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5 Feb 2015: 34649 76.75254 19.35413 114.5557 19.55190 209.9197 20.88294 280.8345 22.38324 17.63480 23.10568 221.0292 23.55057 159.4284 25.3211 290.0137 ... 25.75550 182.9498 28.98305 234.4741 30.25903 146.4806 32.29067 89.69438 34.69780 67.14715 36.27759 246.7832

26 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.

16 Aug 2015: S. Regnier, R. W. Walsh & C. E. Alexander. P1.20.

21 Jul 2015: Chromospheric evaporation in response to coronal nanoflares: 20-36km/s @ 1.1-5.6MK @ loop tops (Patsourakos & Klimchuk 2006) [Increasing trend with temperature]. ... Skylab: 10-20 km/s in coronal UV lines (Cheng et al.

27 Jul 2015: 0. 10. 20. 30. 40. 50. 60. 70. E fre. e [10. ... 29]. 0. 10. 20. 30. 40. 50. 60. 70. E fre. e [10.

26 Jul 2015: 20. 30. 40. 50. 60. Tim. e [H. r]. 0 20 40 60 80 100 120 140S [Mm]. ... B0/L. 1 10 100 1000B0/L [Mas]. 0.0. 0.1. 0.2. 0.3. λQ [. RS]. WTD HeatingEmpirical Heating. Tmax [MK]. 0 20 40 60 80 100Loop Index.

23 Jul 2015: Steady-State Ohmic Heating. At 10 times higher resistivity:. Maximum tilt decreases from 20 to 3.

30 Jul 2015: 3) The loops' intensity increased and reached maximum after 5-20 minutes. ... On the EIT 195 Å images, the precursor looked like a loop with the size 20 Mm, but the arcade was invisible (see Figure 2 right).

30 Jul 2015: More details at: Dudík et al. 2014 (Astrophys. J., 796, 20)).

22 Jul 2015: sub.). Ô. 2000 particles evenly distributedthroughout lower corona. Ô. Uniform initial pitch angle (45)and kinetic energy (20 eV),simulated for 10 s. ... 2011 ApJ, 729, 101[19] Gordovskyy et al., 2014 A&A, 561, A72[20] Grady, K.

28 Jul 2015:  Red-shifts and blue-shifts (up to 20 kms-1) can be reproduced for the different simulated Hinode/EIS.

10 Oct 2015: Fluid Mech. 1994. 0. 20. 40. 60. 80. 100. 0 0.5 1 1.5 2. ... 1. 2. 3. 4. 5. 6. 7. 8. 10 20 30 40 50 60.

22 Jul 2015: Suppression of Heating of Coronal Loops Rooted in Opposite Polarity Sunspot Umbrae. Sanjiv K. Tiwari,. (J. K. Thalmann, A. R. Winebarger, N. K. Panesar#, R. L. Moore#). Marshall Space Flight Center. 21 Jul 2015 Loops VII, Univ. of Cambridge. sanjiv.k

31 Dec 2015: The vibration of the bubble interface underultrasonic forcing results in a strong “acoustic-streaming”jet [20]. ... dary acoustic) streaming, is then dominant [20]. It occursin viscous boundary layers near walls (see Ref.

28 Jul 2015: Fig. 5), we determine that the temperature of the. plasma is between 15 MK and 20 MK.

4 Nov 2015: Fluid Mech. 1994. 0. 20. 40. 60. 80. 100. 0 0.5 1 1.5 2. ... 1. 2. 3. 4. 5. 6. 7. 8. 10 20 30 40 50 60.

23 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

31 Dec 2015: This approachmakes an extensive use of the reciprocal theorem for Stokes flows.20. ... Kim and S. J. Karrila, Microhydrodynamics (Dover Publications, Inc., New York, 2005).20 L.

23 Jul 2015: measured and POSITIVE. 335 - 211 55.2% 54.0% 16.3% 29.6%. 335 - 193 61.9% 45.7% 20.4% 33.8%.

8 Feb 2015: 30) b Tr(Φ. 20). (µ may be regarded as a Lagrange multiplier for the condition Tr(Φ) = 0 whenvarying V (Φ)).

21 Jul 2015: The X-ray emission from loops is highly variable:. 3. SDO observation of an active region NOAA 11564 on 2012 September 7 at 7:20 UT. ... Waves Heating Models. Alfven Wave Turbulence Model. 20. Simulations of Alfven waves in coronal loops (van

28 Jul 2015: EIS: 11:02-17:27 UT 20-steps raster, cadence 212 s, exposure time 9s.

22 Jul 2015: Slajd 15. Slajd 16. Slajd 17. Slajd 18. Slajd 19. Slajd 20.

22 Jul 2015: 2011b). Wednesday 22 July 15. blue. 0 10 20 30time [min].

4 Aug 2015: f C. ambr. idge. on. 04/0. 8/20. 15 1. 5:21. :05. ... Uni. vers. ity o. f C. ambr. idge. on. 04/0. 8/20.

4 Aug 2015: However, recenttheoretical investigation suggests that interactions could. have a longer spacial extent and a slower decay rate thanpreviously thought [20]. ... Meanwhile,at large separations the values compare very well, with thelargest discrepancy

23 Jul 2015: N. Shore,22 A. Sillanpää,20 J. Sitarek,1 I. Snidaric,5 D. Sobczynska,9. F. ... L. Takalo,20 H. Takami,19 F. Tavecchio,3 P. Temnikov,21 T. Terzić,5 D.

