Show that

kμkμ=θ(u2c2)cos21-u2c2

Whereθis the angle between u and F.

Short Answer

Expert verified

KμK°=F21-u2c2cos201-u2c2

It is proved that .

Step by step solution

01

Expression for the Minkowski force:

Using equation 12.69, write the expression for the Minkowski force.

KμKμ=(k0)+K·K …… (1)

Here,kis the ordinary force which is given by,

K·K=11-u2c2F·11-u2c2FK·K=F21-u2c2

02

Determine the zeroth component of K:

Write the zeroth component ofKusing equation 12.70.

K0=dp0dtK0=1cdEdT …… (2)

Here,Eis the energy which is given by,

E=mc2γE=mc21-u2c2

Substitute mc21-u2c2forEin equation (2).

…… (3)

K0=11-u2c2ddtmc21-u2c2K0=mc21-u2c2-12-11c21-u2c2322u·aK0=mcu·a1-u2c22

03

Prove that :

It is known that:

F-m1-u2c2a+uu·ac2-u2

Multiply byuon both sides in the above expression.

SubstituteuFcosθ, foru·Fin equation (3).

K0=mcuFcosθc1u2c2

Substitute mcuFcosθc1u2c2for K0and F21u2c2for K·Kin equation (1).

localid="1654669882880" KμKμ=-mcuFcosθc1u2c22+F21u2c2KμKμ=-u2F2cos2θc21u2c2+F21u2c2KμKμ=F21u2c21u2c2cos2θKμKμ=F21u2c2cos2θ1u2c2

KμKμ=F21u2c2cos2θ1u2c2

Therefore, it is proved that .

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Most popular questions from this chapter

Show that the Liénard-Wiechert potentials (Eqs. 10.46 and 10.47) can be expressed in relativistic notation as

(a) Event Ahappens at point ( role="math" localid="1658241385743" xA=5,yA=3,zA=0) and at time tA given by ctA=15; event Boccurs at role="math" localid="1658241462040" (10,8,0)and, ctB=5 both in systemS .

(i) What is the invariant interval between A and B?

(ii) Is there an inertial system in which they occur simultaneously? If so, find its velocity (magnitude and direction) relative to S.

(iii) Is there an inertial system in which they occur at the same point? If so, find its velocity relative to S.

(b) Repeat part (a) for A=(0,0,0), ct=1; and B=(5,0,0),ct=3 .

An electric dipole consists of two point charges(±q), 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)21...(12.61)

Fself=q2(E1+E2)=q28πε0c2(lc2ad2)(l2+d2)3/2x^...(11.90)

(b) Notice that this self-force is constant (t drops out), and points in the direction of motion—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) In Ex. 12.6 we found how velocities in thex direction transform when you go from Sto S. Derive the analogous formulas for velocities in the y and z directions.

(b) A spotlight is mounted on a boat so that its beam makes an angleθ with the deck (Fig. 12.20). If this boat is then set in motion at speedv, what angleθ does an individual photon trajectory make with the deck, according to an observer on the dock? What angle does the beam (illuminated, say, by a light fog) make? Compare Prob. 12.10.

Find the invariant product of the 4-velocity with itself, ημημ. Is localid="1654516875655" ημtimelike, spacelike, or lightlike?

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