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19 Dec 2012: 24 • • 25. οργανώθηκε η κοινωνία μας τα τελευταία 40 χρόνια, αφετέ-ρου δε, της πληθώρας ευτελών μηνυμάτων που, με τη βοή-θεια Μέσων Μαζικής

3 Oct 2012: Department of Applied Mathematics. and Theoretical Physics. Goldstein Lab. Teaching. DAMTP Summer School on Fluid Dynamics of Sustainability and the Environment. Supplementary Reading (Biological Physics). The following is a collection of primary

27 Aug 2012: h. 1. 992. 24:3. 13-3. 58. D. ownl. oade. d fr. ... u. R. ev. F. luid. Mec. h. 1. 992. 24:3. 13-3.

19 Oct 2012: Instead, we adopt a new approach by adapting aclosure of Hinch and Leal [24] to d 2, yielding. ... G. Woodhouse and R. E. Goldstein (unpublished).[24] E. J. Hinch and L.

31 Jan 2012: ij. 12. ′′ij 18. ′′′ij. (24). Clearly therefore χij is equivalent to the positive Gij under the arbitrariness ex-pressed by (16).

27 Jul 2012: the various coefficients appearing in (3.24), (3.25) depend on the dimensionless couplingsgi. ... 2 112Rφ2, but this may be compensated at zero loop order in (3.24).

27 Dec 2012: 22]. Recent experimental evidence [24] is consistentwith the hypothesis of orbit flexibility and hydrodynamiccoupling as a possible origin of flagellar synchronization.At the same time, synchronization of an isolated pair is ... Custom-made rotation

19 Jan 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J.

5 Sep 2012: 49) , and open 3D bulk suspensions (7, 18,24, 25), bacteria were confined in closed microfluidic chambers to. ... 6. Berg HC (1997) Motile behavior of bacteria. Phys Today 53:24–29.7.

2 Sep 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J.