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  2. 13 Mar 2019: What. motivated your choice? [Suggestions: You could try ψ = cos(πx/2α) or ψ = (α2x2) for |x| < α and vanishingoutside this interval.]. ... 8. Consider the scaled Schrödinger equation. d2ψ. dx2+ λ cos 2xψ = Eψ.
  3. J. Fluid Mech. (2018), vol. 856, pp. 870–897. c© ...

    www.damtp.cam.ac.uk/user/drh39/2018_viscoslender.pdf
    1 Dec 2023: sin α) 2π(2 cos φ, sin φ)/ log Bi1 (see (3.2)). ... Ṽs =U cos(φΦ), ω̃=URH. sin(φΦ). (4.5a,b). Dow. nloa. ded. from. htt.
  4. J. Fluid Mech. (2023), vol. 963, A24, doi:10.1017/jfm.2023.336…

    www.damtp.cam.ac.uk/user/lauga/papers/216.pdf
    24 Jul 2023: Ω sed = mg16πa2η. ln(a. b. )(κ̃x sin θ κ̃y cos θ. ... sin θ, (3.40). Usedx = mg. 8πaηln(a. b. )cos θ sin θ, (3.41).
  5. 10 Oct 2017: 1 q cos p. ). 6. Show that the following transformation is canonical, for any constant, λ :. q1 = Q1 cos λ P2 sin λ , q2 = Q2 cos λ P1 sin λ ,. p1 = ... Q2 sin λ P1 cos λ , p2 = Q1 sin λ P2 cos λ.
  6. dynrel

    www.damtp.cam.ac.uk/user/tong/relativity/four.pdf
    3 Jul 2024: We then define the usual. polar coordinates. x = r cos , y = r sin. – ... l2(4.13). with A and 0 integration constants. (You might be tempted instead to write u =. A cos B sin k/l2 with A and B as integration constants.
  7. §3 IRROTATIONAL FLOWS, aka POTENTIAL FLOWS Irrotational flows are ...

    www.damtp.cam.ac.uk/user/mem/FLUIDS-IB/irrot-rot.pdf
    19 Oct 2013: expected. (ii) all A’s, B’s zero except A1:. φ = A1r cos θ = A1z , u = φ = A1ez. ... z. (iii) all A’s, B’s zero except B1:. φ =B1 cos θ.
  8. Cop yrig ht © 201 7 U nive rsity ...

    www.damtp.cam.ac.uk/user/examples/3R2c.pdf
    1 Nov 2017: 3ρ̄r. (b) Consider linear perturbations about the homogeneous solution. Show that the density. ... t = B (1 cos θ). where you should determine A, B and θ.
  9. J. Fluid Mech. (2020), vol. 882, A11. c© Cambridge ...

    www.damtp.cam.ac.uk/user/drh39/2020_squirm.pdf
    1 Dec 2023: the boundary condition to be imposed is. u=cos θ and τrθ =%Bi sgn(y) at r =1 (2.7a,b). ... balance. But FEAE′ =2FAE, where FAE =rEI Bi[2(πβ2) cos β2 sin β2] is the force on the section AE (see appendix B.1).
  10. Geometric transition in friction for flow over a bubble ...

    www.damtp.cam.ac.uk/user/lauga/papers/25.pdf
    26 Jul 2013: cosh cos ,. it is found that. θ. (a) (b) (c). ... cos cos cosh cos. 4 sin2. cosh cos 2 sin sin.
  11. 20 Jan 2009: Repeat the calculation in spherical geometry, i.e. for concentric spheres of radiir = a, b, b > a. ... For (iii), from a decent diagram of spherical polars, find k = er cos θ eθ sin θ. ].

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