The relevant equation listed above as
##\vec{E} \left( \vec{r} \right) = \frac{1}{4 \pi} \int {\nabla’ \times \frac{\partial \vec{B}}{\partial t}}\frac{1}{\left| \vec{r} - \vec{r}’ \right|}\, d \tau’##
Seems to me to be a natural consequence of the Helmholtz Theorem so I don’t see why it...