Find the velocity of the muon in Ex. 12.8.

Short Answer

Expert verified

The velocity of the muon isv=m2π-m2μm2π+m2μc.

Step by step solution

01

Expression for the conservation of momentum and conservation of energy:

Write the expression for the conservation of momentum.

pbefore=pafterpbefore=pμ+pμ

As the pion is at rest, the initial momentum will be zero. Hence, the above equation becomes,

role="math" localid="1654751319282" 0=pμ+pvpμ=-pv

Write the expression for the conservation of energy.

role="math" localid="1654751332433" Ebefore=Eaftermπc2=Eμ+Ev …… (1)

02

Determine the velocity of the muon:

Here, it is known that:

Ev=pccEv=pμc …… (2)

Using equation 12.54, write the value of pμ.

pμ=E2μ-m2μc4c

Substitute pμ=E2μ-m2μc4cfor pμin equation (2).

mπc2=Eμ+E2μ-m2μc4mπc2=E2μ+E2μ-m2μc4c2m2π+m2μ=2E2μEμ=m2π+m2μc22mπ

Write the formula for the Lorentz contraction.

y=11-v2c2(3)

Here, the value of yin terms of mπandmμis given as:

y=m2π+m2μ2mπmμ

Substitute m2π+m2μ2mπmμfor yin equation (3).

m2π+m2μ2mπmμ=11-v2c211-v2c2=1m2π+m2μ2mπmμ1-v2c2=4m2πm2μm2π+m2μ2v2c2=1-4m2πm2μm2π+m2μ2

On further solving,

role="math" localid="1654753313768" v2c2=m4πm4μ+2m2π+m2μ-4m2π+m2μm2π+m2μ2v2c2=m4πm4μ-2m2πm2μm2π+m2μ2v2c2=m2π-m2μ2m2π+m2μ2v=m2π-m2μm2π+m2μc

Therefore, the velocity of the muon isv=m2π-m2μm2π+m2μc.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

You may have noticed that the four-dimensional gradient operator /xμ functions like a covariant 4-vector—in fact, it is often writtenμ , for short. For instance, the continuity equation, μJμ=0, has the form of an invariant product of two vectors. The corresponding contravariant gradient would beμ/xμ . Prove thatμf is a (contravariant) 4-vector, ifϕ is a scalar function, by working out its transformation law, using the chain rule.

Inertial system S¯moves in the xdirection at speed 35crelative to systemS. (Thex¯axis slides long thexaxis, and the origins coincide at t=t¯=0, as usual.)

(a) On graph paper set up a Cartesian coordinate system with axesrole="math" localid="1658292305346" ct and x. Carefully draw in lines representingx¯=-3,-2,-1,0,1,2,and3. Also draw in the lines corresponding to ct¯=-3,-2,-1,0,1,2,, and3. Label your lines clearly.

(b) InS¯, a free particle is observed to travel from the point x¯=-2,at timect¯=-2to the point x¯=2, atct¯=+3. Indicate this displacement on your graph. From the slope of this line, determine the particle's speed in S.

(c) Use the velocity addition rule to determine the velocity in Salgebraically,and check that your answer is consistent with the graphical solution in (b).

You probably did Prob. 12.4 from the point of view of an observer on the ground. Now do it from the point of view of the police car, the outlaws, and the bullet. That is, fill in the gaps in the following table:

Speed of Relative to

Ground
Police
Outlaws
Bullet
Do they escape?
Ground
0role="math" localid="1654061605668" 12c
34c


Police



13c

Outlaws





Bullet





(a) Repeat Prob. 12.2 (a) using the (incorrect) definition p=mu, but with the (correct) Einstein velocity addition rule. Notice that if momentum (so defined) is conserved in S, it is not conserved inlocalid="1654750932476" S. Assume all motion is along the x axis.

(b) Now do the same using the correct definition,localid="1654750939709" p=mη . Notice that if momentum (so defined) is conserved in S, it is automatically also conserved inlocalid="1654750943454" S. [Hint: Use Eq. 12.43 to transform the proper velocity.] What must you assume about relativistic energy?

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?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free