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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: 174.3860 212.0221 183.4615 275.1014 184.2850 184.2154 184.4135 244.6897 187.3142 70.22635 190.3387 94.84615 197.1700 121.0863 200.5851 -
Dynamic evolution of EUV loops Yin Zhang, Baolin Tan ...
www.damtp.cam.ac.uk/user/astro/cl7/talks/P1_6.pdf26 Jul 2015: 0 50 100 150 200 250-20. -10. 0. 10. 20. 30. ... 0 50 100 150 200 250-40. -20. 0. 20. 40. 60. -
Set of observationsSet of observations ● IRIS: 14:04- 17:44 ...
www.damtp.cam.ac.uk/user/astro/cl7/talks/P1_29.pdf28 Jul 2015: In particular, strong blueshifts ( 200 km/s) are simultaneously observed in both IRIS Fe XXI 1354 A and HINODE/EIS Fe XXIII 263 A hot (>10 MK) emission lines at one ... Large blue shifts (200 km/s) in IRIS Fe XXI and EIS Fe XXIII high temperature lines -
Particle dynamics in a non-flaring solar active region
www.damtp.cam.ac.uk/user/astro/cl7/talks/P1_4.pdf22 Jul 2015: 30. -80. -30. So. lar-. Y [. arc. se. c]. a ). 100 150 200 250. Sola r-X [ar csec]. b). S L1. ... S L2. SL3. CL1. 100 150 200 250. S olar-X [a rcsec]. -
Department of Mathematics,Center for mathematicalPlasma-Astrophysics…
www.damtp.cam.ac.uk/user/astro/cl7/talks/P3_2.pdf26 Jul 2015: 0. 5. 190 200 210 220 230 240 250 260. Ma. ... 15. 20. 25. 30. 35. 40. 45. 50. 190 200 210 220 230 240 250 260. -
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: 2014, Sol. Phys., 289, 1029. AIA FeXVIII 29Apr2015 10:30:01.120 UT. 100 200 300 400 500X (arcsecs). ... rcse. cs). AIA FeXVIII 29Apr2015 10:30:01.120 UT. 100 200 300 400 500X (arcsecs). -
PowerPoint Presentation
www.damtp.cam.ac.uk/user/astro/cl7/talks/P3_6.pdf26 Jul 2015: The time was broken into 200 s for the linear increase, 100 s for the plateau, and 200 s for the linear decrease. -
Efficient Modeling of Two-fluid Coronal Plasma: Effects of Electron…
www.damtp.cam.ac.uk/user/astro/cl7/talks/P1_26.pdf22 Jul 2015: 200 s)I Single-fluid models tacitly assume electron and ion populations in equilibrium violated if heating. ... 1(b) Same as Fig. 1(a), but for aseries of 23 square pulses, each lasting 200 s with amplitudes chosen from a power-law distribution. -
Instabilities of a thin coating on a vertical fibre; Newtonian,…
www.damtp.cam.ac.uk/user/hinch/talks/ICL2015.pdf4 Nov 2015: 100. 200. 300. 400. 500. 600. 700. 800. 0 0.5 1 1.5 2. ... 150. 200. 250. 300. 350. -4 -2 0 2 4 6 8 10 12. -
A Computational Method for Modelling Chromospheric Evaporation
www.damtp.cam.ac.uk/user/astro/cl7/talks/P2_6.pdf23 Jul 2015: Wavefront location xf (t ) (solid line) and STS approximation(asterisks) with resolution : a) Nx = 20, Nt = 50, b) Nx =40, Nt = 100, c) Nx = 80, Nt = 200, d) Nx = 160, Nt -
Emission measure distribution of nanoflare-heated coronal loops…
www.damtp.cam.ac.uk/user/astro/cl7/talks/P1_10.pdf30 Jul 2015: 2.2 Critical condition:. We model the nanoflares with 200 s triangular heating functions. -
Coronal_loops_7_Reva
www.damtp.cam.ac.uk/user/astro/cl7/talks/P1_18.pdf30 Jul 2015: 4) The loops' intensity gradually decreases over approximately 1 hour. All four arcades had similar sizes: the loop length was 170 Mm, and the arcade length was 200 Mm (see Figure -
Instabilities of a thin coating on a vertical fibre; Newtonian,…
www.damtp.cam.ac.uk/user/hinch/talks/Leeds2015.pdf10 Oct 2015: 100. 200. 300. 400. 500. 600. 700. 800. 0 0.5 1 1.5 2. ... 150. 200. 250. 300. 350. -4 -2 0 2 4 6 8 10 12. -
Scientific Programming with R Stephen EglenLaurent Gatto September 6, …
www.damtp.cam.ac.uk/user/sje30/teaching/r/2015/spr-4up.pdf1 Oct 2015: ty w. ith N. orm. al F. it. 0.000.050.100.150.200.25. 60 65 70 75 80. ... Alto 1. Soprano 2. 60 65 70 75 80. 0.000.050.100.150.200.25. Soprano 1. -
Heating Mechanisms (Reconnection and Waves) 1 M. Asgari-Targhi…
www.damtp.cam.ac.uk/user/astro/cl7/talks/IT1_1.pdf21 Jul 2015: At present the spatial resolution of some of the DC models (Binger and Peter 2011) is 200 km. -
Description of MEA data for Charlesworth et al (2015) ...
