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Microbial mutualism at a distance: The role of geometry in diffusive…
www.damtp.cam.ac.uk/user/gold/pdfs/mutualism.pdf27 Feb 2018: PHYSICAL REVIEW E 97, 022411 (2018). Microbial mutualism at a distance: The role of geometry in diffusive exchanges. François J. Peaudecerf,1, Freddy Bunbury,2 Vaibhav Bhardwaj,2 Martin A. Bees,3 Alison G. Smith,2. Raymond E. Goldstein,1,† and -
ELIFE06088 1..31
www.damtp.cam.ac.uk/user/gold/pdfs/Drosophila_axis.pdf23 Sep 2015: along the anterior (kA = 1000 μm, hA0 = 0:8) and strongly along the posterior-lateral cortex (kP = 150 μm, hP0 = 0, see ‘Materials and methods’ MT nucleation. ... the inset of panel C (yellow circles). In all panels, parameter values for anterior -
Publications | Cantab Capital Institute for the Mathematics of…
www.damtp.cam.ac.uk/research/ccimi/publications?page=184 Jul 2024: KA Bacik, S Lovett, C-CP Caulfield, NM Vriend. – Physical review letters. -
Publications | Astrophysics
www.damtp.cam.ac.uk/research/astro/publications?page=494 Jul 2024: MC Chidichimo, G Del Zanna, HE Mason, NR Badnell, JA Tully, KA Berrington. – -
solidstate
www.damtp.cam.ac.uk/user/tong/aqm/solid3.pdf7 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! = -
Numerical studies of the influence of the dynamic contact ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_21_072102.pdf28 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. -
15632687789062 1..20
www.damtp.cam.ac.uk/user/gold/pdfs/universal_swimming.pdf16 Jul 2019: eLife 7:e40018. DOI: https://doi.org/10.7554/eLife.40018,PMID: 30033910. Guasto JS, Johnson KA, Gollub JP. ... 2009. The Chlamydomonas Sourcebook. 2nd edition. London: Academic Press.Hinchliff CE, Smith SA, Allman JF, Burleigh JG, Chaudhary R, Coghill LM, -
, 20120576, published 2 January 2013469 2013 Proc. R. ...
www.damtp.cam.ac.uk/user/md327/skyrmion_proc.pdf14 Aug 2013: Let K = Ka/xa, a = 0,. , 3 be a vector field generating a one-parameter group oftransformations of M with orbits Γ. -
201019079 10940..10945
www.damtp.cam.ac.uk/user/gold/pdfs/noise.pdf6 Jul 2011: 38. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions. -
statphys
www.damtp.cam.ac.uk/user/tong/statphys/three.pdf31 Dec 2018: and, for small ka, the sin function is approximately linear. This means that we get. -
Publications | Theoretical High Energy Particle Physics Group
www.damtp.cam.ac.uk/research/hep/publications?from=damtp&gsearch=MacFarlane%27&page=1264 Jul 2024: KA James, PV Landshoff. – Physics Letters B. (1990). 251,. 167. -
Fluid flows created by swimming bacteria driveself-organization in…
www.damtp.cam.ac.uk/user/gold/pdfs/swimmers_flows.pdf14 Jul 2014: flow field around swimming microorganisms. Phys Rev Lett 105(16):168101.23. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganisms. -
§4 FLOWS WITH A FREE SURFACE Such flows are ...
www.damtp.cam.ac.uk/user/mem/FLUIDS-IB/waves.pdf19 Oct 2013: iσζ̂ kA sinh kh = 0. and from the second (pressure) (). gζ̂ iσA cosh kh = 0. Regarding these as a system of two linear algebraic equations for the two unknown constants ζ̂ -
IOP PUBLISHING CLASSICAL AND QUANTUM GRAVITY Class. Quantum Grav. ...
www.damtp.cam.ac.uk/user/md327/dunajski_hartnol.pdf17 Apr 2007: It therefore followsfrom (22) that Xa, Xa, Ya Y a are gradients and that Ka = Ya Y a is a Killing vector. -
��������� ��� ����������������������� �����…
www.damtp.cam.ac.uk/user/mem/oldftp/airsea-negvisc.pdf19 Oct 2013: J<6{4)01# "9#mI =9? : : "9#r=:; DJzG=x? 0- I?6,z#1 Kj BKj'Kä :6#(8º Jz0 G= 8G? ... 6'? ] BKj0G=>=# Kj Km'Kä :#I =º? :;81#G5#6: º#=>c0- "GG "(8º J= G= 0G=º# Km Kj'EKà :#c X8Ñ? -
��������� � ���� ������ ����� ����������������� �! "��#$�…
www.damtp.cam.ac.uk/user/ngb23/publications/potential7.pdf1 Feb 2008: Aé13<K3è-1 ->EN31ZEF>"3517ð"65:C3EF<@>kA<@ê|:CEF>. S 0 ù ûèé-;Vü35è1zî@1VDN<ì4EN3õþ<Cç3è1î"<@6317òEG;><@3K35è19;éê -
��������� ��� � �� � ����������������������������� !������ "���…
www.damtp.cam.ac.uk/user/rrk26/Papers/PDK09.pdf12 Aug 2016: G?Gh3j|kA:?lH7aPG IP q 2! 6! > ,I, G G)?%c e %3:S&&$J0 )' ,-/./0 %3$H&( )4 5/./0 %dlH&=<>) )@ /B/.2?87%URF&=<>) )@ u/./ &2)5 )! ) ;!V @v _! -
Condensation of Classical Nonlinear Waves in a Two-Component System…
www.damtp.cam.ac.uk/user/ngb23/publications/2compCond.pdf7 May 2008: Condensation of Classical Nonlinear Waves in a Two-Component System. Hayder Salman and Natalia G. BerloffDepartment of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, CB3 0WA, UK. Abstract. We study the formation of -
electro
www.damtp.cam.ac.uk/user/tong/em/el6.pdf3 Dec 2022: of (at least) visible light, meaning ka 1. For this reason, we can. -
Digital Object Identifier (DOI) 10.1007/s00220-014-2046-5Commun.…
www.damtp.cam.ac.uk/user/md327/DT14.pdf25 Jul 2014: e. it is orthogonal to ahyper-surface) as. Ka b Kc = BCιB′ιC ′ιA′αA B′C ′αAαBαCιA′and ((K d K))a = a bcd Kbc Kd = 0 as abcd involves
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