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21 - 30 of 54 search results for KaKaoTalk:ZA31 24 24 |u:www.damtp.cam.ac.uk where 0 match all words and 54 match some words.

  1. Results that match 2 of 3 words

  2. Koop_italy_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/Koopman_workshop_mjc.pdf
    20 May 2024: Slide 23: Example: Verified spectra and modes. Slide 24: Example: Verified dictionary.

  3. 4. The Einstein Equations It is now time to ...

    www.damtp.cam.ac.uk/user/tong/gr/four.pdf
    31 May 2024: ṙ2 Ve(r) = E2 (4.24). but this time with the eective potential. ... This tells us that the particle follows a null geodesic. The equation (4.24) gets replaced.

  4. 4 A Quantum Particle in Three Dimensions We will ...

    www.damtp.cam.ac.uk/user/tong/qm/qm4.pdf
    26 Jun 2024: 0 for all S(r) and R(r) (4.24). This is clearly satisfied if R and S are finite at the origin.

  5. Preprint typeset in JHEP style - HYPER VERSION 2018 ...

    www.damtp.cam.ac.uk/user/tong/gaugetheory/gt.pdf
    26 Jun 2024: in (1.24) because E = (0,0,E) lies parallel to the side of the torus, not perpendicular. ... Instead, both (1.23) and (1.24) are best thought of as integrating the 2-form Fµν over.

  6. PUBLICATION LIST -- J

    www.damtp.cam.ac.uk/user/tsm/jrw_publist1.pdf
    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).

  7. J. Fluid Mech. (2024), vol. 988, A10, doi:10.1017/jfm.2024.223 Flow…

    www.damtp.cam.ac.uk/user/hinch/publications/JFM988_A10.pdf
    10 Jun 2024: Received 10 October 2023; revised 27 December 2023; accepted 24 February 2024). ... F(Z, ζ ) = 13ζ. Z0. H(Z̃) dZ̃. (3.25). We note that solutions (3.24) satisfy the matching conditions between theinner and outer regions.

  8. Lent Term, 2015 ElectromagnetismUniversity of Cambridge Mathematical…

    www.damtp.cam.ac.uk/user/tong/em/electro.pdf
    27 Apr 2024: 2.2.3 General Charge Distributions 20. 2.2.4 Field Lines 23. 2.2.5 Electrostatic Equilibrium 24.

  9. 5. When Gravity is Weak The elegance of the ...

    www.damtp.cam.ac.uk/user/tong/gr/five.pdf
    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.

  10. standardmodel

    www.damtp.cam.ac.uk/user/tong/sm/standardmodel3.pdf
    26 Jun 2024: V (r) =g2s. 4rT AcaT? Adb. (3.24). – 99 –. We’ve still got those colour indices to deal with. ... the result (3.24).) Consider the operator. SA = T A(R1) 1 1 T A(R2).

  11. italy_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/Italy_mpEDMD.pdf
    6 Apr 2024: Slide 23: Convergence of measures. Slide 24: Further convergence. Slide 25: Lorenz system.

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