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1 Classical Field Theory‣ Quantum Field Theory by David Tong
www.damtp.cam.ac.uk/user/tong/qft/qfthtml/S1.html18 Oct 2021: To see that Maxwell’s equations indeed follow from (1.20), we compute. (. ... x. ). You can check that Maxwell’s Lagrangian (1.23) is indeed invariant. -
2 Classical Gases‣ Statistical Physics by David Tong
www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S2.html18 Oct 2021: N. (2.63). which gives us back the ideal gas law. 2.3 Maxwell Distribution. ... 3. /. 2. This is the Maxwell distribution. It is sometimes called the Maxwell-Boltzmann distribution. -
6 Quantum Electrodynamics‣ Quantum Field Theory by David Tong
www.damtp.cam.ac.uk/user/tong/qft/qfthtml/S6.html18 Oct 2021: 6.1 Maxwell’s Equations. The Lagrangian for Maxwell’s equations in the absence of any sources is simply. =. -. ... 6.571). In Coulomb gauge we can rewrite the Maxwell part of the Lagrangian as. -
0 Introduction‣ General Relativity by David Tong
www.damtp.cam.ac.uk/user/tong/gr/grhtml/S0.html16 Oct 2021: It’s worth pausing to see why this analogy does not continue when objects move and the resulting Einstein equations of general relativity are considerably more complicated than the Maxwell equations ... Indeed, in the full Maxwell equations. ρ. e. -
3 Introducing Riemannian Geometry‣ General Relativity by David Tong
www.damtp.cam.ac.uk/user/tong/gr/grhtml/S3.html16 Oct 2021: 3.2.5 The Maxwell Action. Let’s briefly turn to some physics. We take the manifold. ... F. μ. ν. F. μ. ν. This is the Maxwell action, now generalised to a curved spacetime. -
0 Introduction‣ Quantum Field Theory by David Tong
www.damtp.cam.ac.uk/user/tong/qft/qfthtml/S0.html18 Oct 2021: But why then didn’t Faraday, Maxwell and other classical physicists find it useful to introduce the concept of matter fields, analogous to the electromagnetic field? ... The field theories of Maxwell and Einstein remedy the situation, with all -
5 When Gravity is Weak‣ General Relativity by David Tong
www.damtp.cam.ac.uk/user/tong/gr/grhtml/S5.html16 Oct 2021: μ. and. ν. , nor gauge invariant. That’s not such a surprise as it’s also true for Maxwell theory. ... In Maxwell theory, such a term can be added to make the resulting energy-momentum tensor both symmetric and gauge invariant. -
6 Black Holes‣ General Relativity by David Tong
www.damtp.cam.ac.uk/user/tong/gr/grhtml/S6.html16 Oct 2021: K. obeys something very similar to the Maxwell equations,. d. F. =. ... 0. But these are the vacuum Maxwell equations in the absence of any current, so we would expect any “electric charge” to vanish. -
4 Classical Thermodynamics‣ Statistical Physics by David Tong
www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S4.html18 Oct 2021: 4 Classical Thermodynamics. 4 Classical Thermodynamics. “Thermodynamics is a funny subject. The first time you go through it, you don’t understand it at all. The second time you go through it, you think you understand it, except for one or two -
Remarks on the Mathematical Classification of Physical Quantities,
www.damtp.cam.ac.uk/user/tong/vc/maxwell.pdf10 Dec 2021: CLERK-MAXWELL, LL.D., F.R.S. The first part of the growth of a physical science consists in the dis-covery of a system of quantities on which its phenomena ... Rankine and Clerk-Maxwell. Prof. Henrici and Mr.Merrifield, in their remarks on the -
4 The Einstein Equations‣ General Relativity by David Tong
www.damtp.cam.ac.uk/user/tong/gr/grhtml/S4.html16 Oct 2021: Such diffeomorphisms are analogous to the gauge symmetries that are familiar in Maxwell and Yang-Mills theory. -
latestcv
www.damtp.cam.ac.uk/user/mrep/latestcv.pdf8 Aug 2021: Teed (Glasgow) – Nonlinear shear dynamos Prof I. Eltayeb (Oman) – Maxwell-Cattaneo double diffusive convection Prof E.Dormy (ENS, Paris) – Optimizing flows for dynamos. -
3A1b.dvi
www.damtp.cam.ac.uk/user/examples/3A1b.pdf14 Jan 2021: b) Three effects neglected in a non-relativistic theory of MHD are (i) the displacementcurrent in Maxwell’s equations (compared to the electric current), (ii) the bulk electro-static force on -
B9s.dvi
www.damtp.cam.ac.uk/user/examples/B9s.pdf6 Oct 2021: 1862-4: Maxwell identifies light as an EM (electromagnetic) wave. • 1897: Thompson discovers the electron, the first elementary particle. • -
2 A First Look at Quantum Fields In this ...
www.damtp.cam.ac.uk/user/tong/pp/pp2.pdf7 Jun 2021: many centuries ago by Coulomb, Ampére, Faraday and Maxwell, albeit dressed by some. ... The equations, as written above, hide the full beauty of the Maxwell equations. -
1 Geodesics in Spacetime‣ General Relativity by David Tong
www.damtp.cam.ac.uk/user/tong/gr/grhtml/S1.html16 Oct 2021: For each of these, we need a set of equations. In the theory of electromagnetism, the swaying of the fields is governed by the Maxwell equations, while the motion of test ... It is similar to the gauge “symmetry” of Maxwell and Yang-Mills theory which -
Preprint typeset in JHEP style - HYPER VERSION Lent ...
www.damtp.cam.ac.uk/user/tong/aqm/justaqm.pdf25 Aug 2021: Preprint typeset in JHEP style - HYPER VERSION Lent Term, 2017. Applications of Quantum MechanicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical -
2 Introducing Differential Geometry‣ General Relativity by David Tong
www.damtp.cam.ac.uk/user/tong/gr/grhtml/S2.html16 Oct 2021: 2 Introducing Differential Geometry. 2 Introducing Differential Geometry. Gravity is geometry. To fully understand this statement, we will need more sophisticated tools and language to describe curved space and, ultimately, curved spacetime. This is -
Vol. 44 (2013) ACTA PHYSICA POLONICA B No 12 ...
www.damtp.cam.ac.uk/user/tong/talks/zakopane.pdf15 Apr 2021: We willnot turn on any other fields in the bulk, but all the results that we describebelow will hold for any bulk theory with an Einstein–Maxwell sector. ... The Maxwell equation is. (f(r)A′x. )′. w2. f(r)Ax =. A′0r2. L2. -
Field Theory in Cosmology (Part III) Enrico Pajer Contents ...
www.damtp.cam.ac.uk/user/ep551/field_theory_in_Cosmology.pdf15 Apr 2021: In Maxwell’s description of electromagnetic phe-nomena, we learn that the electric and magnetic fields are not just a crutch to computethe forces acting on changed particles.
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