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6 Jun 2012: Cop. yrig. ht. 201. 2 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Part II Mathematical Biology Lent Term 2012. lecturer: Professor Peter Haynes (phh@damtp.cam.ac.uk). May 31, 2012. These

15 Aug 2012: t0,x0,. ,xr1, tr) for some r 0 with xi Z2{O}, ti T, and tj 6= R for. ... iii) r = s 1, xi = yi for i r 1, tj = uj for j r, ys O and us = R.

2 Sep 2012: Phys Rev E Stat Nonlin Soft Matter Phys 80:041922.22. Ishikawa T, Locsei JT, Pedley TJ (2008) Development of coherent structures in concen-. ... Science 325:487–490. 43. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of

16 May 2012: Let Ti,(i = 1,2,3) denote a basis of su(2) with commutation relations [Ti,Tj] = ϵijkTk and TiT i := TiTjδij = 3412.

5 Sep 2012: Science 317:105–108. 52. Pedley TJ (2010) Collective behaviour of swimming micro-organisms.

15 Aug 2012: PERCOLATION ANDDISORDERED SYSTEMS. Georey GRIMMETT. 2PREFACEThis course aims to be a (nearly) self-contained account of part of the mathematicaltheory of percolation and related topics. The rst nine chapters summarise rigorousresults in percolation

2 Sep 2012: FL43CH26-Koch ARI 15 November 2010 14:32. Collective Hydrodynamics ofSwimming Microorganisms:Living FluidsDonald L. Koch1 and Ganesh Subramanian21 School of Chemical and Biomolecular Engineering, Cornell University, Ithaca,New York 14853; email:

2 Sep 2012: J Fluid Mech 669:167–177.21. Ishikawa T, Locsei JT, Pedley TJ (2010) Fluid particle diffusion in a semidilute suspension.

2 Sep 2012: Due to the linearity of the Stokes equations, theirtranslational and rotational velocities, vi and ωi, dependlinearly on all external forces and torques, Fj and Tj [12,18]:.

15 Aug 2012: PERCOLATION ANDDISORDERED SYSTEMSGeorey GRIMMETT. 2PREFACEThis course aims to be a (nearly) self-contained account of part of the mathematicaltheory of percolation and related topics. The rst nine chapters summarise rigorousresults in percolation