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21 Oct 2014: Image Processing for Fluid Dynamics.  Stuart Dalziel. DL Research Partners 1993 – 2001. Version 2.3  DL Research Partners; September 2001 1. Contents Contents.1. 1 Concept.1. 2 DigImage: Particle Tracking.3 2.1 IMAGE CAPTURE. 3 2.2 PARTICLE

6 Oct 2014: ǫABǫF ′Q′C̃A′B′E′Q′ ǫAB(ǫA′E′ǫ. F ′. B′ ǫF ′. A′ ǫB′E′)R. 24+ ǫA′B′ǫ. ... 24. a,b holomorphic functions on C. For these to agree we require.

21 Oct 2014: πFn(θ φ) dφ = f(θ) , (1.24). – 8 –. using property ii) of the Fejér kernel.

30 Aug 2014: t(t v). ], (1.24). where t and n are, respectively, the local tangent and normal vectors along the filament. ... 1.24), up to the unknown translational and rotational velocities,(U,), which will be determined by imposing the overall force-free and

28 Nov 2014: Pg ρ0. r<. wb dV (24). and thus we obtain the scaling relation. ... ρ0a4. )a3 = D. 24. μa7, (53). where we have substituted κ/N 2 = 4/ν.

9 Sep 2014: For example, it is nowpossible to measure the force required to hold a swimmingspermatozoon [24–26], alga [27] or bacterium [28] in an opticaltrap.

21 Oct 2014: DiDiDiDiggggImage: DigiFile Utility Index. Version 2.3  DL Research Partners September 2001 24.

13 Jul 2014: Arakawa’s method is used for evaluation of thePoisson bracket.24 The time stepping algorithm is the third.

22 Jan 2014: Received 8 April 2013; revised 24 September 2013; accepted 7 October 2013;first published online 25 November 2013).

30 Jul 2014: Funding: See page 14. Received: 11 March 2014Accepted: 24 June 2014Published: 29 July 2014.