www.damtp.cam.ac.uk/user/sje30/papers/charlesworth2015_data.pdf17 Sep 2015: Electrodes were aligned in asquare array, spaced 200 um apart.). 1. -
on June 3, 2015http://rsif.royalsocietypublishing.org/Downloaded from …
www.damtp.cam.ac.uk/user/gold/pdfs/metachronal_jrsi.pdf3 Jun 2015: 200. 0. 200. 100. 0. colonyaxis. uÒtur. uq. t = 0 ms 6 ms 12 ms 18 ms 24 ms. ... beats0 200 400 600. no. beats. no. beats0 10 20 30 40 50 0 20 40 60 80 100. -
Instability of a Möbius Strip Minimal Surface and a ...
www.damtp.cam.ac.uk/user/gold/pdfs/meeks_mobius.pdf24 Mar 2015: Comput. Phys. 200, 299 (2004). [12] D. Leppinen and J. R. -
Do Dissolving Objects Converge to a Universal Shape?Elias Nakouzi,†…
www.damtp.cam.ac.uk/user/gold/pdfs/dissolution.pdf1 May 2015: b) Poly(ethyleneglycol) cylinder at 5, 150, 200, and 250 min. Individual image size: 14cm 4 cm. -
on May 16, 2015http://rsfs.royalsocietypublishing.org/Downloaded from …
www.damtp.cam.ac.uk/user/gold/pdfs/streaming_focus.pdf16 May 2015: eH. uH. uyej. 400. 0.5. 0.006 200. –200. –400. 0. 60. ... x (µm)–400 –200 200 4000. –1. 1. –10 –5 0. z (mm). -
Continuous Compressed Sensing of Inelastic and Quasielastic Helium…
www.damtp.cam.ac.uk/research/afha/anders/CS4HAS_Arxiv_2.pdf4 Oct 2015: 200 100 0 100 2000. 0.2. 0.4. 0.6. 0.8. 1. ... For a complete picture of the spectrum consult Figure 7. Notice that the smaller featuresshown here are over 200 times smaller than the elastic peak. -
Continuous Compressed Sensing of Inelastic and Quasielastic Helium…
www.damtp.cam.ac.uk/research/afha/people/anders/CS4HAS_Arxiv_2.pdf4 Oct 2015: 200 100 0 100 2000. 0.2. 0.4. 0.6. 0.8. 1. ... For a complete picture of the spectrum consult Figure 7. Notice that the smaller featuresshown here are over 200 times smaller than the elastic peak. -
Nondecaying Hydrodynamic Interactions along Narrow Channels Karolis…
www.damtp.cam.ac.uk/user/lauga/papers/108.pdf4 Aug 2015: Two additional large connections arepositioned 200 μm away from the narrow channelsallowing pressure equalization between the two reservoirs.For the fabrication of the chips, we use focused ion beam,photolithography, and -
Geometric pumping in autophoretic channels
www.damtp.cam.ac.uk/user/lauga/papers/107.pdf4 Aug 2015: Cðx;ZÞð Þdsðx;ZÞ:. (8). The upper and lower boundaries of the domain are discretizedinto 200 straight-line segments, and C and dC/dn are assumedconstant over each element. -
Green Algae as Model Organisms for Biological Fluid Dynamics
www.damtp.cam.ac.uk/user/gold/pdfs/green_algae.pdf25 Sep 2015: r. Ω (r. ad/s. ). ω (rad/s). r. 1 mm. 200 μm. ... 200 μm. 200 μm. AverageInfalling dataSingularity model. t. Figure 6(a) Observations of the hydrodynamic bound state of Volvox. -
Geometric capture and escape of a microswimmer colliding with an…
www.damtp.cam.ac.uk/user/lauga/papers/105.pdf22 Apr 2015: For instance, even with A 200 and a 0.8, if a sphericalswimmer is initially placed parallel to the surface, the initialdistance from the colloid below which the body is trapped ... 0. A threshold of r 1.5 is chosen in the. Fig. 13 Trapping times Th (with -
Cover Realistic Magnetic Reconnection Processes
www.damtp.cam.ac.uk/user/astro/cl7/talks/IT3_2.pdf23 Jul 2015: the order of a couple hundred shear Alfven times, or 20 ls insmall plasmas such as Alcator C-Mod or MAST to 100–200. -
Numerical stability in the presence of variable coefficients Ernst ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_10.pdf3 Apr 2015: is 8.14 1017 and for N = 200 the norm is2.211033) and has not been displayed in the figure. ... For N = 200 we have. 21. Option α ‖x̃x‖L1 6.22333 105 1.29 105R1 9.78111 106 7.71 106L2 9.96161 106 7.80 106R2 5.07442 105 -
PHYSICAL REVIEW E 92, 023004 (2015) Phase-separation models for ...
