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5 Feb 2015: 30.94268 12.20211 165.4088 14.02198 102.1661 22.39954 130.5360 24.54925 54.39669 27.35860 55.83458 18.97185 260.9365 28.02304 194.9137 ... 5112 155.7039 259.5173 223.7271 266.5150 248.4850 266.6068 122.2994 271.7742 286.1407 280.3929 241.9675 282.2188 162

5 Feb 2015: 277.1 558.79 317.32 36.05 325.27 668.09 344.24 134.28 340.67 316.73 355.22 397.9 361.75 491.87 386.29

16 Aug 2015: G. R. Gupta, D. Tripathi & H. E. Mason. P1.24. CHIANTI version 8.

27 Jul 2015: We examine an extended coronal source6 (2005 Aug 23) with little footpoint emission (left panel) and a more common looptop and footpoint event7 (2011 Feb 24, right panel). ... f). (g) (h). For the 2011 Feb 24 flare we see something close to a power law.

23 Jul 2015: 335 - 193 79.7% 31.2% 24.8% 44.0%. 335 - 171 72.1% 23.9% 23.0% 53.1%. ... 335 - 171 62.8% 29.4% 7.8%. 211 - 193 24.7% 40.8% 34.4%.

22 Jul 2015: 32. 24. 16. 8. 0. 16. Modeling results: high umbral loops. ... 6.0. 6.1. 6.2. 6.3. 6.4. 6.5. (d) Log (T) K. 07 Jul 2014 10:24 UT Another Time Frame.

22 Jul 2015: rMHD 24 Mm. 24 Mm. 17 Mm. R=700 Mm. CZ. corona. • ... chromospheretransition region. corona. Computational setup. 24 Mm. 17 Mm. • domain size: 24x24x17 Mm3. •

22 Jul 2015: 11:00 11:30 12:00 12:30 13:00Start Time (29Apr15 10:30:01). 2022. 24. 2628.

22 Jul 2015: Slajd 21. Slajd 22. Slajd 23. Slajd 24. Slajd 25. Slajd 26.

23 Feb 2015: dΓ =G 2F m. 5µ. 24(2π)4x2(3 2x (2x 1) k̂ s.

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.