Naked Science Forum
On the Lighter Side => New Theories => Topic started by: talanum1 on 02/05/2021 19:19:43

In the Superposition Integral for Electrodynamic Fields we have a position for the source (r) and a position for the observer (r'), Then the quantity: r  r' occurs in the denominator of the integrand.
What if the source is also the observer?

What if the source is also the observer?
I don’t see how that is possible