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An inverse method for estimating thickness and volume with time of a…
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Cowton-2016.pdf20 Jan 2017: Red outline = 20 Hz; green outline = 30 Hz; and blue outline = 40 Hz. -
Newtonian Twistor Theory
www.damtp.cam.ac.uk/user/md327/james_thesis.pdf29 Jul 2017: 2.2.1 Theorems. 20. 2.2.2 Flat model. 23. 2.2.3 Deformations. 23. 2.3 Induced frames and metrics. ... are ASD Einstein rather than just Ricci-flat [80], hyper-Hermitian [20], or scalar-flat Käh-. -
Uniform and high-order practical implementation ofSturm–Liouville…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_04.pdf15 Feb 2017: A , [B, C ]] = 0, [C , [E , E ]] = 0, (3.20)[B, [A , B]] = 0, [C , [A , C ]] = 0, (3.21)[B, [A , D]] = 0, [C , [A , E ]] = 0, (3.22)[B, ... 333. 7511. 20. 412. 412. 125. 4038. 3417. 2857. 2. 408. -
PHYSICAL REVIEW E 92, 022701 (2015) Feeding ducks, bacterial ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/PeaudecerfGoldstein2015.pdf4 Dec 2017: coli, with v 20 μm/s and τ 1 s, run 20 μm, but it can be considerably longer for otherbacteria [28]. ... 30, 235 (1971). [20] J. D. Murray, Mathematical Biology II Spatial Models andBiomedical Applications, 3rd ed. -
Floquet Time Crystals Dominic V. Else,1 Bela Bauer,2 and ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Else_etal2016.pdf4 Sep 2017: Nevertheless, an initial state that is not an eigenstate couldpotentially heat very slowly, leading to nontrivial intermedi-ate-time dynamics [16–20].) This is analogous to the fact(which follows from ... Saito, Phys. Rev. Lett. 116,. 120401 (2016).[20] -
Structural phase transitions of interacting membranes
www.damtp.cam.ac.uk/user/gold/pdfs/structural_phase_transitions.pdf19 Dec 2017: For intermediate chain length lipids the shift in melt-ing temperature upon dehydration to some 5 —10 A fromits values in excess water is on the order of 10—20 ... 0. 18 O. 19 0.20. FIG. 7. Detail of a phase diagram in the region of the criticalpoint -
Twisted Elastic Rings and the Rediscoveriesof Michell’s Instability…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Goriely2006.pdf22 Nov 2017: thrust and gravity. Arch. Ration. Mech. Analysis 84, 289–338 (1981)20. Zajac, E.E.: Stability of two planar loop elasticas. ... Physica D. 105, 20–44 (1997)34. Liu, G.H., Schlick, T., Olson, A.J., Olson, W.K.: Configurational transitions in Fourier -
I. On governors
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Maxwell1868.pdf11 Dec 2017: Clerk M axwell, M.A., F.R.SS.L. &E.Received Feb. 20, 1868. A G overnor is a part of a machine by means of which the velocity of the -
min_concentration_new_thesis.eps
www.damtp.cam.ac.uk/user/hinch/publications/SIAM77_247.pdf14 Feb 2017: SIAM J. APPL. MATH. c 2017 Society for Industrial and Applied MathematicsVol. 77, No. 1, pp. 247–266. FINITE AMPLITUDE STEADY-STATE ONE-DIMENSIONAL WAVESIN FLUIDIZED BEDS. YURI D. SOBRAL† AND E. JOHN HINCH‡. Abstract. In this work, we -
Phase Structure of Driven Quantum Systems Vedika Khemani,1,2…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Khemani_etal2016.pdf4 Sep 2017: Thouless, Phys. Rev. B 27, 6083 (1983).[20] T. Oka and H.
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