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file:///C:/Users/removevirus/Desktop/misc/Streaming/Haldane,%20
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/Haldane.pdf13 Oct 2013: This paper was originally grabbed from the reading list of a course Prof. Kurose taught at UMass. Note: This essay was originally published in 1928 (long before computer networks were invented :-) ) and discussed size in the natural (biological) -
Home Page of Prof. A.S. FOKAS
www.damtp.cam.ac.uk/user/tf227/18 Jan 2013: ii) MEG and EEG. A.S. Fokas, Y. Kurylev and V. Marinakis, The Unique Determination of the Neuronal Current in the Brain via Magnetoencephalography, Inverse Problems 20, 1067-1082 (2004). ... Rev. Lett. 96, 190201 (2006). A.S. Fokas, Nonlinear Fourier -
www.damtp.cam.ac.uk/user/mem/oldftp/AIX/aixf.log
www.damtp.cam.ac.uk/user/mem/oldftp/AIX/aixf.log5 Jun 2013: 15] [16] [17] File: PV_phillips_2.eps Graphic file (type eps) PV_phillips_2.eps [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] File: staircase-jets.eps -
www.damtp.cam.ac.uk/user/mem/papers/LHCE/dilnot-pat-analysis.txt
www.damtp.cam.ac.uk/user/mem/papers/LHCE/dilnot-pat-analysis.txt19 Oct 2013: I don't think it needs to be 20 years and it doesn't need to be 20 years for every country on this planet. -
Averaged Lagrangian
www.damtp.cam.ac.uk/user/hinch/teaching/avlagrnhandout.pdf20 Feb 2013: Averaged Lagrangian. John Hinch. February 20, 2013. Lagrangian formulation. Field equation, e.g. -
Chapter 10 – Strong flows ◮ Birefreingent strand – ...
www.damtp.cam.ac.uk/user/hinch/teaching/nnfm/part10handout.pdf19 Aug 2013: a. 1e-05. 0.0001. 0.001. 0.01. 0 5 10 15 20. t. ... FENE capillary squeezing. Filament breaks in with FENE L = 20. -
Hydrodynamic Attraction of Swimming Microorganisms by Surfaces…
www.damtp.cam.ac.uk/user/lauga/papers/20.pdf26 Jul 2013: We capture 2-second movies at 20 framesper second and measure the number of swimming cells bycounting cells swimming at speed faster than 1 body lengthper second. ... Fitting the measurements to our modelleads to L? 20–76 m. Since the cells swim -
Layout 1
www.damtp.cam.ac.uk/user/tong/talks/diary.pdf17 Nov 2013: On a good day, I could probably get through about 20% of them. -
NL87_authors_proofs
www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_02.pdf14 Mar 2013: 20 EMS Newsletter March 2013. Feature. Feature. EMS Newsletter March 2013 21. -
Mathematical Tripos Part II E.J. Hinch WAVES Lent 2013 ...
www.damtp.cam.ac.uk/user/hinch/teaching/D24a.pdf19 Jan 2013: Mathematical Tripos Part II E.J. Hinch. WAVES Lent 2013. Example Sheet 1: Sound Waves. 1. Plane waves and radiation. A thin piston executes very small oscillations about x = 0 in a. long straight fluid-filled tube with cross-sectional area A and -
PHYSICS OF FLUIDS 18, 091701 �2006� Experimental investigations of ...
www.damtp.cam.ac.uk/user/lauga/papers/14.pdf26 Jul 2013: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11. ... Two datasets are shown: 1 L = 20 cm, D = 0.5 mm, and a0 = 0.435 rad; 2L = 18 cm, D = 0.61 mm, and a0 = 0.814 rad. -
No Job Name
www.damtp.cam.ac.uk/user/lauga/papers/13.pdf26 Jul 2013: factors of 10, untilround off error sets in.) We have tested this algorithm up toN) 20 on the problem of packing circles on free spheres and havefound all of the known ... nondensest jammed packings were found belowN ) 10. ForN below 20, evenwhen -
1B Methods 27 . 1B METHODS LECTURE NOTES Richard ...
