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5 Oct 2013: 2. where T = [1, 1) is the unit torus). Given the Fourier coefficients of f , we would like to reconstruct in theorthonormal basis of Chebyshev polynomials φj (x) = cj Tj (x) ... Given that the first kind Chebyshev polynomials Tj are orthogonal with.

30 Jul 2014: 8:23–29. doi: 10.1007/BF02353701.Brumley DR, Polin M, Pedley TJ, Goldstein RE. 2012.

14 Jun 2014: s < s 1 ## p r e p a r e t o p r o c e s s n e x t s u b j e c tj < j

30 Aug 2009: J Geophys Res—Oceans 110(C9):C09S04.1–C09S04.12. Canadell JG, Quere CL, Raupach MR, Field CB, Buitehuis ET, Ciais P, Conway TJ, Gillett NP, HoughtonRA, Marland G (2007) Contributions

20 Jul 2021: RESEARCH ARTICLE. Hydrodynamics and direction change of. tumbling bacteria. Mariia DvoriashynaID, Eric LaugaID. Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, United. Kingdom. e.lauga@damtp.cam.ac.uk.

26 Feb 2014: 20131160, published 26 February 201411 2014 J. R. Soc. Interface Kirsty Y. Wan, Kyriacos C. Leptos and Raymond E. Goldstein Lag, lock, sync, slip: the many 'phases' of coupled flagella.

8 Jul 2021: RESEARCH ARTICLE. The bank of swimming organisms at the. micron scale (BOSO-Micro). Marcos F. Velho Rodrigues1, Maciej LisickiID2, Eric Lauga1. 1 Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, United.

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]:.

2 Sep 2012: Magar V, Goto T, Pedley TJ (2003) Q J Mech Appl Math 56:65–91.35.

14 Jun 2014: Self-organization in the developing nervoussystem: theoretical models. Stephen J. Eglen1 and Julijana Gjorgjieva1. 1Cambridge Computational Biology Institute, Department of Applied Mathematics and TheoreticalPhysics, University of Cambridge,