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1 Dec 2023: 23 TMP (West Fraser) 112 580 1.59 36.4. 24 TMP (West Fraser) 229 390 1.50 35.6. ... found in Reference 24. At least four trials for each pulp suspension were.

21 Oct 2020: z O(z 2);. TR: yn =[(. I 12 kA)1 (. I 12 kA)]n. ... 24 / 28. Splitting of inhomogeneous systems. Recall our goal, namely fast methods for the two-dimensionaldiffusion equation.

27 Jul 2007: K bb Ka = 12ηKa. Thus K is automatically geodesic, and if it is pure then its trajectories are parameterizedby an affine parameter.

26 Jun 2024: in (1.24) because E = (0,0,E) lies parallel to the side of the torus, not perpendicular. ... Instead, both (1.23) and (1.24) are best thought of as integrating the 2-form Fµν over.

7 Apr 2021: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... N =. 0. which should clearly be an integer. The quantisation (4.24) due to a background magnetic field.

4 Oct 2013: Xn(x) = Bn sinnπx. Lλn =. n2π2. L2. (24). Note that the first set eq. ... if ψ = 0at r = a then Rnk(a) = Jn(ka) = 0 so for each n, ka = kni with i = 1, 2,.

5 Sep 2012: 49) , and open 3D bulk suspensions (7, 18,24, 25), bacteria were confined in closed microfluidic chambers to. ... 6. Berg HC (1997) Motile behavior of bacteria. Phys Today 53:24–29.7.

10 Apr 2011: 3). vs T = - l/Ka• Recall that this expression refers to the formulation in Eq. ... SI=II-KI() • (24) With these results we can study some of the aspects.

5 Aug 2011: Although the strong correlationsuggests an almost constant and linear relationship, it actually appears as ifthe earliest part of the record (before about 650 ka) had lower mixing ratios(both absolutely and ... Science 309, 1714–1717.

5 Nov 2014: ψ1 = Re. [. n=1. ω. ka(n)NN(1 nky)e. nkyein(kxωt)]. (9). Notably, the flow described by eq. ... Sp = (ηω/κk3)1/3, which quantifies the dimensionlessratio of fluid to bending stresses [24].

23 Sep 2015: along the anterior (kA = 1000 μm, hA0 = 0:8) and strongly along the posterior-lateral cortex (kP = 150 μm, hP0 = 0, see ‘Materials and methods’ MT nucleation. ... the inset of panel C (yellow circles). In all panels, parameter values for anterior

4 Aug 2015: The problem is now completely specified bythree geometrical quantities, namely the non-dimensionalmean gap, H = kH, the corrugation amplitude, a = ka, andthe asymmetry parameter, g. ... K. Sia and G. M. Whitesides, Electrophoresis, 2003, 24,.

19 Jan 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J.

28 Sep 2009: respectively. These parameters ka and krare determined as the best fit parameters to the measurement. ... 24, pp. 273–285. 25J. Li, “Calcul d’interface affine par Morceaux piecewise linear interfacecalculation,” Acad.

18 May 2022: Niedermayer, B. Eckhardt, and P. Lenz, Chaos 18,. 037128 (2008).[24] D.

4 Oct 2013: n2π2 1. (24). On the other hand we had in a previous example the expression constructed from homo-geneous solutions:. ... Its FT is easy to calculate:. f̃(k) =. aaeikx dx =. aa. cos(kx) dx =2 sin(ka). k. (41). so by the Fourier inversion theorem we get.

10 Jan 2017: A linear functionon T given by κ = Ka(X)Ẋ a is called a first integral if dκ/dτ = 0 when (1.1) holds, or equivalently if. ... where ξa are local coordinates on the fibres of M, and 24 is the Ricci scalar.

12 Jul 2017: 25 and 38 have gas fractions 26–55%; the gratings in ref.24 have g '1 mm). ... Acc Chem Res 35:491–499. 44. Mori N, Chang KA (2003) Introduction to mpiv.

24 Jul 2023: δjk 12. dR̂jdŝ. dR̂kdŝ. )(ũk (R̂) ũk (ŝ). )dŝ,. (2.24). where R̂i = R̃i(ŝ). ... 3.1.1. Computation of forces and torquesUnder this parametrisation, (2.24) becomes. Ji = η̃s2. [

1 Oct 2016: hydrodynamics and flow sensing. Annu Rev Fluid Mech. (2016) 48:1–24. doi:. ... J Phys Chem. (1927) 31:1663–8. doi: 10.1021/j150281a004. 32. Adapa S, Dingeldein H, Schmidt KA, Herald TJ.