf17 Nov 2020: rL, (24). which is the same estimate as the one dimensional case for boundedd. ... The network weights are providedby the authors of [57] and had been trained on de-identified brainimages from the MGH–USC HCP dataset [24] where the image. -
statphys
www.damtp.cam.ac.uk/user/tong/statphys/five.pdf17 Feb 2020: 5.24). The row of the matrix is specified by the value of si = 1 and the column by si1 = 1. ... siand product over lattice sites. Qiin (5.23) simply tell us. to multiply the matrices defined in (5.24) and the partition function becomes. -
Light-switchable propulsion of active particles with reversible…
www.damtp.cam.ac.uk/user/lauga/papers/175.pdf6 Jul 2020: ARTICLE. Light-switchable propulsion of active particles withreversible interactionsHanumantha Rao Vutukuri 1, Maciej Lisicki 2, Eric Lauga 3 & Jan Vermant 1. Active systems such as microorganisms and self-propelled particles show a plethora of. -
PII: 0022-460X(86)90195-1
www.damtp.cam.ac.uk/user/ms100/PAPERS/JSV86.pdf2 Feb 2020: u,(O) = u(O) = v,(O) = v2(0) = 0. (24). What follows is concerned, not with the general fourth moment at zr but rather with quantities involving intensities at two points -
Hypergeometric function - series representation Claim: F (a, b; ...
www.damtp.cam.ac.uk/user/bg268/Hypergeometric%20function%20as%20a%20series.pdf11 Mar 2020: Hypergeometric function - series representation. Claim:. F (a, b; c; z) =n=0. (a)n(b)n(c)n. zn. n!,. where (x)n = x(x 1).(x n 1), (x)0=1, is the Pochhammer symbol. The series is convergent in |z| < 1. The RSP at z = 1 prohibits the series -
3. The Fractional Quantum Hall E↵ect We’ve come to ...
www.damtp.cam.ac.uk/user/tong/qhe/three.pdf5 Oct 2020: i=1. |i|2 (3.24). The corrected plasma partition function is then. Z Yd2zi e. ... precisely by the partition function with energy (3.24) and hence has no dependence. -
Rough surface reconstruction from phaseless single frequency data at…
www.damtp.cam.ac.uk/user/ms100/PAPERS/main-phaseless-IOP.pdf2 Feb 2020: 2n. ) γ. (24). 9. Provided the data is sufficiently well-resolved, we can use the assumption of continuity to resolveany phase ambiguities arising from this expression. ... 24] Michele D’Urso, Kamal Belkebir, Lorenzo Crocco, Tommaso Isernia, and -
3 Supersymmetric Quantum Mechanics We now turn to consider ...
www.damtp.cam.ac.uk/user/dbs26/SUSY/chap3.pdf30 Jan 2020: η̄k1|eτ H(ˆ̄ψ,ψ̂)|ηk〉 = eτ H(η̄k,ηk) 〈η̄k1|ηk〉 = eτ H(η̄k1,ηk) eη̄k1ηk. (3.24). -
Université Paris-Saclay Mathématiques : Mise à niveau I333a Notes ...
www.damtp.cam.ac.uk/user/tc683/Cours_I333a_2020-21.pdf13 Oct 2020: Par exemple :. 2. 1 12 31 1. = 2 24 62 2. ... 24. Chapitre 3. Diagonalisation. 3.1 Bases et changements de base. Dans cette section, nous rappelons de manière très (trop? ) -
Numerical Analysis - Part II
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/Lect_24_slides.pdf23 Nov 2020: Numerical Analysis - Part II. Anders C. Hansen. Lecture 24. 1 / 25. ... 24 / 25. Single shifts. A good approximation sk = (Ak )nn to the eigenvalue λs generateseven better approximation of sk1 = (Ak1)nn to λs , andconvergence is accelerating at a -
Wave Scattering in a Rough Elastic Layer Adjoining a Fluid Half-space
www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA95elastic.pdf4 Feb 2020: 24). Expanding the se•nd exponential on the right, we finally obtain. -
This article appeared in a journal published by Elsevier. ...
www.damtp.cam.ac.uk/user/ms100/PAPERS/Karunarathna_et_al_2009.pdf4 Feb 2020: Article history:. Received 4 June 2009. Received in revised form. 24 August 2009. ... 8.0. 10.0. 12.0. 14.0. 16.0. 18.0. 20.0. 22.0. 24.0. 26.0. 28.0. -
PUBLICATIONS : NICHOLAS STEPHEN MANTON Research Papers 1. The ...
www.damtp.cam.ac.uk/user/nsm10/Publications.pdf17 Jul 2020: 24. Classical and Quantum Dynamics of BPS Monopoles (with G.W. Gibbons), NuclearPhysics B274 (1986) 183-224. ... 3. LMS Annual General Meeting 19/11/04, London Mathematical Society Newsletter 333(2005) 23-24. -
Fluid Dynamics II (D) John Hinch Draft 1, September ...
