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Show that it is possible to outrun a light ray, if you're given a sufficient head start, and your feet generate a constant force.

Short Answer

Expert verified

It is possible to outrun a light ray.

Step by step solution

01

Write the given data from the question.

The force generated by the force is constant.

The initial velocity is constant.

02

Show that it is possible to outrun a light ray.

The expression for position as function of time, with the initial velocity is zero and generated force is constant is given as follows.

x(t)=mc2F[1+(ftmc)2-1]+v0t

Here,m is the mass,c is the speed of the light,F is the generated force,v0 is the initial force andt is the time.

The expression for the position of the photon is given by,

xp(t)=ct

The time-position graph is shown below.

From the above graph, the photon which starts fromt<0 ca easily catches the person in the hyperbolic motion but the photon which starts fromt>0 would not be able to catch up the person in hyperbolic motion.

Therefore, the outrun is possible.

Hence it is possible to outrun a light ray.

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Most popular questions from this chapter

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

Kradฮผ=ฮผ0q26ฮ cdฮฑฮผdb

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

(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.

An electric dipole consists of two point charges(ยฑq), each of massm, fixed to the ends of a (massless) rod of lengthd. (Donotassumedis small.)

(a) Find the net self-force on the dipole when it undergoes hyperbolic motion (Eq. 12.61) along a line perpendicular to its axis. [Hint:Start by appropriately modifying Eq. 11.90.]

x(t)=Fmt'1+(Ft'mc)2dt'=mc2F1+(Ft'mc)2|0t=mc2F1+(Ftmc)2โˆ’1...(12.61)

Fself=q2(E1+E2)=q28ฯ€ฮต0c2(lc2โˆ’ad2)(l2+d2)3/2x^...(11.90)

(b) Notice that this self-force is constant (t drops out), and points in the direction of motionโ€”just right to produce hyperbolic motion. Thus it is possible for the dipole to undergo self-sustaining accelerated motion with no external force at all !! [Where do you suppose the energy comes from?] Determine the self-sustaining force, F, in terms of m, q, and d.

(a) Construct a tensor Dฮผฯ…(analogous to Fฮผฯ…) out of Dand H. Use it to express Maxwell's equations inside matter in terms of the free current density Jfฮผ.

(b) Construct the dual tensor Hฮผฯ…(analogous to Gฮผฯ…)

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

Dฮผฯ…ฮทฯ…=c2ฮตFฮผฯ…ฮทฯ… andHฮผฯ…ฮทฯ…=1ฮผGฮผฯ…ฮทฯ…

Where ฮตis the proper permittivity, ฮผis the proper permeability, andฮทฯ… 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.

Show that the (ordinary) acceleration of a particle of mass m and charge q, moving at velocity u under the influence of electromagnetic fields E and B, is given by

a=qm1โ€u2/c2[E+uร—B-1c2uuโ€E]

[Hint: Use Eq. 12.74.]

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