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Recall that a covariant 4-vector is obtained from a contravariant one by changing the sign of the zeroth component. The same goes for tensors: When you “lower an index” to make it covariant, you change the sign if that index is zero. Compute the tensor invariants

FμvFμv,GμvGμvandFμvGμv

in terms of E and B. Compare Prob. 12.47.

Short Answer

Expert verified

The tensor invariants are FμvFμv=2B2-E2c2GμvGμv=2E2c2-B2andFμvGμv=-4cE.B

Step by step solution

01

Expression for the Product of  and :

Write the expression for the product of FμvFμv

FμvFμv=F00F00-F01F01-F02F02-F03F03-F10F10-F20F20-F30F30+F11F11+F12F12+F13F13+F21F21+F22F22+F23F23+F31F31+F32F32+F33F33Here,F00=0,F01=Exc,F02=Eyc,F03=Ezc,F12=Bz,F31=ByandF23=Bx .......(1)

Write the expression for the product of GμvGμv

GμvGμv=G00G00-G01G01-G02G02-G03G03-G10G10-G20G20-G30G30+G11G11+G12G12+G13G13+G21G21+G22G22+G23G23+G31G31+G32G32+G33G33Here,G00=0,G01,G12=Bz,G31=By,G23=Bx,Exc,G02=EycandG03=Ezc ......(2)

02

Determine the Product of :

Substitute F00=0,F01=Exc,F02=Eyc,F03=Ezc,F12=Bz,F31=ByandF23=Bxin equation (1).

FμvFμv=0-Exc2--Eyc2-Ezc2-Exc2-Eyc2-Ezc2+0+Bz2+By2+Bx2+0+Bz2+By2+Bx2+0FμvFμv=-2Ex2c2-2Ey2c2-2Ez2c2+2Bx2+2By2+2Bz2Here,Bx+By+Bz=BandEx+Ex+Ex=E

So, the above equation becomes,

FμνFμν=-2Ex2c2-2Ey2c2-2Ez2c2+2Bx2+2By2+2Bz2FμνFμν=-2c2Ex2+Ey2+Ez2+2Bx2+By2+Bz2FμνFμν=-2E2c2+2B2FμνFμν=2B2E2c2

03

Determine the Product of :

Substitute G00=0,G01=Bx,G01=By,G01=Bz,G12=EZc,G31=EycandG31=Excin equation (2).

GμνGμν=0-Bx2-Bx2-Bx2-Bx2-Bx2-Bx2+0+-Ezc2+-Eyc+-Ezc+0+-Exc+-Eyc+-Exc+0GμνGμν=-2Bx2-2Bx2-2Bx2+Ez2c2+Ey2c2+Ez2c2+Ex2c2+Ez2c2+Ex2c2GμνGμν=-2Bx2+By2+Bz2+2c2Ex2+Ey2+Ez2

On further solving,

GμνGμν=-2B2+2c2E2GμνGμν=2E2c2-B2

04

Determine the Product of :

Write the expression for the product of FμνFμν

role="math" localid="1654678337382" FμνFμν=-2F01G01+F02G02+F03G03+2F12G12+F13G13+F23G23

Substitute, role="math" localid="1654679206876" F01=Exc,F02=Eyc,F03=Ezc,F12=Bz,F31=BzandF23=Bx

G01=Bx,G02=By,G03=BzG12=-Ezc,G31=-EzcandG23=-Ezcin the above expression.

FμνFμν=2ExcBx+EycBx+EzcBx+2BzEzc+ByEyc+BxExcFμνFμν=-2cExBx+EyBy+EzBz-2cExBx+EyBy+EzBzFμνFμν=-2cE.B-2cE.BFμνFμν=-4cE.B

Therefore, the tensor invariants areFμνFμν=2B2-E2c2GμνGμν=2E2c2-B2andFμνGμν=4cE.B.

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Most popular questions from this chapter

A Lincoln Continental is twice as long as a VW Beetle, when they are at rest. As the Continental overtakes the VW, going through a speed trap, a (stationary) policeman observes that they both have the same length. The VW is going at half the speed of light. How fast is the Lincoln going? (Leave your answer as a multiple of c.)

The natural relativistic generalization of the Abraham-Lorentz formula (Eq. 11.80) would seem to be

Kradμ=μ0q26Πcdαμdb

This is certainly a 4-vector, and it reduces to the Abraham-Lorentz formula in the non-relativistic limitvc .

(a) Show, nevertheless, that this is not a possible Minkowski force.

(b) Find a correction term that, when added to the right side, removes the objection you raised in (a), without affecting the 4-vector character of the formula or its non-relativistic limit.

Show that the potential representation (Eq. 12.133) automatically satisfies [Suggestion: Use Prob. 12.54.]

(a) Draw a space-time diagram representing a game of catch (or a conversation) between two people at rest, apart. How is it possible for them to communicate, given that their separation is spacelike?

(b) There's an old limerick that runs as follows:

There once was a girl named Ms. Bright,

Who could travel much faster than light.

She departed one day,

The Einsteinian way,

And returned on the previous night.

What do you think? Even if she could travel faster than light, could she return before she set out? Could she arrive at some intermediate destination before she set out? Draw a space-time diagram representing this trip.

In system S0, a static uniform line chargeλ coincides with thez axis.

(a) Write the electric fieldE0 in Cartesian coordinates, for the point (x0,y0,z0).

(b) Use Eq. 12.109 to find the electric in S, which moves with speedv in the x direction with respect to S0. The field is still in terms of (x0,y0,z0); express it instead in terms of the coordinates(x,y,z) in S. Finally, write E in terms of the vector S from the present location of the wire and the angleθ between S and x^. Does the field point away from the instantaneous location of the wire, like the field of a uniformly moving point charge?

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