www.damtp.cam.ac.uk/user/hinch/teaching/FluidsIInotes.pdf18 Sep 2020: 24. The solution is. u = 12µ. dp. dx(h2 y2). The volume flux (per unit length in z-direction) is. -
Black Holes
www.damtp.cam.ac.uk/user/hsr1000/black_holes_lectures_2020.pdf3 Mar 2020: m0 <. 16. 243πρ0(1.24). Part 3 Black Holes March 3, 2020 9 H.S. ... Dividing (2.24) by (dv/dλ)2 gives. 2 drdv 2M. r 1 2 dr. -
HYSICALEVIEWETTERS PRL American Physical Society 28 JUNE 2019 Volume…
www.damtp.cam.ac.uk/user/mjc249/pdfs/mjc_PhysRevLett.122.250201.pdf19 May 2020: current interest in the spectral properties of systems withcomplicated spectra. The study of aperiodic systems, suchas quasicrystals [18,19], often leads to complicated, evenfractal-like spectra [20–24], which can make ... 24, 81 (2011).[14] M. Marletta -
4.6 Monodromy: the reason for the logarithmic term in ...
www.damtp.cam.ac.uk/user/bg268/Monodromy%20-%20need%20in%20log%20term.pdf11 Mar 2020: 4.6 Monodromy: the reason for the logarithmic term in the solution. Recall that forw′′ p(z)w′ q(z)w = 0, (1). in the vicinity of a RSP at z = 0 (WLOG - other points obtained by translation),there exist two linearly independent solutions of (1), -
J. Fluid Mech. (2020), vol. 903, A11. © The ...
www.damtp.cam.ac.uk/user/gold/pdfs/stability_of_dancing_volvox.pdf22 Sep 2020: t = 18 s t = 21 s t = 24 s t = 27 s t = 30 s t = 33 s. -
Gauge/Gravity Duality Mathematical Tripos, Part IIIAron C. Wall…
www.damtp.cam.ac.uk/user/aw846/AdSCFT/GGexamples_1.pdf1 May 2020: 23). ds2 = dT 2 cos(T)2[dr2 sinh(r)2d2D2. ]; (24). 5. ... Note that (24) looks like a recollapsing FLRW cosmology with k = 1 (negativecurvature), but the apparent ‘Big Bang’ and ‘Big Crunch’ singularities areactually just coordinate artifacts. -
Dr A. Hansen Mathematical Tripos Part II: Michaelmas Term ...
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/b12.pdf26 Oct 2020: 24. the even and odd portions of y, respectively. Note that y(E),y(O) Πm. -
Stokes flow due to point torques and sources in a spherical geometry
www.damtp.cam.ac.uk/user/lauga/papers/179.pdf8 Sep 2020: f (ξ ) = R3δ(ξ R1 ), (24)and so the flow is simply given by. ... 24] using a solution obtained with the use of flow potentialsand sphere theorems. -
Traveling waves are hydrodynamically optimal for long-wavelength…
www.damtp.cam.ac.uk/user/lauga/papers/182.pdf14 Dec 2020: Fluid Mech. 24, 313 (1992).[17] J. S. Guasto, R. Rusconi, and R. ... Fluid Mech. 762,. (2015). 123101-9. ERIC LAUGA. [24] T. D. Montenegro-Johnson and E. -
Collective stiffening of soft hair assemblies
www.damtp.cam.ac.uk/user/lauga/papers/178.pdf6 Jul 2020: For apoint force located at a distance h above the flat bottom sur-face, and assuming no-slip boundary conditions, the flow canbe obtained using the hydrodynamic image method ... Like us, they interpreted theirresults using the models of Refs. [24,25]. -
Numerical Analysis - Part II
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/Lect_7_slides.pdf15 Oct 2020: 24 / 26. Stability: Backward Euler and the diffusion equation. 2) For the backward Euler method. -
SIAM J. SCI. COMPUT. c© 2019 Society for Industrial ...
www.damtp.cam.ac.uk/user/mjc249/pdfs/hybrid_spec_mjc.pdf16 Jul 2020: Second, it has led to novel analyticalformulations of a variety of important physical problems from water waves [1, 23, 8,46, 61, 24] to three-dimensional layer scattering [3]. ... 10-6. 10-4. 10-2. 4 6 8 10 12 14 16 18 20 22 24 2610-15. -
4. Non-Abelian Quantum Hall States The vast majority of ...
www.damtp.cam.ac.uk/user/tong/qhe/four.pdf5 Oct 2020: 12, 34) (13, 24) = (z1 z2)21423. Then, using the definition of the Pfaan (4.3), we have. ... Pf(13),(24)(z) = A(13, 24). z1 z2(13, 24). z3 z4. = A(12, 34) (z1 z2)21423. -
Dr A. Hansen Mathematical Tripos Part II: Michaelmas Term ...
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/b19.pdf16 Nov 2020: This gives expression for αk in (4.7). 37. Method 4.24 (The steepest descent method) This method takes d(k) =F1(x(k)) = b Ax(k)for every k, the
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