UFT346 Section 3

Many thanks, I recall the interesting graphics, and I will study it.

To: EMyrone@aol.com
Sent: 10/08/2017 13:25:22 GMT Daylight Time
Subj: Re: Interesting Graphics

The method is described in section 3 of UFT 346 with a dipole example.

Horst

Am 10.08.2017 um 14:17 schrieb EMyrone:

Do you have a reference for these graphics? Thanks in anticipation.

To: EMyrone
Sent: 10/08/2017 12:38:24 GMT Daylight Time
Subj: Re: Conservation of Antisymmetry by the Magnetic Dipole Field

good idea, I used the magnetic scalar potential for some graphics some time ago.

Horst

Am 10.08.2017 um 13:32 schrieb EMyrone:

This will be the last note for UFT385. I intend to use the Hodge dual of the field tensor and develop the little known magnetic scalar potential described by Jackson on page 180 into a new antisymmetry law. So the development can continue in exactly the same was as for the electric dipole field. The electric scalar potential is replaced by the much less well known magnetic scalar potential, and the new concept of electric vector potential is replaced by the well known magnetic vector potential. The Hodge dual of a two form is also a two form, so the Hodge dual field tensor is antisymmetric. There are many other ways of developing the problem of conservation of antisymmetry, but this is an elegant solution. The general problem is one of n equations in n unknowns.

Advertisements
  1. No trackbacks yet.

Leave a Reply

Fill in your details below or click an icon to log in:

WordPress.com Logo

You are commenting using your WordPress.com account. Log Out / Change )

Twitter picture

You are commenting using your Twitter account. Log Out / Change )

Facebook photo

You are commenting using your Facebook account. Log Out / Change )

Google+ photo

You are commenting using your Google+ account. Log Out / Change )

Connecting to %s

%d bloggers like this: