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13 Oct 2013: This paper was originally grabbed from the reading list of a course Prof. Kurose taught at UMass. Note: This essay was originally published in 1928 (long before computer networks were invented :-) ) and discussed size in the natural (biological)

18 Jan 2013: ii) MEG and EEG. A.S. Fokas, Y. Kurylev and V. Marinakis, The Unique Determination of the Neuronal Current in the Brain via Magnetoencephalography, Inverse Problems 20, 1067-1082 (2004). ... Rev. Lett. 96, 190201 (2006). A.S. Fokas, Nonlinear Fourier

5 Jun 2013: 15] [16] [17] File: PV_phillips_2.eps Graphic file (type eps) PV_phillips_2.eps [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] File: staircase-jets.eps

19 Oct 2013: I don't think it needs to be 20 years and it doesn't need to be 20 years for every country on this planet.

26 Jul 2013: We capture 2-second movies at 20 framesper second and measure the number of swimming cells bycounting cells swimming at speed faster than 1 body lengthper second. ... Fitting the measurements to our modelleads to L? 20–76 m. Since the cells swim

17 Nov 2013: On a good day, I could probably get through about 20% of them.

14 Mar 2013: 20 EMS Newsletter March 2013. Feature. Feature. EMS Newsletter March 2013 21.

20 Feb 2013: Averaged Lagrangian. John Hinch. February 20, 2013. Lagrangian formulation. Field equation, e.g.

19 Aug 2013: a. 1e-05. 0.0001. 0.001. 0.01. 0 5 10 15 20. t. ... FENE capillary squeezing. Filament breaks in with FENE L = 20.

26 Jul 2013: factors of 10, untilround off error sets in.) We have tested this algorithm up toN) 20 on the problem of packing circles on free spheres and havefound all of the known ... nondensest jammed packings were found belowN ) 10. ForN below 20, evenwhen

4 Oct 2013: 2P. x2. The assumed behaviour of the variance eq. (20) occurs commonly in actual physicalprocesses. ... λ)(6 λ)x4. 4! (λ)(6 λ)(20 λ)x6. 6! ],. Θ1 = a1.

4 Nov 2013: The measurements of k can be fitted by an ap-proximate scaling k Ra0:4, though the data also hint at apossible decrease in the exponent for Ra > 20 000 ... 20] Counts from a plume-tracking algorithm suggest a scalingexponent of 0:96 0:05 for the rib

4 Nov 2013: 20. 40. 60. 80. 100. 120. 1 2 3 4 5 6 7. ... E. Huppert, J. A. Neufeld and C. Strandkvist. 0 20 40 60 80 100.

5 Oct 2013: On the. 128 256 512 1024 2048 40960. 10. 20. 30.

19 Oct 2013: The boundary-layerequation then reduces to @6 T@r6 6 T 0 ; (5)in which the boundary-layer thickness is given by = 20 2iB20r2cN2L4! ... Astrophys. J.,(submitted)20. Dziembowski, W. A. & Goode, P. R. The toroidal magnetic eld inside the sun.Astrophys.

5 Oct 2013: 10. [6] R. Frank and C. Ueberhuber, Iterated Deferred Correction for Differential Equations,part 1, Computing, 20 (1978), 207-228. ... Comput. Phys., 189, 351–376, 2003. [15] B. Lindberg, Error Estimation and Iterative Improvement for Discretization

27 Aug 2013: The parameter space was divided upinto a 20 20 grid, and the full set of parameters was simulatedfor each of 50 different instances of random initial conditions.Combined with a linear ... The entire setof 20 20 parameters was simulated for 50 different

26 Jul 2013: r1. θ = πθ = 3π/4θ = π/2θ = π/4. 0 20 40 60 80 1000. ... Sci. Eng. 3, 16–21 (2001).20 S. Bohn, “Bubbles under stress,” Eur.

26 Jul 2013: σ 1 = 0, (20). u1 = 0, (21)where. σ 1 = p1I γ̇ 1! ... 2.5. 3. 3.5. 4. 20. 40. 60. 80. 100. 120. hRU.

5 Oct 2013: See [12, 20]. In a similar spirit, Driscoll & Fornberg introduced Padé-based method in[25]. ... 105. 20 40 60 80 100. 0.1. 0.2. 0.3. 20 40 60 80 100.

19 Oct 2013:  . 20. Snare drum. CHOIR. Piano. . . .      pp.

19 Oct 2013: 0. 2. 4. (a). 2 0 20. 0.5. 1. 1.5. 2. ... 2.5. 3. 3.5. 4. z. 0.2 0 0.20. 0.5. 1. 1.5.

26 Jul 2013: Slip length λeff 2–8 µm 20–90 nm 200–450 µm 1 µm 10–30 nm. ... Effective slip in pressure-driven Stokes flow 67. 010–20. 1. 2. 3.

26 Jul 2013: eled individually using slender body theory1,20 or singularity. methods.21 The second approach, to which this work. ... field (up to /(nmax)18–20 for thehighest values of Pe considered) and increase its resolution.

26 Jul 2013: Tetradecane 2138 3.5 nm (rms) 0 – 5 nm NLMica+.2 PPO Water 90110 2 nm (rms) 0 – 20 nm NL. ... Tetradecane – 2 nm (rms) 0 – 20 nm NLMicaOTE Water 110 0.2 nm (rms) 0 – 40 nm NL.

