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A reciprocal theorem for boundary-driven channel flows
www.damtp.cam.ac.uk/user/lauga/papers/111.pdf31 Dec 2015: 2p 1)" 2p1. L. x. 2+. 2q1Ly. 2# ez, (24). while the sensitivity on the vertical walls Hvert(y) at x = 0 and x = Lx can be obtained by symmetry.The ... Rev. Lett. 99, 048102 (2007).24 R. Golestanian, T. B. Liverpool, and A. -
SM.dvi
www.damtp.cam.ac.uk/user/ho/SM.pdf8 Nov 2015: By following a similar argument as forthe bosonic field and using eq.(1.24) we see that. ... P̂ψ(x)P̂1 = ηPγ0ψ(xP). (1.54). The u spinor has the property (1.24) which leads to eq.(1.25). -
Propulsion of Bubble-Based Acoustic Microswimmers Nicolas Bertin,1,*…
www.damtp.cam.ac.uk/user/lauga/papers/113.pdf31 Dec 2015: 24]), forexample, at an air-water interface such as the surface of abubble [25,26]. ... Rev. 73, 68 (1948). [24] W. L. Nyborg, Acoustic streaming near a boundary,J. -
Scientific Programming with R Stephen EglenLaurent Gatto September 6, …
www.damtp.cam.ac.uk/user/sje30/teaching/r/2015/spr-4up.pdf1 Oct 2015: joe. age height. 24.0 1.7. 30 / 191. Naming indexes of a vector. > ... x. [1] 20.00000 24.14214 27.32051 30.00000 32.36068. 62 / 191. -
Nondecaying Hydrodynamic Interactions along Narrow Channels Karolis…
www.damtp.cam.ac.uk/user/lauga/papers/108.pdf4 Aug 2015: Cambridge CB3 0HE, United Kingdom(Received 16 February 2015; revised manuscript received 24 April 2015; published 15 July 2015). ... 24] M. Padgett and R. Di Leonardo, Holographic opticaltweezers and their relevance to lab on chip devices, LabChip 11, -
www.damtp.cam.ac.uk/user/sje30/data/mosaics/hor/w00h72.txt
www.damtp.cam.ac.uk/user/sje30/data/mosaics/hor/w00h72.txt5 Feb 2015: 30.94268 12.20211 165.4088 14.02198 102.1661 22.39954 130.5360 24.54925 54.39669 27.35860 55.83458 18.97185 260.9365 28.02304 194.9137 ... 5112 155.7039 259.5173 223.7271 266.5150 248.4850 266.6068 122.2994 271.7742 286.1407 280.3929 241.9675 282.2188 162 -
Part II Principles of Quantum MechanicsMichaelmas 2015 Prof. A.C. ...
www.damtp.cam.ac.uk/user/acd/pqm.pdf14 Oct 2015: 2.4.24)r Note that the convolution theorem derived here. uNow return to the key condition in Eq. ... 4 THE HARMONIC OSCILLATOR 24. ‚ Consider a smooth potential V pxq with equilibrium point x0 (V 1px0q “ 0). -
Mathematical Methods University of Cambridge Part IB Mathematical…
www.damtp.cam.ac.uk/user/dbs26/1BMethods/All.pdf30 Nov 2015: 2.3 Self-adjoint differential operators 22. 2.4 Eigenfunctions and weight functions 24. ... 1)k1. ikeikθ (1.24). do in fact converge on the sawtooth function everywhere except at the discontinuity. -
on May 16, 2015http://rsfs.royalsocietypublishing.org/Downloaded from …
www.damtp.cam.ac.uk/user/gold/pdfs/streaming_focus.pdf16 May 2015: on May 16, 2015http://rsfs.royalsocietypublishing.org/Downloaded from. rsfs.royalsocietypublishing.org. ResearchCite this article: Goldstein RE, van de MeentJ-W. 2015 A physical perspective on. cytoplasmic streaming. Interface Focus 5:20150030. http: -
On the discretisation of the semiclassical Schrödinger equation with …
www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_02.pdf5 May 2015: On the discretisation of the semiclassical Schrödinger. equation with time-dependent potential. Arieh Iserles, Karolina Kropielnicka† & Pranav Singh‡. April 30, 2015. AMS Mathematics Subject Classification: Primary 65M70, Secondary 35Q41,65L05,
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