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NATURAL SCIENCES TRIPOS Part II Wednesday 19 January 2011 ...
www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam11.pdf24 Jan 2011: xµ = (t, x) with x the two-dimensional position vector. Thedynamics of Aµ are determined by the ‘Maxwell-Chern-Simons’ Lagrangian. -
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www.tcm.phy.cam.ac.uk/~achc2/pt2thermo.pdf30 Apr 2011: 4. Use a Maxwell relation and the chain rule to show that for any substancethe rate of change of T with p in a reversible adiabatic compression is givenby. (. -
NATURAL SCIENCES TRIPOS Part II Wednesday 19 January 2011 ...
www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam11sol.pdf24 Jan 2011: 4 The ‘Maxwell-Chern-Simons’ Lagrangian is. LMCS = 1. 4FµνF. µν gϵµνλAµνAλ.
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