- #1
timn
- 19
- 0
Dear Physics Forums,
Given the potential
[tex]\Phi(\bar{r}) = \Phi_0\ln{\left(\frac{r_0}{r}\right)}[/tex]
calculate the electric field strength.
[tex]- \nabla \Phi = \bar{E}[/tex]
Due to the symmetry of the problem, consider the position vector [tex]\bar{r}[/tex] as a vector in spherical coordinates.
[tex]\bar{E}(\bar{r}) = -\nabla \Phi(\bar{r}) [/tex]
The potential depends only on the radial component, so the other terms of the gradient vanish.
[tex]\bar{E}(\bar{r}) = - \Phi_0 \frac{\partial}{\partial r} \ln{\frac{r_0}{r}} \hat{r}
= \Phi_0 \frac{1}{r} \hat{r} [/tex]
where [tex]\hat{r}[/tex] denotes the normalised radial base vector.
The answer is supposed to be [tex]\Phi_0 \frac{1}{r^2} \hat{r} [/tex], with a square in the denominator. What did I do wrong?
Homework Statement
Given the potential
[tex]\Phi(\bar{r}) = \Phi_0\ln{\left(\frac{r_0}{r}\right)}[/tex]
calculate the electric field strength.
Homework Equations
[tex]- \nabla \Phi = \bar{E}[/tex]
The Attempt at a Solution
Due to the symmetry of the problem, consider the position vector [tex]\bar{r}[/tex] as a vector in spherical coordinates.
[tex]\bar{E}(\bar{r}) = -\nabla \Phi(\bar{r}) [/tex]
The potential depends only on the radial component, so the other terms of the gradient vanish.
[tex]\bar{E}(\bar{r}) = - \Phi_0 \frac{\partial}{\partial r} \ln{\frac{r_0}{r}} \hat{r}
= \Phi_0 \frac{1}{r} \hat{r} [/tex]
where [tex]\hat{r}[/tex] denotes the normalised radial base vector.
The answer is supposed to be [tex]\Phi_0 \frac{1}{r^2} \hat{r} [/tex], with a square in the denominator. What did I do wrong?