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6 Jul 2020: Maximal stress at the surface Σ = 200 Pa within the range 80500 Pa from finiteelement computations. ... Perturbationsize ξ equals the organism size: 50 µm in diameter and 200 µm in length.

22 Jul 2014: 2001 109,900 70,900 83,700 157,200 130,500 552,200. 2010 119,800 80,900 94,200 165,300 145,200 605,400.

6 Jul 2020: a) Single helix with a diameter of 100 lm. (b) Single helix with adiameter of 200 lm. ... c) Single helix with a diameter of 200 lm and double the magnetic material of the spiral used in (b).

26 Oct 2020: Numerical Balancing Act: Magnetic Graphene. B. 0 200 400 600 800 1000. ... 0. 100. 200. 300. 400. 500. 600. 700. 800. 900. 1000.

14 Jul 2021: Numerical Balancing Act: Magnetic Graphene. B. 0 200 400 600 800 1000. ... 0. 100. 200. 300. 400. 500. 600. 700. 800. 900. 1000.

11 Mar 2024: 200. D.W.Hughes, J.Mason and M.R.E.Proctor. Mean Field responses in dispordered systems: andexample from nonlinear MHD.

4 Feb 2020: 0 50 100 150 200 250 300 The random surface was fairly jagged, with a subfractalX autocorrelation function of the form. ... To begin this solution an 0 50 100 150 200 250 300initial value is required either for T'(0) or for h(O) (or yiji).

19 Apr 2021: The Chinese (c. 200 BCE), buying& selling, taxes. Diophantus (c. 200-c.284)solution to 4 = 4x 20 is ‘absurd’!

13 Mar 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... 1. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.

13 Mar 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... 1. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.

1 Dec 2023: 19 BCTMP (Rayonier) 13 200 0.77 23.5. 20 BCTMP (Rayonier) 30 128 0.72 23.7. ... The fiber aspect ratios vary from about 50 to. 200 across the library.

13 Mar 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... 1. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.

24 Apr 2019: when n > 13.  For gas molecules in the room d/r 200 leads rapidly to chaos.

25 Jan 2007: 200. 4 U. nive. rsity. of C. ambr. idge. Not. to b. ... This is acorollary to Theorem 5.5.). Cop. yrig. ht. 200. 4 U.

12 Aug 2016: 200. 220. 240. 260. 280. 300. 320. 340. 0 50 100 150 200 25010-12. ... 10-5. 10-4. 10-3. 10-2. 10-1. 100. 0 50 100 150 200 250 300time (D/U).

26 Jun 2024: 4. Lattice Gauge Theory 200. 4.1 Scalar Fields on the Lattice 202.

3 Jun 2024: Martin and M. J. Simons, pp. 235-250. Kluwer, Dordrecht (2002). 200.

13 Mar 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... 1. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.

26 Nov 2017: converts garden waste to soil conditioner Saves 200,000 tonnes per year from landfill A Dutch company recover cellulose from used toilet paper, to add to tarmac.

25 Jan 2007: 200. 4 U. nive. rsity. of C. ambr. idge. Not. to b. ... viIN. TR. OD. UC. TIO. N. Cop. yrig. ht. 200. 4 U.

11 May 2024: Grade: Distinction.Ranked 3rd in year (out of > 200) and top in Department of Applied Mathematics and Theoretical Physics. •

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.

28 Jun 2024: Annals of Physics. (1990). 200,. 1. (doi: 10.1016/0003-4916(90)90241-f). Super p-branes as gauge theories of volume preserving diffeomorphisms.

13 May 2014: 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.

30 Sep 2008: Wave-particle duality. Light exhibits wave-like properties,. 3. Cop. yrig. ht. 200. ... dV. = 2|α|2N1 2|β|2N2 < ¤. 17. Cop. yrig. ht. 200.

22 Jul 2014: 150. 200. 250. 300. 350. 400. Essex Hertforshire Bedfordshire Cambridgeshire Norfolk Suffolk. ... 05/12/2012 Cambridge sub-region 2030 visioning - energy p.13. 0. 200. 400.

25 Jan 2007: λsin. q̃ q2. , (4.1.4). 16. Cop. yrig. ht. 200. 7 U. ... M1x i[σ3, M2] = QM1. (4.3.18). 21. Cop. yrig. ht. 200.

1 Dec 2023: b,c) Marginal stability curves (σ =0, outlines)and regions of instability (σ > 0, shaded areas), for R = 3 and (b) Pe = 25, 200, 500 and(c) Pe=15, 20, 25.

