![8.7 Summary Just as Chap. 4 was initiated with the representation of an irrotational vector field E, this chapter began by focusing on the solenoidal character of the magnetic flux density. Thus, o H was portrayed as the curl of another vector, the vector ... 8.7 Summary Just as Chap. 4 was initiated with the representation of an irrotational vector field E, this chapter began by focusing on the solenoidal character of the magnetic flux density. Thus, o H was portrayed as the curl of another vector, the vector ...](https://web.mit.edu/6.013_book/www/chapter8/ch8-t871.gif)
8.7 Summary Just as Chap. 4 was initiated with the representation of an irrotational vector field E, this chapter began by focusing on the solenoidal character of the magnetic flux density. Thus, o H was portrayed as the curl of another vector, the vector ...
![Magnetic vector potential of a rotating uniformly charged shell. – M Dash Foundation: C Cube Learning Magnetic vector potential of a rotating uniformly charged shell. – M Dash Foundation: C Cube Learning](https://infyinfo.files.wordpress.com/2019/07/rotatingshell-page1-1.jpg)
Magnetic vector potential of a rotating uniformly charged shell. – M Dash Foundation: C Cube Learning
![8.7 Summary Just as Chap. 4 was initiated with the representation of an irrotational vector field E, this chapter began by focusing on the solenoidal character of the magnetic flux density. Thus, o H was portrayed as the curl of another vector, the vector ... 8.7 Summary Just as Chap. 4 was initiated with the representation of an irrotational vector field E, this chapter began by focusing on the solenoidal character of the magnetic flux density. Thus, o H was portrayed as the curl of another vector, the vector ...](https://web.mit.edu/6.013_book/www/chapter8/ch8-t872.gif)