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27 Jan 2015: But the importance of Maxwell's work was not obvious to his contemporaries. ... It took about thirty years after Maxwell before his equations were generally understood.

16 Jun 2015: 10) Einstein--Maxwell Gravitational Instantons.

22 Jul 2015: κ = 5 Maxwell κ = 3 Maxwell κ = 2 Maxwell T: 1.4x104 1x104 K T: 2x104 1x104 K T: 4x104 1x104 K Tail: 15% particles Tail: 25% particles Tail: 35% particles ... κ = 2 Maxwell T: 4x106 1x106 K Tail: 35 % particles 75 % energy.

12 Mar 2015: Show. that if the reflected fields are given by. Eref = E0x̂ ei(kzωt) , Bref =. E0cŷ ei(kzωt). then the total fields E = Einc Eref and B = Binc Bref satisfy the Maxwell ... with constant A0 and φ0. Use Maxwell’s equations to find a relationship

13 Jan 2015: 3.3. The correspondence between Maxwell’s equations and the discontinuity formulas is clear:. ... This is governed by Maxwell’s. equations without. tterms, so that we have.

13 Mar 2015: Verify that these are consistent with the remaining Maxwell. equations E = B = 0 and E B/t = 0.

23 Jul 2015: Disadvantage: do not use Newton and Maxwell rigorously • Need to develop ideas in (fully) 3D MHD : NOT Reduced MHD: Problems and limitations.

3 Feb 2015: Define the other functions of state by appropriate Legendre transformations,for example F = U TS and hence obtain the Maxwell relations:(.

26 Jan 2015: 5. From Maxwell’s equation νFµν = eψ̄γµψ,Fµν = µAν νAµ derive the required.

16 Jun 2015: and so? : Λ2(M) Λ2(M) is conformally invariant.Maxwell’s equations. dF = 0, d?