www.damtp.cam.ac.uk/user/examples/B8Lb.pdf4 Oct 2013: 2P. x2. The assumed behaviour of the variance eq. (20) occurs commonly in actual physicalprocesses. ... λ)(6 λ)x4. 4! (λ)(6 λ)(20 λ)x6. 6! ],. Θ1 = a1. -
Ultimate Regime of High Rayleigh Number Convection in a ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Hewitt-2012.pdf4 Nov 2013: The measurements of k can be fitted by an ap-proximate scaling k Ra0:4, though the data also hint at apossible decrease in the exponent for Ra > 20 000 ... 20] Counts from a plume-tracking algorithm suggest a scalingexponent of 0:96 0:05 for the rib -
doi:
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Huppert-2013.pdf4 Nov 2013: 20. 40. 60. 80. 100. 120. 1 2 3 4 5 6 7. ... E. Huppert, J. A. Neufeld and C. Strandkvist. 0 20 40 60 80 100. -
Breaking the coherence barrier: asymptoticincoherence and asymptotic…
www.damtp.cam.ac.uk/research/afha/bogdan/AHPRSampta13.pdf5 Oct 2013: On the. 128 256 512 1024 2048 40960. 10. 20. 30. -
pnas201302736 14132..14137
www.damtp.cam.ac.uk/user/gold/pdfs/streaming_selforganization.pdf27 Aug 2013: The parameter space was divided upinto a 20 20 grid, and the full set of parameters was simulatedfor each of 50 different instances of random initial conditions.Combined with a linear ... The entire setof 20 20 parameters was simulated for 50 different -
Convergence theory for spectral deferred correction Anders C. Hansen, …
www.damtp.cam.ac.uk/research/afha/people/anders/Spectral.pdf5 Oct 2013: 10. [6] R. Frank and C. Ueberhuber, Iterated Deferred Correction for Differential Equations,part 1, Computing, 20 (1978), 207-228. ... Comput. Phys., 189, 351–376, 2003. [15] B. Lindberg, Error Estimation and Iterative Improvement for Discretization -
Inevitability of a magnetic �eld in the Sun'sradiative interiorD. …
www.damtp.cam.ac.uk/user/mem/oldftp/solar-nature.pdf19 Oct 2013: The boundary-layerequation then reduces to @6 T@r6 6 T 0 ; (5)in which the boundary-layer thickness is given by = 20 2iB20r2cN2L4! ... Astrophys. J.,(submitted)20. Dziembowski, W. A. & Goode, P. R. The toroidal magnetic eld inside the sun.Astrophys. -
PHYSICS OF FLUIDS 24, 072102 (2012) Buckling instability of ...
www.damtp.cam.ac.uk/user/lauga/papers/67.pdf26 Jul 2013: r1. θ = πθ = 3π/4θ = π/2θ = π/4. 0 20 40 60 80 1000. ... Sci. Eng. 3, 16–21 (2001).20 S. Bohn, “Bubbles under stress,” Eur. -
A stability barrier for reconstructions from Fourier samples Ben ...
www.damtp.cam.ac.uk/research/afha/anders/AdcockHansenShadrin.pdf5 Oct 2013: See [12, 20]. In a similar spirit, Driscoll & Fornberg introduced Padé-based method in[25]. ... 105. 20 40 60 80 100. 0.1. 0.2. 0.3. 20 40 60 80 100. -
PHYSICS OF FLUIDS 24, 103102 (2012) Micropropulsion and microrheology …
www.damtp.cam.ac.uk/user/lauga/papers/72.pdf26 Jul 2013: σ 1 = 0, (20). u1 = 0, (21)where. σ 1 = p1I γ̇ 1! ... 2.5. 3. 3.5. 4. 20. 40. 60. 80. 100. 120. hRU. -
Proc. July 2007 Conf. onUnsolved Problems in Stellar Physics, ...
www.damtp.cam.ac.uk/user/mem/papers/SQBO/woodmcintyre-preprint.pdf19 Oct 2013: 0. 2. 4. (a). 2 0 20. 0.5. 1. 1.5. 2. ... 2.5. 3. 3.5. 4. z. 0.2 0 0.20. 0.5. 1. 1.5. -
Springer Handbook of Experimental Fluid Mechanics: Chapter 19
www.damtp.cam.ac.uk/user/lauga/papers/19.pdf26 Jul 2013: Tetradecane 2138 3.5 nm (rms) 0 – 5 nm NLMica+.2 PPO Water 90110 2 nm (rms) 0 – 20 nm NL. ... Tetradecane – 2 nm (rms) 0 – 20 nm NLMicaOTE Water 110 0.2 nm (rms) 0 – 40 nm NL. -
flm469.dvi
www.damtp.cam.ac.uk/user/lauga/papers/4.pdf26 Jul 2013: Slip length λeff 2–8 µm 20–90 nm 200–450 µm 1 µm 10–30 nm. ... Effective slip in pressure-driven Stokes flow 67. 010–20. 1. 2. 3. -
pv-score-japan12-1.dvi
www.damtp.cam.ac.uk/user/mem/oldftp/pv-score-japan12-1.pdf19 Oct 2013: . 20. Snare drum. CHOIR. Piano. . . . pp. -
Optimal feeding is optimal swimming for all Péclet numbers ...