www.damtp.cam.ac.uk/user/lauga/papers/109.pdf4 Aug 2015: Thediameter of the particle (Xanthan gum in the experiment ofRef. [42]) is about 200 μm. -
J. Fluid Mech. (2014), vol. 745, pp. 592–620. c© ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2014.pdf21 Jan 2015: J. Fluid Mech. (2014), vol. 745, pp. 592–620. c Cambridge University Press 2014doi:10.1017/jfm.2014.76. 592. Fluid injection into a confined porous layer. Samuel S. Pegler1,†, Herbert E. Huppert1,2,3 and Jerome A. Neufeld1,4. 1Institute of -
J. Fluid Mech. (2014), vol. 757, pp. 330–353. c© ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2014-1.pdf21 Jan 2015: J. Fluid Mech. (2014), vol. 757, pp. 330–353. c Cambridge University Press 2014doi:10.1017/jfm.2014.469. 330. Fluid migration between confined aquifers. Samuel S. Pegler1,†, Herbert E. Huppert1,2,3 and Jerome A. Neufeld1,4. 1Institute of -
ELIFE06088 1..31
www.damtp.cam.ac.uk/user/gold/pdfs/Drosophila_axis.pdf23 Sep 2015: elifesciences.org. RESEARCH ARTICLE. Cortical microtubule nucleation canorganise the cytoskeleton of Drosophilaoocytes to define the anteroposterior axisPhilipp Khuc Trong1,2, Hélène Doerflinger3, Jörn Dunkel1,4, Daniel St Johnston3,Raymond E -
CORONAL LOOP VII, Workshop
www.damtp.cam.ac.uk/user/astro/cl7/cl7_abstract_book.pdf15 Jul 2015: CORONAL LOOP VII WORKSHOP Cambridge 21 – 23 July 2015. ABSTRACTS. SESSION 1: Coronal Heating: Global Active Region Models and. Mechanisms. INVITED TALKS. IT1.1 Mahboubeh Asgari-Targhi. Title - Heating Mechanisms (Reconnections vs Waves) Authors: -
J. Fluid Mech. (2014), vol. 756, pp. 844–869. c© ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Hewitt-2014-3.pdf21 Jan 2015: roughly 1–5 m deep) than the formation itself (roughly 200 mdeep) (Bickle et al. -
On the Solvability Complexity Index, the n-Pseudospectrumand…
www.damtp.cam.ac.uk/research/afha/anders/JAMS_Final_Preprint2.pdf8 Nov 2015: On the Solvability Complexity Index, the n-Pseudospectrumand Approximations of Spectra of Operators. ANDERS C. HANSENApplied and Computational Mathematics, California Institute of Technology,. hansen@acm.caltech.edu. Abstract. We show that it is -
The Standard Model
www.damtp.cam.ac.uk/user/wingate/Notes/StdM/stdmodel.pdf2 Mar 2015: M AT T H E W B W I N G AT E. T H E S TA N D A R D M O D E L. These notes are for use with the Cambridge University Part III lecture course The Standard Model, givenin the Department of Applied Mathematics and Theoretical Physics in Lent Term 2015. -
On the Solvability Complexity Index, the n-Pseudospectrumand…
www.damtp.cam.ac.uk/research/afha/people/anders/JAMS_Final_Preprint2.pdf8 Nov 2015: On the Solvability Complexity Index, the n-Pseudospectrumand Approximations of Spectra of Operators. ANDERS C. HANSENApplied and Computational Mathematics, California Institute of Technology,. hansen@acm.caltech.edu. Abstract. We show that it is
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