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20 Mar 2024: where Λµν satisfies. Λµσ ηστ Λντ = η. µν (1.24). For example, a rotation by θ about the x3-axis, and a boost by v < 1 along the x1-axis. ... The condition (1.24) for Λ to be a Lorentz transformation. becomes. (

31 May 2024: They solvedtheir lubrication equations (24)–(32), again by an expansion in a small Deborah numberWe 1, going to the first correction. ... p/. (1. c). p 1. De. H = 21/22. 23/24. Figure 1.

21 Mar 2024: Pedley and J. Kessler, Annu. Rev. Fluid Mech. 24, 313(1992). [16] B. ... 24] A. Creppy, F. Plouraboué, O. Praud, X. Druart, S. Cazin, H.Yu, and P.

3 Jun 2024: Mech. Phys. Solids 24 (1976) 225-238. 43. F. J. Sabina and J. ... Mech. Phys. Solids, 40. (1992) 1671-1681. 126. J. R. Willis, “Asymptotic analysis of crack bridging by ductile fibres”, Composites 24 (1993).

21 Mar 2024: orthogonal projection. 24. Convergence theoryKey ingredient: unitary discretization. 25. Spectral measures. ... Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

31 May 2024: 1 1. 2He. i!t. (5.24). where, as we mentioned previously, we should take the real part of the right-hand-side. ... S1(0)2 S2(0)2 = R2. The solutions (5.24) tell us how these geodesics evolve.

31 May 2024: should identify. g00(x) (1. 2Φ(x). c2. )(1.24). where Φ(x) is the Newtonian gravitational field. ... 1.24) but with a linear gravitational potential Φ of the kind that we would invoke for.

18 Jun 2024: 𝑒𝑗 𝑒𝑗1. 𝑈 =. Back to the shift! ෍. 24. 0 1. ... Slide 24: Back to the shift! Slide 25: Back to the shift!

6 Apr 2024: Slide 23: Convergence of measures. Slide 24: Further convergence. Slide 25: Lorenz system.

31 May 2024: should identify. g00(x) 1. 2(x). c2. (1.24). where (x) is the Newtonian gravitational field. ... 1.24) but with a linear gravitational potential of the kind that we would invoke for.