KleZMeR
- 125
- 0
Homework Statement
The electric field is described by [itex]E = \frac{C e^{-br}}{r^2}[/itex],
find the charge density and then integrate over all-space and show it's zero.
[/B]
Homework Equations
[itex]E = \frac{C e^{-br}}{r^2} \\ \\[/itex]
[itex]\nabla \cdot E = \frac{\rho}{\epsilon_0} \\ \\[/itex]
[itex]\rho(r) = Q \delta^3 (r-r_0) \\ \\[/itex][/B]
[itex]I_{AllSpace} = \int_{0}^{\infty}\:f(r,\phi,\theta) \: r^2 \: dr \: sin\theta \: d\theta \: d\phi \\ \\[/itex]
[itex]\nabla = \frac{d}{dr} \hat{r} \\ \\[/itex]
[itex]\int_{0}^{\infty}f(r)Q \delta^3(r-r_0)dr = f(r_0) \\ \\[/itex]
The Attempt at a Solution
I tried to take [itex]\nabla E = \frac{\rho}{\epsilon_0}[/itex] and used the quotient solve for [itex]\rho(r)[/itex] and then integrated over all space and I do not get a zero.
With [itex]\nabla \cdot E = (\frac{-e^{-ar}}{r} \:(ra+2))[/itex]
[itex]\rho(r) = (\frac{-e^{-ar}}{r} \:(ra+2)) \: \epsilon_0[/itex]
and integrating over all space gives me
[itex]4\pi \int_{0}^{\infty}\rho(r) \: r^2 \: dr[/itex]
and this gives me [itex](-1 + undefined) \: \epsilon_0[/itex]
my only other idea here is to use the delta function, which in the case of the radial integral does give me a zero due to the [itex]r^2[/itex] term being evaluated at zero.
[itex]E_{AllSpace} = 4\pi \int_{0}^{\infty}\rho(r) \: r^2 \: dr = 4\pi Q \int_{0}^{\infty} \delta^3(r-r_0)r^2 \:dr = 0[/itex]
This second solution seems a bit short but I think it is still valid, I'm not sure if my first attempt if I made a mistake on the integral or if there is some other way of doing this? Any help would be appreciated.