By Ryan T Kelly

ISBN-10: 9535101064

ISBN-13: 9789535101062

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Lett. 91: 154104. APL/91/154104/1 Jonáš, A. & Zemánek, P. (2008). Light at work: the use of optical forces for particle manipulation, sorting, and analysis, Electrophoresis 29: 4813–4851. , Steffen, P. & Fischer, T. M. (2002). Migration of a droplet in a liquid: effect of insoluble surfactants and thermal gradient, J. : Condens. Matter 14: 4823–4828. org/0953-8984/14/i=19/a=309 Kim, H. S. & Subramanian, R. S. (1989a). Thermocapillary migration of a droplet with insoluble surfactant: I. Surfactant cap, J.

Surface tension mediated conversion of light to work, J. Am. Chem. Soc. 131: 5396–5398. 1021/ja900130n Ottino, J. M. & Wiggins, S. (2004). Introduction: mixing in microﬂuidics, Phil. Trans. R. Soc. Lond. A 362: 923–935. , Teitell, M. A. -Y. (2011). High-speed droplet generation on demand driven by pulse laser-induced cavitation, Lab Chip 11: 1010–1012. , Lereu, A. , Farahi, R. , Ferrell, T. L. & Thundat, T. (2006). Nonradiative surface plasmon assisted microscale Marangoni forces, Phys. Rev. E 73: 066311.

The second condition is dependent on tracer particle diameter, as the diffusion speed is proportional (Einstein-Stokes formula) to particle diameter. Fig. 19. The classical micro-PIV (A) and the idea of its modification as SeS-PIV (B) Assuming that the focused stream is narrower than the depth of focus of a microscope, the measurement becomes independent of optical parameters. Due to limiting the source of fluorescent light to well-defined thin surface, the signal to noise ratio is strongly improved – see Fig.

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