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Solve Eqs. 12.18 forx,y,z,tin terms ofx,y,z,t and check that you recover Eqs. 12.19.

Short Answer

Expert verified

The coordinates of the S frame in terms of coordinates in Sare found as:

x=γx+yty=yz=zt=γt+vc2x

Step by step solution

01

Expression for the Lorentz transformation equations:

Write the expression for the Lorentz transformation equations of coordinates x,y,zand tin Sframe.

First equation:

x=Y(x-vt) …… (1)

Second equation:

y=y

Third equation:

z=z

Fourth equation:

localid="1654594577273" t=Y(1-VXc2) …… (2)

02

Determine the coordinate of x in terms of x:

Rearrange the equation (2) in terms of t.

t=tγ+vxc2 ……. (3)

Substitute the value of equation (3) in equation (1).

x=γx-vtγ+vxc2x=γ×1-v2c2-vt

Rearrange the above expression in terms of x.

x=γx+vt …… (4)

03

Determine the coordinate of t in terms of t :

Substitute the value of equation (4) in equation (3).

t=γ1-vγx+vtc2t=γt-vc2xγ+vt

Rearrange the above expression in terms of t.

t=γt-vc2x

Therefore, the coordinates of the S frame in terms of coordinates in are found as:

x=γx+vty=yz=zt=γt+vc2x

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Most popular questions from this chapter

Why can’t the electric field in Fig 12.35 (b) have a, z component? After all, the magnetic field does.

Work out, and interpret physically, theμ=0 component of the electromagnetic force law, Eq. 12.128.

(a) Write out the matrix that describes a Galilean transformation (Eq. 12.12).

(b) Write out the matrix describing a Lorentz transformation along the yaxis.

(c) Find the matrix describing a Lorentz transformation with velocity v along the x axis followed by a Lorentz transformation with velocity valong they axis. Does it matter in what order the transformations are carried out?

(a) Construct a tensor Dμυ(analogous to Fμυ) out of Dand H. Use it to express Maxwell's equations inside matter in terms of the free current density Jfμ.

(b) Construct the dual tensor Hμυ(analogous to Gμυ)

(c) Minkowski proposed the relativistic constitutive relations for linear media:

Dμυηυ=c2ε¹óμυηυ andHμυηυ=1μGμυηυ

Where εis the proper permittivity, μis the proper permeability, andηυ is the 4-velocity of the material. Show that Minkowski's formulas reproduce Eqs. 4.32 and 6.31, when the material is at rest.

(d) Work out the formulas relating D and H to E and B for a medium moving with (ordinary) velocity u.

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 limitv≪c .

(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.

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