Search

19 Aug 2011: 1 10-6. 1.5 10-6. 2 10-6. 0 200 400 600 800 1000 1200. ... 1.5 10-6. 2 10-6. 0 200 400 600 800 1000 1200.

10 Apr 2011: Chloroplasts. Indifferent zone. 400. 200. y (μ. m). x (μm). 0. ... 0 200 400–200–400. –200. –400. (b) (c). Figure 1. (a) Internode ‘stalks’ of the Chara Corallina algae consist of single,millimetre-diameter and 10 cm long cells.

10 Apr 2011: 400 –200 200 4000 –40 –20 20 400. Position (μm). x (μm). ... 1). u the. ory. (μm. s–1. ). uNMR (μm s–1). –400 –200 200 400.

10 Apr 2011: Due to plume’s downward motion, the. 200 400 600 800Film thickness (µm). ... 0 cm. )-3. 0 100 200 300z (µm). 0.1. 0.15. 0.2.

10 Apr 2011: carteri using standard biological oxygen demand(BOD) bottles. We find Rb 50 –200 m. ... 2), viewedat 4 magnification on the stage of an inverted microscope(Nikon Diaphot 200).

10 Apr 2011: on. July. 24,. 200. 9 w. ww. sci. ence. mag. org. ... July. 24,. 200. 9 w. ww. sci. ence. mag. org. Dow.

10 Apr 2011: The Atmosphere During the Younger Dryas [pp.195-197]. A 50,000-Year Record of Climate Oscillations from Florida and Its Temporal Correlation with the Heinrich Events [pp.198-200].

10 Apr 2011: Figure 5(a) shows the. 0 50 100 150 200 2500. 50. ... 100. 150. 200. X (µm). Y (µm. ). FIG. 4. Flows at the bottom of a pendant drop.

10 Apr 2011: 2, 3, 5 for 0 = 3.8, D0 = 50, = 3, v0 = 0.2, = 3, = 0.5 in the periodic domain of 200 200 units.

10 Apr 2011: July. 23,. 200. 9 w. ww. sci. ence. mag. org. Dow. ... ER. /MIT. Published by AAAS. on. July. 23,. 200. 9 w.

1 Sep 2011: Woo J. Fluid Mech. vol. 86, 1978, pp. 179-200. We regret overlooking the fact that the first use of the result (2.12) for the numbers of surface saddle and

5 Aug 2011: 2140 E. W. Wolff. –440. –410. –380. 0 200 400 600 800age (EDC3 kyr BP). ... 200 ppbv) than in interglacials (up to 280 ppbv) [53], although therecord is patchy because artefacts do occur that make the records in some sectionsof ice unreliable.

10 Apr 2011: 6b reveals a peak of 800 ms for acolony of radius 200 m. ... Movies acquired with ananalog charge-coupled device camera (SSC-M374, Sony; 480 640 pixels) consisted of 1,000 images taken at 30 frames pers, averaged over 200 frames.

10 Apr 2011: Scales are 200 m. (d) Alinear Volvox cluster viewed from above (scale is 1 mm).

10 Apr 2011: Scale bar: 200 μm.). Fig. S3. Photoresponse of V. carteri as a function of stimulus frequency.

10 Apr 2011: 200 M. Lombardi, C. P. Caulfield, C. Cossu, A. I. Pesci and R. ... Results for Rein = 0.05, Sc = 667 andGr = 49.05 for (a) the base flow and τ = (b) 133.67, (c) 200.33 and (d ) 250.33.

10 Apr 2011: 12 bit digital CCD cameras(Hamamatsu C7300) with 80 – 200 mm f=2:8 lenses acquireimages to a personal computer.

10 Apr 2011: Typical f luid velocities atthe free surface are in the range of 20 –200 ms, acceleratingas the meniscus slope increases near the contact line. ... Experimental observations and numerical results presentedare as described for Fig. 2, with A and A at

10 Apr 2011: relative Volvox carteri [18], aspherical alga (R 200 m) which swims by the action of103 Chlamydomonas-like cells on its surface.

1 Sep 2011: For g! = R M! this provides100) g! 2 Wk1[0;1]200) g! = (

10 Apr 2011: c) Boundary layer scale near IZþ vs time forPe 0, 10, 50, 200, 103, 5 103, 2 104.

10 Apr 2011: cm. Hence, 80 cm3 or 200 g of CaCO3 isadded per century.

10 Apr 2011: K. U. L e u u e n , Celestijnenlaan. 200 F , B-3030 Heverlee, B e l g i u m.

10 Apr 2011: R 200–400 m) there is the striking con-clusion that R; the Stokeslet dominates the flow field.It was therefore suggested [5] that suspensions of Volvoxwould be more similar to

10 Apr 2011: a Chlamydomonas reinhardtii scale bar of 5 m and b Vol-vox carteri scale bar of 200 m. ... The imageswere taken at 2 magnification. The scale bar is 200 m.

