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PHYS 832 Problem Set #3 Due: March 17, 2015 1. Jackson 12.2 b) Show explicitly that gauge transformation A α A α + α Λ of the potentials in the chargedparticle Lagrangian (for a charged particle moving in an external EM field) generates another equivalent Lagrangian. 2. Jackson 12.18 Prove, by means of the divergence theorem in four dimensions or otherwise, that for sourcefree electromagnetic fields confined to a finite region of space, the 3space integrals of Θ 00 and Θ 0i transform as the components of a constant 4vector, as implied by (12.106). T 00 d 3 x = 1 2 μ 0 E 2 + B 2 ( ) d 3 x = Energy field T 0i d 3 x = 1 μ 0 ! E × ! B ( ) i d 3 x = cP field i 3. Show that the 4vector form for the LiénardWiechert potential discussed in class can be written in more familiar form for a source point charge q at rs with velocity vs: φ ( ! r , t ) = 1 4πε 0 q (1 ! n ! β s ) ! r ! r s t r ! A( ! r , t ) = μ 0 c 4π q ! β s (1 ! n ! β s ) ! r ! r s t r where ! β s = v s (t ) c , and ! n = ! r ! r s ! r ! r s

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  • PHYS 832 Problem Set #3 Due: March 17, 2015

    1. Jackson 12.2 b) Show explicitly that gauge transformation A A + of the potentials in the charged-particle Lagrangian (for a charged particle moving in an external EM field) generates another equivalent Lagrangian.

    2. Jackson 12.18 Prove, by means of the divergence theorem in four dimensions or otherwise, that for source-free electromagnetic fields confined to a finite region of space, the 3-space integrals of 00 and 0i transform as the components of a constant 4-vector, as implied by (12.106).

    T 00d3x = 120

    E 2 + B2( ) d3x = Energyfield

    T 0id3x = 10

    !E

    !B( )i d3x = cPfieldi

    3. Show that the 4-vector form for the Linard-Wiechert potential discussed in

    class can be written in more familiar form for a source point charge q at rs with velocity vs:

    (!r, t) = 140

    q(1 !n

    !s )

    !r !rs

    tr!A(!r, t) = 0c

    4q!s

    (1 !n !s )

    !r !rs

    tr

    where!s =

    v s (t)c, and !n =

    !r !rs!r !rs