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8 Nov 2017: a r t i c l e’s s u r f a c e τ τ ζ θ ζ ξ ζ = C kA D/ ( ) ( , ) (1 ) /0.

6 Oct 2016: Hencethere exists xa 6= x(0), and e(0)a ,. ,e(T1)a with supp(e(t)a ) Ka that generate the same sequence y(0),. ... y(T1) of ob-served values, with in addition, |Ka| |K| q. We thereforehave two different initial conditions x(0) 6= xa and twodifferent

20 Oct 2019: eLife 7:e40018. DOI: https://doi.org/10.7554/eLife.40018,PMID: 30033910. Guasto JS, Johnson KA, Gollub JP. ... 2009. The Chlamydomonas Sourcebook. 2nd edition. London: Academic Press.Hinchliff CE, Smith SA, Allman JF, Burleigh JG, Chaudhary R, Coghill LM,

4 Jan 2024: Ex = ωA sin(nπy. a. ). sin(kz ωt). and. By = kA sin(nπy.

20 Apr 2024: automatically patched at x = a as well. We have. (x) cts at x = a ) B cos ka = Aea. ... plot the graph = k tan ka in blue, and then superpose this with the circle.

6 Feb 2019: 2αβ. f. Qαg. Qβ. 1. 2ij. f. qig. qj,. Isometries are generated by Killing potentials KA(Q+,q+,u) that obey the. ... conservation law” KA {KA,L(4)} = 0. L(4) =P(4)(Q+). (qu)2. P(4)(Q+) = 112.

23 Oct 2023: Indeed, withk = t, we have:. Euler: un1 = (I kA)un, ez = 1 z O(z2);Implicit Euler: un1 = (I kA)1un, ez = (1 z)1 O(z2);.

27 Jun 2024: Microwave Ionization of Hydrogen Atoms: Experiment versus Classical Dynamics. van Leeuwen KA, G Oppen, S Renwick, JB Bowlin, PM Koch, RV Jensen, O Rath, D Richards, JG Leopold. –

26 Jul 2013: FIG. 4. (Color online) Instantaneous velocity and pressure fields (left) and z component of the vorticity (right) for the in-plane beating oftwo flagella, with ka = kb = 0.05, R = 1, ... Bottom: Variation of the ratio of the minimum to themaximum of the

27 Jun 2024: KA James, PV Landshoff. – Physics Letters B. (1990). 251,. 167.