Chapter 12: Q32P (page 541)
Find the velocity of the muon in Ex. 12.8.
Short Answer
The velocity of the muon is.
Chapter 12: Q32P (page 541)
Find the velocity of the muon in Ex. 12.8.
The velocity of the muon is.
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Get started for freeYou may have noticed that the four-dimensional gradient operator functions like a covariant 4-vector—in fact, it is often written , for short. For instance, the continuity equation, , has the form of an invariant product of two vectors. The corresponding contravariant gradient would be . Prove that is a (contravariant) 4-vector, if is a scalar function, by working out its transformation law, using the chain rule.
Inertial system moves in the direction at speed relative to system. (Theaxis slides long theaxis, and the origins coincide at , as usual.)
(a) On graph paper set up a Cartesian coordinate system with axesrole="math" localid="1658292305346" and . Carefully draw in lines representingand. Also draw in the lines corresponding to , and. Label your lines clearly.
(b) In, a free particle is observed to travel from the point at timeto the point at. Indicate this displacement on your graph. From the slope of this line, determine the particle's speed in .
(c) Use the velocity addition rule to determine the velocity in algebraically,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 | 0 | role="math" localid="1654061605668" | |||
Police | |||||
Outlaws | |||||
Bullet |
(a) Repeat Prob. 12.2 (a) using the (incorrect) definition , but with the (correct) Einstein velocity addition rule. Notice that if momentum (so defined) is conserved in S, it is not conserved inlocalid="1654750932476" . Assume all motion is along the x axis.
(b) Now do the same using the correct definition,localid="1654750939709" . Notice that if momentum (so defined) is conserved in S, it is automatically also conserved inlocalid="1654750943454" . [Hint: Use Eq. 12.43 to transform the proper velocity.] What must you assume about relativistic energy?
In system , a static uniform line charge coincides with thez axis.
(a) Write the electric field in Cartesian coordinates, for the point .
(b) Use Eq. 12.109 to find the electric in S, which moves with speedv in the x direction with respect to . The field is still in terms of ; express it instead in terms of the coordinates in S. Finally, write E in terms of the vector S from the present location of the wire and the angle between S and . 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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