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24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Meck. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 292 E. J.

5 Feb 2020: motor surface.22 Active rotational motion hasalso been studied for Janus motors with a coupling of electro-chemical forces to fluid flow23 or under an external field such asgravity,24 nonspherical ... dy:. (24). The integral in eqn (24) may be evaluated

27 May 2019: pRR. pTR. 24. 35. lR þlTe lRþlTð ÞtlR þ lT. lT lTe lRþlTð ÞtlR þ lT. ... Tt. :. (24). The MSD follows from a double integration in time of eqn (24),leading to the result.

13 Sep 2023: e2 2. )(t. time. Figure 24: The fixed space frame and the moving body frame. ... 2, 000 12 = 24, 000 years. The actual value of the precession is 25, 700 years.

30 Sep 2011: CR strain CC124 [12] was grown axenically in tris-acetate-phosphate medium [11] in a growth chamber(Binder, Germany) set to 24 C and a cycle of 16 h lightat 100 ... Nikaido, J. Cell Sci. 109, 57 (1996). [24] M. A. Silverman and M.

8 Nov 2017: I 1. 2ezez. ). (I ezez) = I, (24). and we further note that ξ/4πµ 1/ln(1/ϵa) [9]. ... Rev. Lett., 96 (2006). 058102.[24] Guirao B. and Joanny J. F., Biophys.

8 Sep 2020: 24) and βh = 1/2, and furthersubstituting into Eq. (50) gives access to the asymptotic solution for the swimming speed as(. ... 24]. When viewed as a run-reverse motionwith rotational diffusion, a change in the reversal rate modifies the mean path length

6 Jul 2020: In a given frequency range, this motionleads to a stable forward propulsive force.24,25 An example response,called the step-out profile, is illustrated in Fig. ... Mater. 24, 811–816 (2012). 7H. Ceylan et al., “Mobile microrobots for bioengineering

20 May 2024: Slide 23: Example: Verified spectra and modes. Slide 24: Example: Verified dictionary.

10 Apr 2011: An estimate of the hydrodynamic coupling between twoidealized flagella [24] is est ’ rRL. ... E.Goldstein, Science 325, 487 (2009). [24] T. Niedermayer, B. Eckhardt, and P.

19 Oct 2018: 14,24,26] The inner sur-face of the cone is chemically active and catalyzes a chemi cal reaction. ... Li, W. Gao, L. Zhang,. J. Wang, ACS Nano 2015, 9, 117.[24] M.

12 Aug 2016: Re2ν = 0. (24). The last equation is the ‘dual (or adjoint) linearized Navier-Stokes equation’. ... Step.3 Backwards time integrate the dual linearized Navier-Stokes equation (24) with in-compressibility (14) and boundary condition (13) from t = T

4 Nov 2019: J. Am. Chem. Soc. 2010; 132:14403. [24] Ghosh A. and Fischer P. ... 1992; 24: 313–58. [55] Purcell E. M. Life at low Reynolds number.

27 Feb 2013: Ann travels at a speed given. by β u/c = 24/25 in the x-direction for seven years and then comes back at the.

21 Feb 2017: 24 FEBRUARY 2017. 0031-9007=17=118(8)=088001(5) 088001-1 Published by the American Physical Society. ... 24 FEBRUARY 2017. 088001-3. freezing [Fig. 4(a)], a strong experimental signature of theformation of rotator phase next to the perimeter [3].

4 Aug 2015: pattern-ing the particle surface with active and passive sites (e.g. Janusparticles),23,24,28 (ii) spontaneous symmetry-breaking resultingfrom the advection of the field responsible for the phoreticresponse by ... K. Sia and G. M. Whitesides,

1 Oct 2016: The stresslet also controlsthe interactions of active organisms with their environment[21,22], enhanced transport through biological fluids[23,24], and the rheology of active fluids [25].If the stresslet of ... cζ dζ: ð26Þ. Using Eq. (24), the

18 May 2022: Rev. Fluid Mech. 24, 313–358 (1992). 8R. E. Goldstein, “Green algae as model organisms for biological fluid dynami-cs,” Annu. ... Miller, “Roles for motility in bacterial–host inter-actions,” Mol. Microbiol. 24, 1109–1117 (1997).