www.damtp.cam.ac.uk/user/lauga/papers/59.pdf26 Jul 2013: eled individually using slender body theory1,20 or singularity. methods.21 The second approach, to which this work. ... field (up to /(nmax)18–20 for thehighest values of Pe considered) and increase its resolution. -
Swimming in Circles: Motion of Bacteria near Solid Boundaries ...
www.damtp.cam.ac.uk/user/lauga/papers/12.pdf26 Jul 2013: Also, we observe that. aVxUy. aVLUxyMLVxx. aLk. 3 1; (20). so the timescale for reorientation of the bacteria perpendic-. ... 1=2 20 to 25mm/s; both set of values compare also favorably with pastexperimental results as described in the Introduction. -
gl044728 1..5
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Neufeld-2010-2.pdf4 Nov 2013: H 20 m,motivated by the Sleipner site in the North sea [Bickle et al.,2007]. ... FCO2 DDCO2. HSh DCO2. kgD. 4=5 DH. 1=5. ’ 20 kg m2 yr1. -
PHYSICAL REVIEW E 84, 061905 (2011) Energetics of synchronized ...
www.damtp.cam.ac.uk/user/lauga/papers/62.pdf26 Jul 2013: 2un2 = EnKn1(r) FnKn1(r) BnrKn(r), (20)2vn1 = FnKn1(r) EnKn1(r). (21). The w component can be computed from u and v using thecontinuity equation, Eq. ... 15. 20. 0 0.5 189.5. 90. 90.5. 91. 100 101 102 103100. -
b924548k 1737..1747
www.damtp.cam.ac.uk/user/lauga/papers/40.pdf26 Jul 2013: also well known that many biological cells actively modify or. maintain the shapes of their membranes,20,21 either for develop-. ... double-layer integral,. u(x) ð. S(t)q(y)$T(x,y)$n̂(y) dSy (20). where q(x) is an unknown density of the singular -
J. Fluid Mech. (2012), vol. 705, pp. 120–133. c� ...
www.damtp.cam.ac.uk/user/lauga/papers/69.pdf26 Jul 2013: 1rn1. r(rn1Sn) rn1. r. Qn. rn1. 2 Wn. z= 0 (n 1), (3.20). -
flm1000491a
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Vella-2011.pdf4 Nov 2013: φ+. x. x=0. φx. x=0. 4. 1 y2=. (23π. )1/2λ̄φ. 1/20. ... 3.20). Substituting the similarity solution for h from (3.16) and (3.15), we find that. -
REDUCED CONSISTENCY SAMPLING IN HILBERT SPACES Ben Adcock1, Anders ...
www.damtp.cam.ac.uk/research/afha/anders/AdcockHansenSampTA.pdf5 Oct 2013: 20 40 60 80 100 120 140. - 10. - 5. -
pnasSI201302736 1..6
www.damtp.cam.ac.uk/user/gold/pdfs/streaming_selforganization_SI.pdf27 Aug 2013: Phys Fluids 20(12):123304. 2. Woodhouse FG, Goldstein RE (2012) Spontaneous circulation of confined activesuspensions. ... 1. 2. 3. 4. 5. p. c. 1.000.20. 0.15. 0.10. 0.05. -
C2SM27089G 1711..1720
www.damtp.cam.ac.uk/user/lauga/papers/74.pdf26 Jul 2013: g(k) 2[1 cos(k) g log(k) kSi(k) Ci(k)], (20). and with the sine and cosine integrals dened by. ... Roman and J. Bico, J. Phys.: Condens. Matter, 2010, 22,493101. 20 S. -
flm1100223a
www.damtp.cam.ac.uk/user/lauga/papers/54.pdf26 Jul 2013: F (ζ ) f (z(ζ )), G(ζ ) g(z(ζ )), (5.20). ... 0.20. 0.25. 0.30. 0.35. Ca. c. c = 8 Ca. Figure 6. -
flm1000488a
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Neufeld-2011.pdf4 Nov 2013: R. Lister. –40 –20 0 20 40. x. 0. 0.2. 0.4. ... Thesink is resolved by a 20 cell pattern arranged to roughly approximate a cylindrical fissurein the cap rock. -
A stability barrier for reconstructions from Fourier samples Ben ...