26 Jul 2013: 440. D.L. egen. dre,. E.L. auga. and. J.M. agnaudet. Kn = 0 Re = 5 20 50 100 200 500 800. ... 1000.0. 0 0.5 1.0 1.5 2.0 2.5. 47.5. Kn. Re. Re = 200.

18 Oct 2023: We use the geodesicicosahedron f3; 5þgð3;0Þ in standard notation [17], with 92total vertices, and take patches with N 58 to be repre-sentative of experimentally observed sizes (10–200

26 Jul 2013: In 1963,Rothschild measured the distribution of bull spermatozoaswimming between two glass plates (separation 200 m).The cell distribution was nonuniform, with a constantdensity in the center strongly increasing near the ... 48:3 15 m; when H 200 m,

10 Jun 2024: J. Fluid Mech. (2024), vol. 988, A10, doi:10.1017/jfm.2024.223. Flow of an Oldroyd-B fluid in a slowly varyingcontraction: theoretical results for arbitraryvalues of Deborah number in the ultra-dilutelimit. Evgeniy Boyko1,†, John Hinch2 and Howard

2 Jan 2024: CEOS DCOR probe corrector.The microscope was operated at 200 keV with a beam current of 80 pA. ... TheSTEM convergence angle used was 25.5 mrad with HAADF detector inner andouter collection angles of 50 and 200 mrad, respectively.

13 Sep 2023: theory took over 200 years to discover; and it’s not at all clear what the relationship is.

25 Jan 2007: 200. 2 U. nive. rsity. of C. ambr. idge. Not. to b. ... Suppose the surface charge to be18. Cop. yrig. ht. 200. 2 U.

1 Dec 2023: 2 m3 s1, and the total volume over the 200 sduration to 4.95 m3. ... The resultingtime constant D was 18,200 s for BH19c, 25,000 s for BH19e and23,000 s for BH19g(e).

13 Dec 2018: Israel J. Math. 50 (1985) 193-200. Department of Applied Mathematics. and Theoretical Physics.

14 Jun 2014: 50 200. 300 400. Figure3: Examplefinal networks usingdiffer-ent numbersof cells. Only the cell position isplottedfor clarity. ... Journal of Theoretical Biology,167:27–43,1994. [3] H. WässleandH. J. Riemann.Themosaicof nerve cells in the

4 Feb 2020: This is bound- ed by. 0.25. 0.20 -. 0.15 -. 0.05 -. -0.10 -. -0.15. I. I. I. I. I. 0 100 200 ]00 400 500 600.

4 Feb 2022: 50. 0. 50. 100. 150. 200. ν = 0.7. Re(z). Im(z. ). ... ν = 0.4. 0 200 400 600 800 1000. 10-15. 10-10.

17 Jul 2020: Sutcliffe),Physics Letters 342B (1995) 196-200. 51. Geometry of Defect Scattering, in Formation and Interactions of TopologicalDefects, NATO ASI Series B: Physics Vol.

15 Mar 2005: imposed vertical magnetic field Bz = (200)1/2. Units are such that Lx = Ly/4 = Lz = = ρ = µ0 = 1.

28 Feb 2024: 800. 600. 400. 200. 0. 20. t1 t2. Dis. tanc. eto.

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.

16 Jul 2018: a cell with flagellar filaments undergoing normal CCW rotation) with two different hook stiffnesses over a time scale t = 200 (time nondimensionalised by the rotation rate of the flagella). ... stiff hook. (A) Initial position and conformation of each

22 Jul 2014: IT Diploma level 2 and 3. • Apprenticeships 16-19. • Enrichment - students 14- 19 over the past 10 months have completed over 200 fully accredited MOS courses.

14 Jun 2014: 10. 100 200 300 400. cove. rage. number of cells. c=0.6. ... 200 sin 60= 30.4 µm). We also find that as the dendritic.

29 Nov 2021: 20 -10 0 10 20-20 -10 0 10 200. 10. 20. ... 100. 200(b) vorticity (1/s). -50. 0 2 4 6 8 10 120.

2 Nov 2021: 20 -10 0 10 20-20 -10 0 10 200. 10. 20. ... 100. 200(b) vorticity (1/s). -50. 0 2 4 6 8 10 120.

4 May 2017: 200 100 1.10 s 6.635e-06 0.88 s 2.767e-06400 200 3.38 s 2.662e-05 0.72 s 1.164e-05600 300 9.14 s ... 100 200 7.60 s 1.853e-06 2.69 s 3.769e-06200 200 7.47 s 2.441e-07 3.72 s 7.505e-07200 400 42.71 s