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8 Jul 2021: Cells interact with their surroundingsthrough complex hydrodynamic and steric interactions.21,22 Rigidboundaries, free surfaces and other obstacles in suspensions areknown to strongly affect swimming behaviour.23,24 Relevantcomplex media include

18 May 2021: 24 CHAPTER 2. GENERALISED SOLUTIONS. The representation (2.8) makes it clear again that the Moore-Penrose inverse is un-bounded if R(A) is infinite dimensional.

23 Apr 2021: Particle PhysicsCERN Lectures. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge, CB3 OBA, UK. http://www.damtp.cam.ac.uk/user/tong/particlephysics.html.

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2 Dec 2021: 2/x0 0 24 6/x4 2/x2.

18 Oct 2021: 2 Classical Gases. 2 Classical Gases. Our goal in this section is to use the techniques of statistical mechanics to describe the dynamics of the simplest system: a gas. This means a bunch of particles, flying around in a box. Although much of the

18 Oct 2021: 3 Quantum Gases. 3 Quantum Gases. In this section we will discuss situations where quantum effects are important. We’ll still restrict attention to gases — meaning a bunch of particles moving around and barely interacting — but one of the

16 Oct 2021: ζ. Δ. ϕ. ϕ. (. 𝐱. ). Figure 24: RG flows when.

26 May 2021: Demonstration of convergence. 24 THE BARRIERS OF DEEP LEARNING AND SMALE’S 18TH PROBLEM.

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23 Apr 2021: 1.2.2 The Scattering Amplitude 22. 1.2.3 Partial Waves 24. 1.2.4 The Optical Theorem 27. ... r(1.24). The 1/r fall-o follows from solving the free Schrödinger equation; we’ll see this ex-.

17 Jan 2021: We then changed the ciliated fraction areain the simulations by changing the distance between cilia in thedirection perpendicular to the beating (d=0.08, 0.16, 0.24,

7 Apr 2021: qg = 2πn with n Z (1.24). This is the famous Dirac quantisation condition. ... qg = 2πn with n Z. This, of course, is the Dirac quantisation condition (1.24).

8 Jul 2021: Received 13 May 2020; revised 18 February 2021; accepted 24 February 2021). ... Ω. , (2.23). where. A = 6ζ‖ 4Δζ (φ21 φ22 ) O(φ4), (2.24)B = 4Δζ (φ1 φ2) 83 Δζ (φ31 φ32 ) O(φ4), (2.25).

16 Apr 2021: D : (3 ττ ) kiki , (4.24)b K : (3 ττ ) 2biki b kkiki 2kikibjkj. ... R|comoving R =A. 2. (5.24). The metric then takes the form.

18 Oct 2021: Figure 24:. Expressing the work as. -. d. W. =. -. p. d. V. also allows us to underline the meaning of the new symbol. -.

22 Apr 2021: 23/82. 24/82. Hilbert’s question. Are all nonnegative polynomials sums of squares?

22 Feb 2021: A theory ofnon-Euclidean plates [23] has been developed in parallel.Apart from a general geometric theory of morphoelastic sur-faces [24], studies of morphoelastic shells have remained. ... 1 εκsζ 0 ζ0,ζ. (24). The elastic deformation gradient is,

20 Apr 2021: The quantities we are interested in are vortices. 24. 2 Vortices III Classical and Quantum Solitons.

8 Jul 2021: While recent numerical work reported that the elasticstresses in the wake of rigid cylinders depend on the orientation of the cylinder relative to its velocity[24], the dependence of the drag ... symmetry breaking, Phys. Fluids 24, 103102 (2012).[19] J. A