Abstract
For symmetry reasons, the magnetic field is azimuthal and depends only on the radial coordinate r.
This is a preview of subscription content, log in via an institution.
Notes
- 1.
The present explanation of Feynman’s “paradox” is taken from J. Belcher and K. McDonald (http://cosmology.princeton.edu/~mcdonald/examples/feynman_cylinder.pdf) who further discuss subtle aspects of this problem.
Author information
Authors and Affiliations
Corresponding author
Rights and permissions
Copyright information
© 2017 Springer International Publishing AG
About this chapter
Cite this chapter
Macchi, A., Moruzzi, G., Pegoraro, F. (2017). Chapter S-8 Solutions for Chapter 8. In: Problems in Classical Electromagnetism. Springer, Cham. https://doi.org/10.1007/978-3-319-63133-2_21
Download citation
DOI: https://doi.org/10.1007/978-3-319-63133-2_21
Published:
Publisher Name: Springer, Cham
Print ISBN: 978-3-319-63132-5
Online ISBN: 978-3-319-63133-2
eBook Packages: Physics and AstronomyPhysics and Astronomy (R0)