10 Apr 2011: 24 OCTOBER 2008. 178102-3. [Fig. 4(b)] is dominated by a 1= dependence, leading to avery strong 3 scaling as the amplitude of the streamfunction approaches zero. ... G. Bessoth, A. J. deMello, and A. Manz, Anal. Commun. 36, 213 (1999).[24] J.

2 Oct 2017: Rev. 35 415–24[8] Grant M A, Waclaw B, Allen R J and Cicuta P 2014 J. ... Rev. Lett. 109 168105[24] Ravnik M and Yeomans J M 2013 Phys.

8 Oct 2013: Camalet and F. Jülicher, New J. Phys. 2, 24 (2000).[21] Chlamydomonas Resource Center at the University of. ... Malasarn,Plant J. 66, 770 (2011). [24] 5 mM HEPES, 40 mM KCl, 10 mM CaCl2, pH 7.2.[25] K.

8 Jul 2021: B. Microsphere motion. The dynamics of a microsphere forced by an optical trap whose position is laterally oscillated isa well-studied problem [24]. ... Phys. 1, 28 (2018).[24] K. C. Neuman and S. M. Block, Optical trapping, Rev.

10 Feb 2010: y0, n = 0, 1, 2,. 24. The following four-stage Runge–Kutta method has order four,.

26 Jul 2013: 18 JULY 2008. 038102-2. wall-induced velocity is reminiscent of the shear-inducedmigration of deformable bodies and polymers away fromboundaries [21– 24], with the difference that, in thesecases, the dipoles ... Fluid Mech. 24,313 (1992). [20] J. R.

24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Meoh. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 470 H. A.

7 Jul 2022: Eng. Sci.,1976, 31, 901–911. 24 S. Engelnkemper, M. Wilczek, S. V. ... Tcholakova, M. Vethamuthuand A. Lips, Surfactant Mixtures for Control of Bubble SurfaceMobility in Foam Studies, Langmuir, 2008, 24, 9956–9961.

18 Nov 2022: mpEDMD: First convergent Galerkin method! 24/34. Numerical examples. 25/34. Lorenz system: scalar-valued spec measሶ𝑥1 = 10 𝑥2 𝑥1 , ሶ𝑥2 = 𝑥1 28 𝑥3 𝑥2, ሶ𝑥3 = 𝑥1𝑥2.

27 Apr 2024: 2.2.3 General Charge Distributions 20. 2.2.4 Field Lines 23. 2.2.5 Electrostatic Equilibrium 24.

26 Jul 2023: Slide 23: InfBeyn algorithm. Slide 24: Stability and convergence result. Slide 25: Proof sketch.

10 Apr 2011: The wires of [23, 24]are of finite length and attached to electrodes at either end. ... Our results may also be relevant to explain the observed stability of gold wires with largerradii [23, 24].

10 Apr 2011: This progression along the “devel-opmental path” [24] can work on a global scale to breakthe symmetry of circular waves, either by competition witha postulated third wave [19], tuning of the ... 24] A. Goldbeter and L. A. Segel, Differentiation 17,

6 Jul 2020: 24). For many ions in water atroom temperature, the diffusivity is approximately Ds 109 m2 /s [33]. ... 24), we can integrate eq. (59) directly to obtainthe following result for the non-reacting model:.

28 Jan 2014: Although the relative importance of chemical,hydrodynamic, and steric interactions for collective microbialmotion is still under debate [24,25], recent experiments [26]have shown that the different surface-scattering laws of ... 47] H. H. Wensink and H.

27 May 2019: 24 s. cba. fed. 0 10 20 40300. 0.2. 0.4. 0.6. ... The shaded area starting at time =24 s indicates the duration of motility-deactivation.