26 Jul 2013: Also, we observe that. aVxUy. aVLUxyMLVxx. aLk. 3 1; (20). so the timescale for reorientation of the bacteria perpendic-. ... 1=2 20 to 25mm/s; both set of values compare also favorably with pastexperimental results as described in the Introduction.

4 Nov 2013: H 20 m,motivated by the Sleipner site in the North sea [Bickle et al.,2007]. ... FCO2 DDCO2. HSh DCO2. kgD. 4=5 DH. 1=5. ’ 20 kg m2 yr1.

26 Jul 2013: 2un2 = EnKn1(r) FnKn1(r) BnrKn(r), (20)2vn1 = FnKn1(r) EnKn1(r). (21). The w component can be computed from u and v using thecontinuity equation, Eq. ... 15. 20. 0 0.5 189.5. 90. 90.5. 91. 100 101 102 103100.

26 Jul 2013: also well known that many biological cells actively modify or. maintain the shapes of their membranes,20,21 either for develop-. ... double-layer integral,. u(x) ð. S(t)q(y)$T(x,y)$n̂(y) dSy (20). where q(x) is an unknown density of the singular

26 Jul 2013: 1rn1. r(rn1Sn) rn1. r. Qn. rn1. 2 Wn. z= 0 (n 1), (3.20).

4 Nov 2013: φ+. x. x=0. φx. x=0. 4. 1 y2=. (23π. )1/2λ̄φ. 1/20. ... 3.20). Substituting the similarity solution for h from (3.16) and (3.15), we find that.

5 Oct 2013: 20 40 60 80 100 120 140. - 10. - 5.

27 Aug 2013: Phys Fluids 20(12):123304. 2. Woodhouse FG, Goldstein RE (2012) Spontaneous circulation of confined activesuspensions. ... 1. 2. 3. 4. 5. p. c. 1.000.20. 0.15. 0.10. 0.05.

26 Jul 2013: g(k) 2[1 cos(k) g log(k) kSi(k) Ci(k)], (20). and with the sine and cosine integrals dened by. ... Roman and J. Bico, J. Phys.: Condens. Matter, 2010, 22,493101. 20 S.

26 Jul 2013: F (ζ ) f (z(ζ )), G(ζ ) g(z(ζ )), (5.20). ... 0.20. 0.25. 0.30. 0.35. Ca. c. c = 8 Ca. Figure 6.

5 Oct 2013: See [12, 20]. In a similar spirit, Driscoll & Fornberg introduced Padé-based method in[25]. ... 105. 20 40 60 80 100. 0.1. 0.2. 0.3. 20 40 60 80 100.

4 Nov 2013: to store the energy sector’s emssions at current levels for the next 100 years [19, 20]. ... In this regeneration stage,between 13 and 20% of the power output of the plant can be lost.

2 Oct 2013: SIAM J. Sc. Comp., 20(1):33–61, 1998. 12. [9] I. Daubechies. Ten Lectures on Wavelets, volume 61.

4 Nov 2013: 0.5, 2, 5, 20.5 and 52. ... t. 1.0. 0.8. 0.6. 0.4. 0.2. 0 10 20 30 40.

4 Nov 2013: Equation (2.15) is subject to the non-dimensional boundary conditions[HH. X. ]. 0. = αT α1, (2.19). [HH. X. ]. XN. = 0, (2.20). ... short-dashed line), 20(dash–dotted line), 25 (long-dashed line) and 30 (dashed–dotted–dotted line).

26 Jul 2013: ESliding t =G. 2. 0. L. 2ds. 20. As with the bending Eq. ... Even though the hydrodynamic efficiencyonly decays 13% from the optimal sawtoothed solution, theswimming speed decreases by approximately 20%.

4 Nov 2013: w1. = k2RmΠ1(φ)θ1. (4.20). The boundary conditions can be similarly transformed. ... 348 J. A. Neufeld and J. S. Wettlaufer. 0 5 10 15 20 25 30.

26 Jul 2013: The main features of this problem have been successfullyexploited experimentally to measure the bending modulus ofbiopolymers actin filaments and microtubules, either usingthermal fluctuations 20 or using an active actuation ... Optimal III 0.24 3.34

14 Aug 2013: Received: 24 April 2012 / Accepted: 20 November 2012Published online: 21 May 2013 – Springer-Verlag Berlin Heidelberg 2013. ... The existence of the Lax pair for an arbitrary conformal structurewith vanishing self-dual Weyl curvature has the following

19 Oct 2013: 20. Eliminate U2:. 12g(h21 h. 22) = h2. V (h2 h1).

19 Oct 2013: perhaps 20 days or more) ozone concentrations in Europe, for example, are. ... 9in x 6in lecturenotes˙190410. 20 P. H. Haynes. Fig. 3. Reproduced from [13].

5 Oct 2013: 20 40 60 80 100 120 140. - 10. - 5.

4 Nov 2013: χ 1 ζ /ζ0, (3.10)and letting. ϕ(χ) H 0 /ζ 20. ... 5 10 15 20 25 30 350. 0.2. 0.4. 0.6. 0.8.

7 Jan 2013: Scale bar: 20 μm.) (B) The mutant pusher mbo1 remains trapped for several seconds (Movie S6). ... 20. Rüffer U, Nultsch W (1991) Flagellar photoresponses of Chlamydomonas cells heldby micropipettes: II.

26 Jul 2013: R =8c/3. 02 1log 0 1. 0 1 20 19. see Ref. ... 19,we find the efficiency. E =20. 2 10 coth10 12. 0 02 1coth102.