Azael
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I apologise for any spelling errors or terms missnamed since I am swedish and this course I am reading is only swedish books and terms. But I think I have gotten the translations right. Also my first try with latex.
I have a non conducting sphere with the radius R and the volume charge density
[tex]\rho (r) = \rho_o (1- \frac{r}{R}[/tex] when 0<r<R
and [tex]\rho(r) = 0[/tex] when r>R
where [tex]\rho_0[/tex] is a positive constant.
I want to calculate the field E(r) for 0<r<R and R<r and I want to use this formula
[tex] E = \int \frac{dQ \hat{r}}{4 \pi \epsilon r^2}[/tex]
This is how I do it
[tex] E = \frac{\rho}{4 \pi \epsilon_0 } \int_{0}^{r} (1-\frac{r}{R}) sin\theta d\theta dr d\phi[/tex]
I get that to [tex]\bar{E}= \frac{\rho_o}{\epsilon_0} (r- \frac{r^2}{2R}) \hat{r}[/tex]
is that a correct answere for 0<r<R??
gonna post this now and se if I got the latex right
I have a non conducting sphere with the radius R and the volume charge density
[tex]\rho (r) = \rho_o (1- \frac{r}{R}[/tex] when 0<r<R
and [tex]\rho(r) = 0[/tex] when r>R
where [tex]\rho_0[/tex] is a positive constant.
I want to calculate the field E(r) for 0<r<R and R<r and I want to use this formula
[tex] E = \int \frac{dQ \hat{r}}{4 \pi \epsilon r^2}[/tex]
This is how I do it
[tex] E = \frac{\rho}{4 \pi \epsilon_0 } \int_{0}^{r} (1-\frac{r}{R}) sin\theta d\theta dr d\phi[/tex]
I get that to [tex]\bar{E}= \frac{\rho_o}{\epsilon_0} (r- \frac{r^2}{2R}) \hat{r}[/tex]
is that a correct answere for 0<r<R??
gonna post this now and se if I got the latex right
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