12 Aug 2016: û(x, t) = ũ(y)eikzσt (24). (known to be critical for the energy stability problem), (23) becomes. ... Rev. FluidMech., 43 (2011), pp. 1–24. [12] M. Nagata, Three-dimensional finite-amplitude solutions in plane Couette flow: bi-furcation from

3 Dec 2022: 2.2.3 General Charge Distributions 20. 2.2.4 Field Lines 23. 2.2.5 Electrostatic Equilibrium 24.

26 Jul 2013: on 24 November 2009rspa.royalsocietypublishing.orgDownloaded from. 108 O. S. Pak and E. ... s 1 ab s. s 11. )(e. s4y e2y)cos2x. (3.24). 4.

26 Jul 2013: Although suchcooperative effects have already been demonstrated forcoupled active but non-self-propelled particles in severaldifferent contexts 24–26, the generalization of our resultsto a large number of active particles remains ... Weinheim, Ger. 19,

14 Jun 2014: It would make a great text for a graduate course. Visual Neuroscience 2007!, 24, 763.

14 Nov 2019: Phys. J. E (2015) 38: 7. portant similarities with self-thermophoresis [24] or theself-propulsion of droplets through Marangoni effects, forwhich the slip velocity is replaced with a surface shearstress discontinuity ... 1 µ cosh τcosh τ µ eρ, (24).

26 Jul 2013: 24" as! 1 iDe1"!̃3!1"! 1 iDe2"#̃̇3! 1". =12. De2 De11 2iDe1. ... 32# 3#3 8#De1De2 3#3De1De2+ 24#De1. 2 4"! 20 3#2 12De12 8De1De2.

28 Sep 2009: Equations, 30 (4), (2007), 523–546.24 pages. ... 24. D. Stuart, “Perturbation theory for kinks”, Communications in Mathematical Physics,149 (1992), 433-462.

24 Jun 2013: 2Department of Physics, University of Arizona, Tucson, Arizona 85721, USA(Received 10 April 2013; published 24 June 2013). ... Stocker,Phys. Fluids 24, 091107 (2012). [28] W. R. DiLuzio, L. Turner, M.

4 Mar 2005: Further, show that if oneJacobi iteration is performed, thenu3,3 = 23/24 occurs, which is the estimate ofu( 12 ,.

6 Jan 2023: Can we do better? 24/36. 𝑚th order rational “smoothing” kernels:. 𝐾 𝑥 =1. ... Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24: Why study these foundations?

26 Jul 2013: also include an induced electrophoreticcomponent,24 proportional to their zeta potential and thestreaming electric field. ... Up(z) ) Uhydro(z) Uelec(z) UkBT (24). Uhydro(z) ) [1 - O(ad)]UPD(z)ex (25).

6 Oct 2016: i. |hi|2. where := cos(π/N) x F(N,C). 15 / 24. ... and the sos hierarchy needs only dN/4e levels. 24 / 24.

3 Dec 2022: 2. Zd3r0 r0 J(r0) (3.24). Just as in the electric case, the multipole expansion continues to higher terms. ... 3.24),. B(r) =µ04. 3(m1 r̂)r̂ m1. r3. (3.30). Now we’ll consider how this aects the second dipole m = m2.

26 Jul 2013: 061701-2 Michelin, Lauga, and Bartolo Phys. Fluids 25, 061701 (2013). by interfacial stresses arising from the self-generated gradients of reactive surfactants.21, 24, 25 Unlikeautophoretic Janus particles, which swim ... Mater. 24, 811–816 (2012).7 P.

19 Feb 2019: 2ψ̈ μ4 sin ψ. 1 μ cos ψ[. 24 32. ψ̇ 2 14. ... ε2 = 1 (1 D). (24)We therefore expand. ψ (σ ) = ε[ψ0 (σ ) εψ1 (σ ) ε2ψ2 (σ ) O. (