24 Mar 2015: DOI: 10.1103/PhysRevLett.114.127801 PACS numbers: 68.15.e, 02.40.-k, 47.20.Ky, 83.10.-y. The subject of this Letter lies at the intersection ofseveral branches ... 137 (American Mathemati-cal Society, Providence, RI, 2007). [20] For a summary of open

28 May 2015: Op;cal Conduc;vity. 0 5 10 15 20 250. 2. 4. 6. ... 20. Hartnoll, 2014. which of these processes describes actual materials? Lesson 2: Incoherent Transport.

26 Jul 2015: 15. 20. 25. 30. 35. 40. 45. 50. 190 200 210 220 230 240 250 260. ... 5. 10. 15. 20. 25. 30. 0 900 1800 2700 3600 4500.

5 Aug 2015: coli, with v 20 μm/s and τ 1 s, run 20 μm, but it can be considerably longer for otherbacteria [28]. ... 30, 235 (1971). [20] J. D. Murray, Mathematical Biology II Spatial Models andBiomedical Applications, 3rd ed.

22 Apr 2015: Fig. 6 shows thetrajectories of non-interacting pullers with a 0.8 swimmingtowards a sphere of size A 20. ... Fig. 8provides a general picture of the scattering dynamics, where wex the colloid size to A 20.

9 Nov 2015: We already have the Green’s function. solution to the homogeneous problem in (7.20), so we simply need to find a solution to. ... sin x. sin 1. 1. xf(ξ) sin(1 ξ) dξ (7.35). using the result (7.20). –

1 May 2015: Notice that higher temperatures induce unwantedcaramelization.20 The molten sugar is poured into a cylindrical Teflonmold (length 14 cm and inner diameter 2 cm) until it fills the entirebore volume (approximately ... Phys. Rev. E 2013, 87, 011003.(20)

30 May 2015: Forpolynomial reconstructions see [19] and [20]. IV. NUGS IN ONE DIMENSIONIn one dimension we take ZK R̂ to be the interval. ... Com-put. Phys., vol. 229, no. 3, pp. 933–946, 2010. [20] B.

31 Mar 2015: These satellites aretypically much smaller than the primary drop (20) and almostalways undesirable in applications (2). ... Nat Phys 5:697–702. 20. Collins RT, Harris MT, Basaran OA (2007) Breakup of electrified jets.

30 May 2015: Forpolynomial reconstructions see [19] and [20]. IV. NUGS IN ONE DIMENSIONIn one dimension we take ZK R̂ to be the interval. ... Com-put. Phys., vol. 229, no. 3, pp. 933–946, 2010. [20] B.

5 Feb 2015: Define some common functions for plotting.soma.rad <- 20/2 #20 um soma diameter.on.col <- "red"of.col <- "blue"show.on <- function(pts, main) {. symbols(pts, circles = rep(soma.rad,

9 Nov 2015: There are two real zeros.One is close to 0.2144 and the other is (up to 20 digits). ... V̇ CD̂V = F(t), U(0) = U0, (31) advectionnumv. 21. 25 20 15 10 5.

21 Jan 2015: The dimensionless form of the inequality (2.20) is. B < QF < Qmax BD1(1B). ... 1 20. 0.5. 1.0. 0 1 2 0 1 2 3.

3 Jun 2015: roto. rro. tor. 0 5 10 10 20 30 0 1 2 315 20 25 30. ... 0.9. 0.85 10 15. 0.98 1.021. 20 25 30. 102030. 51525.

25 Sep 2015: l use. onl. y. FL47CH15-Goldstein ARI 1 December 2014 20:34. 1. ... FL47CH15-Goldstein ARI 1 December 2014 20:34. g h. a b c.

1 Oct 2015: x. [1] 20.00000 24.14214 27.32051 30.00000 32.36068. 62 / 191. ... y. 0 5 10 15 20 25 30. 0.0. 0.5. 1.0.

4 Oct 2015: gj =. Nk=N. Aj,kfk, j = 0,. , 2N, gj = ρ̃N (λj,N ), (20). ... 20 40 60 80 1000. 0.2. 0.4. 0.6. 0.8. 1. Frequencies.

4 Oct 2015: gj =. Nk=N. Aj,kfk, j = 0,. , 2N, gj = ρ̃N (λj,N ), (20). ... 20 40 60 80 1000. 0.2. 0.4. 0.6. 0.8. 1. Frequencies.

13 Jan 2015: 20). Here (17) has been used. Eq. (20) expresses the conservation of charge. ... drop. tterms, and replace (.) by n(.)|. Thus, from (20), we expect that n J|. =

26 Jul 2015:  The loop is highly non-Maxwellian, with κ < 2.  Calibration uncertainty is large (20%) and ought to be reduced in future missions.

10 Jul 2015: 20. 0. 20. Wx0 thresholded to s = 150. 0 500 1000 1500 2000 2500 3000 3500 4000 45000. ... Magn.Reson. Imaging, 58(6):1182–1195, 2007. [20] C. Poon. On the role of total variation in compressed sensing.

17 Dec 2015: x1 = x′1 hx′21 h2x′31 k(x2,x3; h). (2.20). where the function k denotes an integration constant that we can choose appropriately.The simplest VP integrator satisfying ... 20. effective algorithms for the solution of linear systems, computation of

26 Oct 2015: An,m =4. ab. [0,a][0,b]sin. (nπxa. )sin. (mπyb. )f(x, y) dx dy (3.20). ... x2 (λ)(6 λ). 4!x4. (λ)(6 λ)(20 λ)6! x6. Θ1(x) = x (2 λ).