An Introduction to Thermal Physics
An Introduction to Thermal Physics
1st Edition
ISBN: 9780201380279
Author: Daniel V. Schroeder
Publisher: Addison Wesley
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Chapter 8.2, Problem 22P
To determine

The analogue of equation 8.50 , the magnetization of the system as a function of both the external field strength and the temperature and the sketch of the region in the TB plane for which the equation has three solutions.

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Consider a spring made of a superconducting material (electrical resistance very close to zero) containing N turns, radius R, natural length X0 and elastic constant k, as shown in the figure opposite. Somehow, an electric current I0 is passed through the spring. Calculate the spring length variation at the new equilibrium state. Tip: the magnetic flux over the spring must be constant at all times.
For Problem 8.16, how do I prove the relations and give the correct expressions?
Example 7.7. A uniform magnetic field B(1), pointing straight up, fills the shaded circular region of Fig. 7.25. If B is changing with time, what is the in- duced electric field? Solution E points in the circumferential direction, just like the magnetic field inside a long straight wire carrying a uniform current density. Draw an Amperian loop of radius s, and apply Faraday's law: do E-d1 = E(27s) = (s²B(1)) =-7S 2 dB di dt Therefore s dB E 2 dr If B is increasing, E runs clockwise, as viewed from above. 13 Magnetostatics holds only for time-independent currents, but there is no such restriction on 3B/ar. Chapter 7 Electrodynamics B(1) E Amperian loop FIGURE 7.25 dt Rotation direction dl λ FIGURE 7.26
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