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www.damtp.cam.ac.uk/user/sje30/data/mosaics/hor/w00h72.txt
www.damtp.cam.ac.uk/user/sje30/data/mosaics/hor/w00h72.txt5 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 -
www.damtp.cam.ac.uk/user/sje30/data/mosaics/w81_scan/w81s1on.txt
www.damtp.cam.ac.uk/user/sje30/data/mosaics/w81_scan/w81s1on.txt5 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 -
Coronal Loop Workshop VII
www.damtp.cam.ac.uk/user/astro/cl7/program.html16 Aug 2015: G. R. Gupta, D. Tripathi & H. E. Mason. P1.24. CHIANTI version 8. -
PowerPoint Presentation
www.damtp.cam.ac.uk/user/astro/cl7/talks/P3_8.pdf27 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. -
Nanoflare vs footpoint heating : Observational signatures
www.damtp.cam.ac.uk/user/astro/cl7/talks/CT1_4.pdf23 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%. -
Hi-C observations of an active region corona, and investigation of…
www.damtp.cam.ac.uk/user/astro/cl7/talks/CT1_6.pdf22 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. -
Classical transition region vs. low-lying loops Jul 22, 2015 ...
www.damtp.cam.ac.uk/user/astro/cl7/talks/IT2_2.pdf22 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. • -
SDO/A IA, Hinode/XRT, and NuSTAR For the poster and ...
www.damtp.cam.ac.uk/user/astro/cl7/talks/P1_21.pdf22 Jul 2015: 11:00 11:30 12:00 12:30 13:00Start Time (29Apr15 10:30:01). 2022. 24. 2628. -
Miniature coronal loops Krzysztof Barczyński1 Hardi Peter1 1) Max ...
www.damtp.cam.ac.uk/user/astro/cl7/talks/CT2_3.pdf22 Jul 2015: Slajd 21. Slajd 22. Slajd 23. Slajd 24. Slajd 25. Slajd 26. -
Standard Model Mathematical Tripos, Part IIIDr M B Wingate ...
www.damtp.cam.ac.uk/user/wingate/Notes/StdM/sheet3.pdf23 Feb 2015: dΓ =G 2F m. 5µ. 24(2π)4x2(3 2x (2x 1) k̂ s. -
Slide 1
www.damtp.cam.ac.uk/user/astro/cl7/talks/P1_5.pdf28 Jul 2015: Viall, N. M., Klimchuk, J. A. 2011, ApJ, 738, 24. Viall, N. -
Geometric pumping in autophoretic channels
www.damtp.cam.ac.uk/user/lauga/papers/107.pdf4 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, -
Instability of a Möbius Strip Minimal Surface and a ...
www.damtp.cam.ac.uk/user/gold/pdfs/meeks_mobius.pdf24 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 -
A reciprocal theorem for boundary-driven channel flows
www.damtp.cam.ac.uk/user/lauga/papers/111.pdf31 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. -
Heating Mechanisms (Reconnection and Waves) 1 M. Asgari-Targhi…
www.damtp.cam.ac.uk/user/astro/cl7/talks/IT1_1.pdf21 Jul 2015: Spicules. 24. Jets and spicules dominate the region between the chromosphere and corona. -
Propulsion of Bubble-Based Acoustic Microswimmers Nicolas Bertin,1,*…
www.damtp.cam.ac.uk/user/lauga/papers/113.pdf31 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. -
Plethora of transitions during breakup ofliquid filamentsJosé Rafael…
www.damtp.cam.ac.uk/user/hinch/publications/PNAS-2015.pdf31 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, -
Nondecaying Hydrodynamic Interactions along Narrow Channels Karolis…
www.damtp.cam.ac.uk/user/lauga/papers/108.pdf4 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, -
Instabilities of a thin coating on a vertical fibre; Newtonian,…
www.damtp.cam.ac.uk/user/hinch/talks/Leeds2015.pdf10 Oct 2015: 24. More terms: matching two regions. At c0:G0 = (R+ R)/2π. -
PHYSICAL REVIEW E 92, 022701 (2015) Feeding ducks, bacterial ...
www.damtp.cam.ac.uk/user/gold/pdfs/ducks.pdf5 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.
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