www.damtp.cam.ac.uk/research/afha/people/anders/AdcockHansenShadrin.pdf5 Oct 2013: See [12, 20]. In a similar spirit, Driscoll & Fornberg introduced Padé-based method in[25]. ... 105. 20 40 60 80 100. 0.1. 0.2. 0.3. 20 40 60 80 100. -
Document 1
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Daniels-2012.pdf4 Nov 2013: to store the energy sector’s emssions at current levels for the next 100 years [19, 20]. ... In this regeneration stage,between 13 and 20% of the power output of the plant can be lost. -
Mathematics of Information Arieh Iserles, and Carola-Bibiane…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_05.pdf2 Oct 2013: SIAM J. Sc. Comp., 20(1):33–61, 1998. 12. [9] I. Daubechies. Ten Lectures on Wavelets, volume 61. -
flm1100072a
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Zimoch-2011-1.pdf4 Nov 2013: 0.5, 2, 5, 20.5 and 52. ... t. 1.0. 0.8. 0.6. 0.4. 0.2. 0 10 20 30 40. -
Modelling carbon dioxide sequestration in layered strata
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Neufeld-2009-1.pdf4 Nov 2013: Equation (2.15) is subject to the non-dimensional boundary conditions[HH. X. ]. 0. = αT α1, (2.19). [HH. X. ]. XN. = 0, (2.20). ... short-dashed line), 20(dash–dotted line), 25 (long-dashed line) and 30 (dashed–dotted–dotted line). -
Shear-enhanced convection in a mushy layer
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Neufeld-2008-2.pdf4 Nov 2013: w1. = k2RmΠ1(φ)θ1. (4.20). The boundary conditions can be similarly transformed. ... 348 J. A. Neufeld and J. S. Wettlaufer. 0 5 10 15 20 25 30. -
The optimal elastic flagellumSaverio E. Spagnoliea� and Eric Laugab�…
www.damtp.cam.ac.uk/user/lauga/papers/36.pdf26 Jul 2013: ESliding t =G. 2. 0. L. 2ds. 20. As with the bending Eq. ... Even though the hydrodynamic efficiencyonly decays 13% from the optimal sawtoothed solution, theswimming speed decreases by approximately 20%. -
Floppy swimming: Viscous locomotion of actuated elastica Eric…
www.damtp.cam.ac.uk/user/lauga/papers/16.pdf26 Jul 2013: The main features of this problem have been successfullyexploited experimentally to measure the bending modulus ofbiopolymers actin filaments and microtubules, either usingthermal fluctuations 20 or using an active actuation ... Optimal III 0.24 3.34 -
Digital Object Identifier (DOI) 10.1007/s00220-013-1729-7Commun.…
www.damtp.cam.ac.uk/user/md327/CDT13_file.pdf14 Aug 2013: Received: 24 April 2012 / Accepted: 20 November 2012Published online: 21 May 2013 – Springer-Verlag Berlin Heidelberg 2013. ... The existence of the Lax pair for an arbitrary conformal structurewith vanishing self-dual Weyl curvature has the following -
§4 FLOWS WITH A FREE SURFACE Such flows are ...
www.damtp.cam.ac.uk/user/mem/FLUIDS-IB/waves.pdf19 Oct 2013: 20. Eliminate U2:. 12g(h21 h. 22) = h2. V (h2 h1). -
May 31, 2010 Lecture Note Series, IMS, NUS — ...
www.damtp.cam.ac.uk/user/phh/papers/singapore2011.pdf19 Oct 2013: perhaps 20 days or more) ozone concentrations in Europe, for example, are. ... 9in x 6in lecturenotes˙190410. 20 P. H. Haynes. Fig. 3. Reproduced from [13]. -
REDUCED CONSISTENCY SAMPLING IN HILBERT SPACES Ben Adcock1, Anders ...
www.damtp.cam.ac.uk/research/afha/people/anders/AdcockHansenSampTA.pdf5 Oct 2013: 20 40 60 80 100 120 140. - 10. - 5.
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