- #1
heyo12
- 6
- 0
a really hard one here. would appreciate help on how to do this question:
a physical system is governed by the following:
curl E = [tex]-\frac{\partial B}{\partial t}[/tex],
div B = 0,
curl B = J + [tex]\frac{\partial E}{\partial t}[/tex],
div E = [tex]\rho[/tex]
where t = time, and time derivatives commute with [tex]\nabla[/tex]
.........
how could you show that [tex]\frac{\partial p}{\partial t}[/tex] + div J = 0
.........
when [tex]\rho = 0[/tex] and J = 0 everywhere how can you show that:
[tex]\nabla^2E - \frac{\partial^2E}{\partial t^2}[/tex] = 0
and
[tex]\nabla^2B - \frac{\partial^2B}{\partial t^2}[/tex] = 0
a physical system is governed by the following:
curl E = [tex]-\frac{\partial B}{\partial t}[/tex],
div B = 0,
curl B = J + [tex]\frac{\partial E}{\partial t}[/tex],
div E = [tex]\rho[/tex]
where t = time, and time derivatives commute with [tex]\nabla[/tex]
.........
how could you show that [tex]\frac{\partial p}{\partial t}[/tex] + div J = 0
.........
when [tex]\rho = 0[/tex] and J = 0 everywhere how can you show that:
[tex]\nabla^2E - \frac{\partial^2E}{\partial t^2}[/tex] = 0
and
[tex]\nabla^2B - \frac{\partial^2B}{\partial t^2}[/tex] = 0