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J. Fluid Mech. (2015), vol. 778, pp. 335–360. c© ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Hewitt-2015.pdf11 Jan 2016: 0 100–100 200–200 300–300 400–400. 6. 2. 0. 4. 0.5. 0. ... 0 100–100 200–200 300–300 400–400. 15. 20. 5. 0. 10. 15. -
J. Fluid Mech. (2015), vol. 777, pp. 97–121. c© ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2015.pdf11 Jan 2016: Inlet. Outlet. Glycerine. 200 cm. Air6 cm 14 cm. FIGURE 10. ... predictions. Our experiments were performed in a Hele-Shaw cell composed of twoacrylic sheets, each 200 cm long and 14 cm high (see figure 10) and spacing w 0.38 -
Geophysical Journal InternationalGeophys. J. Int. (2015) 201, 764–782 …
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Lythgoe-2015.pdf11 Jan 2016: Thermal conductivity k W m1 K1 36 – 200 Stacey & Davis (2008); de Koker et al. ... For ex-ample a thermal conductivity of 200 W m1 K1 requires QCMB 32 TW for the inner core to be thermally unstable (̄ > 0) andconvect. -
Generalized sampling and infinite-dimensionalcompressed sensing Ben…
www.damtp.cam.ac.uk/research/afha/anders/BAACHGSCS_Rev10.pdf21 Jan 2016: Generalized sampling and infinite-dimensionalcompressed sensing. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd, -
Generalized sampling and infinite-dimensionalcompressed sensing Ben…
www.damtp.cam.ac.uk/research/afha/people/anders/BAACHGSCS_Rev10.pdf21 Jan 2016: Generalized sampling and infinite-dimensionalcompressed sensing. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd, -
Supplemental InformationMotility of Colonial Choanoflagellates and…
www.damtp.cam.ac.uk/user/gold/pdfs/choanowalks_SI1.pdf22 Jan 2016: v p(µ. m/s. )0 100 200. Area (µm2 ). 0. 10. -
Slender-ribbon theory
www.damtp.cam.ac.uk/user/lauga/papers/115.pdf25 Feb 2016: PHYSICS OF FLUIDS 28, 013101 (2016). Slender-ribbon theoryLyndon Koens. a). and Eric Lauga. b). Department of Applied Mathematics and Theoretical Physics, University of Cambridge,Wilberforce Road, Cambridge CB3 0WA, United Kingdom. (Received 20 May -
NE7405
www.damtp.cam.ac.uk/user/sje30/papers/network97.pdf26 Feb 2016: 0.6. 0.7. 0.8. 0.9. 1. 0 100 200 300 400 500 600 700. -
mssmRge.eps
www.damtp.cam.ac.uk/user/examples/3P7.pdf8 Mar 2016: Cop. yrig. ht. 201. 6 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Prepared for submission to JHEP. Supersymmetry. B. C. Allanacha F. Quevedoa. aDepartment of Applied Mathematics and -
Ferromagnetic and antiferromagnetic order in bacterial vortex…
www.damtp.cam.ac.uk/user/gold/pdfs/nphys3607-s1.pdf1 Apr 2016: 0 0.5 1-0.5-1Mean vortex spin. 0. 100. 200. 300. Freq. uenc. ... 1Stag. gere. dvo. rtex. spin. t = 50 t = 100 t = 150 t = 200 t = 250 t = 300.
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