10 Apr 2011: 1976) Nature 259, 200 –201.24. Acrivos, A. & Taylor, T. D.

10 Apr 2011: n A, with M = 1. j It) tiJ: e/eB et/eB A A 200 1 0.15 -4.2 B B 200 1 0.15 -7.2 A B 200

10 Apr 2011: A similar single-photon-induced ionization of ice has been anticipated but several attempts to observe this phenomenon in pure ice a t wavelengths greater than 200 nm have been u

10 Apr 2011: Phys Fluids15:568–578. 18. Nitsche M, Steen PH (2004) Numerical simulations of inviscid capillary pinchoff.J Comput Phys 200:299–324.

10 Apr 2011: Theory of multiple phase separations in binary mixtures: Phase diagrams, thermodynamic properties, and comparisons with experiments. Raymond E. Goldstein. Departments 0/ Chemistry and Physics, Massachusetts Institute 0/ Technology, Cambridge,

10 Apr 2011: We can imagine the elongation in atime to correspond to the addition of a disk at the attach-ment point, so R2 80 cm3 or 200 g of CaCO3 or80 g ... FIG. 6. Growth velocity c vs pH, using CO2 partial pressure in the cave of3 104 atm, a temperature of 20 C,

10 Apr 2011: As such, caution in certain areas is. 200. 150. o 1= r 100. ... Data is from Ref. 19. 0. 500. ---,--"T""-r----T-.,.-T"".,;--,--,.--. 400. 300. 200.

6 Jul 2011: grownfor 7 h on a rotary shaker (200 rpm) at 33 C.

13 Apr 2011: 9. been sent by e-mail to about 200 people. The objective function is specified bya subroutine, provided by the user, that calculates F(x) for any x in Rn thatsatisfies ... 103.92 32.86 / 32.21160 34.62499 / 26.13208 436.25 / 352.69 200.73 / 173.07.

27 Nov 2011: CDa)a-C/) -200. -400. -600. -800. -40 -20 0 20 40. Applied torque (%). FIGURE 9 Speed as a function of applied torque for two cells brokenprogressively. ... 0 a. o. 0. 100. NI4-a)0-oa)a). Cn. -200 -100 0 100 200 300.

10 Apr 2011: Reiso-lation of B. burgdorferi from the flaB inoculated mice tissuesalso failed even when the animals received 200 times the ID50(M.

10 Apr 2011: For hydrogen thistransition occurs atR;c/10 eV;a0 /a;200 A. For dis-tances comparable to or greater than this value, we mustretardation into account.

3 Dec 2011: 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

24 Aug 2011: Scale bar, 200 mm. Volvocalean algae: phenotypic plasticity C. A. Solari et al.

22 Nov 2011: 20 trials) (middle)and f fN1,N2,m2,t (avg. 20 trials) (bottom), where N = N2 = 1001,m = 370, N1 = 170, m2 = 200.

10 Apr 2011: with a sloping upper surface, varying in thickness from. ‘‘zero’’ to 200 lm.

10 Apr 2011: Scale bar, 200 mm. Volvocalean algae: phenotypic plasticity C. A. Solari et al.

2 Nov 2011: Generalized sampling and infinite-dimensionalcompressed sensing. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd,

27 Nov 2011: 200). Coarser fluctuations, probably associated with variations in the number ofactive torque-generating units, have been studied by Kara-Ivanov et al. ... At 23C, the torque exertedby the motor is approximately constant, all the way from negative speeds

20 Jun 2011: grownfor 7 h on a rotary shaker (200 rpm) at 33 C.

10 Oct 2011: PART I: Symmetries and particles. NOTES BY PROF. HUGH OSBORN. Books. Books developing group theory by physicists from the perspective of particle physics are. H. F. Jones, Groups, Representations and Physics, 2nd ed., IOP Publishing (1998).A fairly

26 Jan 2011: Extreme Ultraviolet Spectroscopyof the Solar Corona. Giulio Del Zanna. A thesis submitted inpartial fulfilment. of the requirementsfor the degree of. Doctor of Philosophy. Centre for AstrophysicsUniversity of Central Lancashire. July 1999. Abstract.

14 Jul 2011: Fundamentals of Atmosphere–OceanDynamics. M. E. McIntyre. LATEX version edited by. Björn Haßler. and. Christophe Koudella. with the kind assistance of. Teresa Cronin. and. Sarah Shea–Simonds. Version of 2007–8. ii Part , 0.0. Author’s