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28 Jul 2015: Viall, N. M., Klimchuk, J. A. 2011, ApJ, 738, 24. Viall, N.

4 Aug 2015: pattern-ing the particle surface with active and passive sites (e.g. Janusparticles),23,24,28 (ii) spontaneous symmetry-breaking resultingfrom the advection of the field responsible for the phoreticresponse by ... K. Sia and G. M. Whitesides,

24 Mar 2015: Received 1 December 2014; published 24 March 2015). We describe the first analytically tractable example of an instability of a nonorientable minimal surfaceunder parametric variation of its boundary. ... 24] M. do Carmo and C. K. Peng, Stable complete

31 Dec 2015: 2p 1)" 2p1. L. x. 2+. 2q1Ly. 2# ez, (24). while the sensitivity on the vertical walls Hvert(y) at x = 0 and x = Lx can be obtained by symmetry.The ... Rev. Lett. 99, 048102 (2007).24 R. Golestanian, T. B. Liverpool, and A.

21 Jul 2015: Spicules. 24.  Jets and spicules dominate the region between the chromosphere and corona.

31 Dec 2015: 24]), forexample, at an air-water interface such as the surface of abubble [25,26]. ... Rev. 73, 68 (1948). [24] W. L. Nyborg, Acoustic streaming near a boundary,J.

31 Mar 2015: Similarly, when viscouseffects are dominant, thinning and pinching occur in a viscous(V) regime (24) where viscous and capillary forces balance, andhmin and ReðtÞ vary with τ as. ... of satellites is associated with inviscid fluids (20, 23, 24,

4 Aug 2015: Cambridge CB3 0HE, United Kingdom(Received 16 February 2015; revised manuscript received 24 April 2015; published 15 July 2015). ... 24] M. Padgett and R. Di Leonardo, Holographic opticaltweezers and their relevance to lab on chip devices, LabChip 11,

10 Oct 2015: 24. More terms: matching two regions. At c0:G0 = (R+ R)/2π.

5 Aug 2015: When the nutrient is essential for life, suchas oxygen for obligate aerobes, f (c) may vanish below somec [24,25]. ... μ̄ = 1λ. λ0. dx y(c)cb. (24). 022701-5. FRANÇOIS J. PEAUDECERF AND RAYMOND E.