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4 Nov 2013: Adjacent to the Sleipner field,this sandstone formation is 200–300 m thick [Chadwicket al., 2004] (Figure 1). ... The highestintrareservoir mudstone is 5 m thick, although the ultimateseal is the Nordland Shale, which is 200 m thick [Zweigelet al., 2000

26 Jul 2013: Exp. Biol.200, 1145 1997. 29R. Ewoldt and G. H. McKinley private communication.30I.

4 Nov 2013: 8. 7. 6. Hei. ght (. mm. )5. 4. 3. 20 200 400 600 800 1000 1200. ... 20. 10. Tem. pera. ture. (C. ). 0. –10. –20. –300 200 400 600 800 1000 1200.

4 Nov 2013: efficiency of storage does indeed tend to a steady-state value. Six experiments wereconducted in a Hele-Shaw cell measuring 200 cm 30 cm 0.5 cm.

19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret

19 Oct 2013: Pub. lishe. d by. Man. ey P. ublis. hing. (c). IOM. Com. mun. icat. ions. Ltd. Lucidity and scienceIII: Hypercredulity, quantum mechanics,and scientific truth. PROFESSOR MICHAEL E. McINTYRECentre for Atmospheric Science at the Department of Applied

26 Jul 2013: 3040. 3. 2. 1. 0. 0 5 10 15 200 5 10 15 20. ... 200. 250. 300. 350. 6.00 1.0 2.0 3.0 5.5. FIGURE 18.

26 Jul 2013: dioxide,and has a width of 200–300 nm and a length of 1–2 µm.25 In both cases, the artificial bacteriaflagella possess a magnetic moment perpendicular to the long

27 Aug 2013: Protoplasma. 200(1-2):17–30.33. Yotsuyanagi Y (1953) Recherches sur les phénomenès moteurs dans les fragments de.

19 Oct 2013: and has had over 200 individuals directly contribute code to the kernel.

3 Feb 2013: We determined the temperature-dependent distributions of θfrom more than 200 scattering events by tracking the position of thecell body up to a distance of 70 μm from the corner (Fig.

19 Oct 2013: Pageoph, Vol. 118 (1980), Birkhiuser Vertag, Basel. An Introduction to the Generalized Lagrangian-Mean Description of Wave, Mean-Flow Interaction'. B y M. E. MCINTYRE z'3). A b s t r a c t - T h e generalized Lagrangian-mean description is motivated

19 Oct 2013: British Higher Education Policy in the last Twenty Years: The Murder of a Profession. Richard F. Gombrich. Tokyo, January 2000. Preamble. This is the text of a lecture I gave on 7 January 2000 in Tokyo at the Graduate Institute of Policy Studies

4 Nov 2013: σi. (a). 5 10 15 20 25 30–400. –300. –200. –100. ... 5. 10. 15. 20. 25. Rmc. –200. –150. –100. –50. 0.

19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret

20 Dec 2013: Part 3 General Relativity. Harvey Reall. Part 3 General Relativity 4/11/13 ii H.S. Reall. Contents. Preface vii. 1 Equivalence Principles 11.1 Incompatibility of Newtonian gravity and Special Relativity. 11.2 The weak equivalence principle. 21.3 The

26 Jul 2013: J. Fluid Mech. (2013), vol. 715, pp. 1–31. c Cambridge University Press 2013 1doi:10.1017/jfm.2012.484. Unsteady feeding and optimal strokes ofmodel ciliates. Sébastien Michelin1,† and Eric Lauga2. 1LadHyX – Département de Mécanique,

4 Nov 2013: of storage for experiment 1 (), 2 (), 3 (), 4 () and 5 (). The horizontal dashedline indicates a storage efficiency of 50 % which was reached in approximately 20 T 200 s.

19 Oct 2013: 23 Nov 2004 1:27 AR AR235-FL37-11.tex AR235-FL37-11.sgm LaTeX2e(2002/01/18) P1: IBD10.1146/annurev.fluid.37.061903.175710. Annu. Rev. Fluid Mech. 2005. 37:263–93doi: 10.1146/annurev.fluid.37.061903.175710. Copyright c 2005 by Annual Reviews. All

5 Oct 2013: Generalized Sampling: Extension to Frames and Inverse andIll-Posed Problems. Ben Adcock Anders C. Hansen † Evelyn Herrholz ‡ Gerd Teschke‡. Abstract. Generalized sampling is new framework for sampling and reconstruction in