stunner5000pt
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Homework Statement
Griffith's problem 10.8
Show that retarded potentials satisfy the Lorentz condition. Hint proceed as follows
a) Show that
[tex]\nabla\cdot\left(\frac{J}{R}\right)=\frac{1}{R}\left(\nabla\cdot\vec{J}\right)+\frac{1}{R}\left(\nabla '\cdot\vec{J}\right)-\nabla '\cdot\left(\frac{J}{R}\right)[/tex]
b) Show that [tex]\nabla\cdot\vec{J}=-\frac{1}{c}\frac{\partial\vec{J}}{\partial t_{r}}\cdot(\nabla R)[/tex]
c) Note that [tex]\vec{J}=\vec{J}\left(\vec{r'},t_{r}\right)[/tex]
[tex]\nabla '\cdot J=-\frac{\partial \rho}{\partial t}-\frac{1}{c}\frac{\partial J}{\partial t_{r}}\cdot (\nabla ' R)[/tex]
where [tex]\vec{R}=\vec{r}-\vec{r'}[/tex]
2. The attempt at a solution
I managed to do the first and second parts but its the third part that i am unable to prove.
Ok so i know that [tex]\vec{J}=\vec{J}\left(\vec{r'},t_{r}\right)=\vec{J}\left(\vec{r'},t-\frac{\vec{r}-\vec{r'}}{c}\right)[/tex]
To make it simpler for me to understand let's do it for one dimension.
[tex]\frac{\partial J_{x}}{\partial x'} = \frac{\partial J_{x}}{\partial t_{r}}\frac{\partial t_{r}}{\partial x'}[/tex]
But [tex]\frac{\partial t_{r}}{\partial x'}=\frac{1}{c}\frac{\partial R}{\partial x'}[/tex]
so [tex]\frac{\partial J_{x}}{\partial x'} = \frac{1}{c}\frac{\partial J_{x}}{\partial t_{r}}\frac{\partial R}{\partial x'}[/tex]
THat explains the second term which i need to get in the proof. But how do i get the first term?
Also is it supposed to be [tex]\nabla\cdot J=-\frac{\partial \rho}{\partial t}[/tex]
or is it supposed to be [tex]\nabla'\cdot J=-\frac{\partial \rho}{\partial t}[/tex]
Thanks for your help!