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  2. 5 When Gravity is Weak‣ General Relativity by David Tong

    www.damtp.cam.ac.uk/user/tong/gr/grhtml/S5.html
    16 Oct 2021: 5 When Gravity is Weak. 5 When Gravity is Weak. The elegance of the Einstein field equations ensures that they hold a special place in the hearts of many physicists. However, any fondness you may feel for these equations will be severely tested if
  3. 2 Classical Gases‣ Statistical Physics by David Tong

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S2.html
    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
  4. Form CHRIS/5: Application for Employment

    https://www.hr.admin.cam.ac.uk/files/chris5_v12_251021.rtf
    25 Oct 2021: CHRIS/5, Version 10, 24.04.18 University of Cambridge – Application for Employment Part 1, Page 2 of 7. ... CHRIS/5, Version 10, 24.04.18 University of Cambridge – CV Cover Sheet Part 3, Page 1.
  5. 1 Classical Field Theory‣ Quantum Field Theory by David Tong

    www.damtp.cam.ac.uk/user/tong/qft/qfthtml/S1.html
    18 Oct 2021: ϕ. (. y. ). (1.24). A priori, there’s no reason for this.
  6. 3 The Renormalisation Group‣ Statistical Field Theory by David Tong

    www.damtp.cam.ac.uk/user/tong/sft/sfthtml/S3.html
    16 Oct 2021: ζ. Δ. ϕ. ϕ. (. 𝐱. ). Figure 24: RG flows when.
  7. Oldroyd B, and not A? John Hincha, Oliver Harlenb,∗ ...

    www.damtp.cam.ac.uk/user/hinch/publications/Oldroyd12b.pdf
    25 Oct 2021: 24. I (Significance of limited free rotation for the viscosity and flow birefringence. ... J. Chem. Phys. 24, 269–. 278. [34] J.G. Kirkwood and J Riseman (1948) The Intrinsic Viscosities and Diffu-.
  8. Capillary-Induced Motion of Particles Bridging Interfaces of a…

    www.damtp.cam.ac.uk/user/hinch/publications/PhysRevLett.122.098001.pdf
    25 Oct 2021: a temperature of about 24 C (1 C), and a relativehumidity of 35% (2%). ... N. Manoharan, Nat. Mater. 11, 138 (2012).[24] M. Zanini, C. Marschelke, S.
  9. 4 Classical Thermodynamics‣ Statistical Physics by David Tong

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S4.html
    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. -.
  10. 5 Phase Transitions‣ Statistical Physics by David Tong

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S5.html
    18 Oct 2021: 5 Phase Transitions. 5 Phase Transitions. A phase transition is an abrupt, discontinuous change in the properties of a system. We’ve already seen one example of a phase transition in our discussion of Bose-Einstein condensation. In that case, we
  11. 3 Structure Formation‣ Cosmology by David Tong

    www.damtp.cam.ac.uk/user/tong/cosmo/cosmohtml/S3.html
    18 Oct 2021: 3 Structure Formation. 3 Structure Formation. Until now, we have discussed a universe which is perfectly homogeneous and isotropic. But that is not the universe we live in. Instead, our universe contains interesting objects which clump together,

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