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24 Nov 2005: 5. Electromagnetic Waves In units where %0 = µ0 = c = 1 (‘Heaviside-Lorentz’) Maxwell’s equations are. ... E and B, and hence Maxwell’s equations, are invariant under gaugetransformations.

22 Mar 2005: Futter, C.E., Gibson, A., Allchin, E.H., Maxwell, S., Ruddock, L.J.,cells, 125I-EGF was internalized at 19.5C, as described in the perme-Odorizzi, G., Domingo, D., Trowbridge,

27 Sep 2005: Tu. 29 Nov. 2–3 Maxwell Lecture Theatre 3–5 TR1/2. Statistical MethodsBasic Module.

30 Sep 2005: Maxwell’s equations, B = 0, insists they never will be. Yet they have been arecurrent theme in high energy particle physics for the past 30 years!

6 Jul 2005: 6.1. Prediction of the neck propagation stress. In general, a Maxwell-type energy construction cannot be used to predict the applied load for the propagationof an instability, such as a

7 Nov 2005: PA RT IChancellor: H.R.H. The Prince PHILIP, Duke of Edinburgh, T. Vice-Chancellor: 2003, Prof. ALISON FETTES RICHARD, N, 2010Deputy Vice-Chancellors: for 2005–2006: Sir RICHARD DEARLOVE, PEM, GORDON JOHNSON, W, ANNE MARYLONSDALE, NH, The Rt Hon.

6 Jan 2005: J., Dodson, E. J., Maxwell, A.& Dodson, G. (1991). Crystal structure of an N-term-inal fragment of the DNA Gyrase B protein.

21 Jan 2005: Section H: Trust Funds 2003–04Permanent Capital. Opening Increase/ Closing Investedbalance Income (decrease) balance at1 August Additional capit- in value of 31 July 31 July. 2003 capital alised investments 2004 2004£ £ £ £ £ £.

27 Sep 2005: 11–1 Maxwell Lecture Theatre, Free SchoolLane. The rise of the Secret World: Governments andintelligence committees since c.1900 (Paper 7).

7 Nov 2005: PA RT I IM E M B E R S O F U N I V E R S I T Y B O D I E S. N O M I NAT I N G A N D A P P O I N T I N G B O D I E S : A B B R E V I AT I O N S. SPECIAL NO. 5] OFFICERS NUMBER–MICHAELMAS TERM 2005 55. C University CouncilCSAH Council of the School