thank you for the detailed analysis
If we start with the Lorenz gauge, we will eventually arrive at the same spot right?
interesting, that's kinda tricky
Don't worry, its been pretty useful to me for understanding electromagnetism. :)
I'd just like to see one more step.
Is it correct to...
I see, thanks, that makes sense.
I noticed that from (30) to (31), the curl operator applied to the fraction ends up being equivalent to applying it to the numerator only. Do you know why that's the case?