Chapter 12: 53 (page 568)
Obtain the continuity equation (Eq. 12.126) directly from Maxwell’s equations (Eq. 12.127).
Short Answer
The continuity equation is obtained as .
Chapter 12: 53 (page 568)
Obtain the continuity equation (Eq. 12.126) directly from Maxwell’s equations (Eq. 12.127).
The continuity equation is obtained as .
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Get started for freeShow that the potential representation (Eq. 12.133) automatically satisfies [Suggestion: Use Prob. 12.54.]
A car is traveling along the line in S (Fig. 12.25), at (ordinary) speed .
(a) Find the components and of the (ordinary) velocity.
(b) Find the componentsrole="math" localid="1658247416805" and of the proper velocity.
(c) Find the zeroth component of the 4-velocity, .
System is moving in the x direction with (ordinary) speed , relative to S. By using the appropriate transformation laws:
(d) Find the (ordinary) velocity components and in .
(e) Find the proper velocity components and in .
(f) As a consistency check, verify that
“Derive” the Lorentz force law, as follows: Let chargeqbe at rest in, so , and let move with velocitywith respect to S. Use the transformation rules (Eqs. 12.67 and 12.109) to rewrite in terms of F, and in terms of E and B. From these, deduce the formula for F in terms of E and B.
Question: A stationary magnetic dipole, , is situated above an infinite uniform surface current, (Fig. 12.44).
(a) Find the torque on the dipole, using Eq. 6.1.
(b) Suppose that the surface current consists of a uniform surface charge , moving at velocity , so that , and the magnetic dipole consists of a uniform line charge , circulating at speed (same ) around a square loop of side I , as shown, so that .Examine the same configuration from the point of view of system, moving in the direction at speed . In , the surface charge is at rest, so it generates no magnetic field. Show that in this frame the current loop carries an electric dipole moment, and calculate the resulting torque, using Eq. 4.4.
Define proper acceleration in the obvious way:
(a) Findand α in terms of u and a (the ordinary acceleration).
(b) Expressin terms of u and a.
(c) Show that.
(d) Write the Minkowski version of Newton’s second law, in terms of. Evaluate the invariant product.
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