A hollow metal sphere of radius $R$ is uniformly charged. The electric field due to the sphere at a distance r from the centre
increases as $\mathrm{r}$ increases for $\mathrm{r}<\mathrm{R}$ and for $\mathrm{r}>\mathrm{R}$
zero as $\mathrm{r}$ increases for $\mathrm{r}<\mathrm{R}$, decreases as $\mathrm{r}$ increases for $\mathrm{r}>\mathrm{R}$
zero as $\mathrm{r}$ increases for $\mathrm{r}<\mathrm{R},$ increases as $\mathrm{r}$ increases for $\mathrm{r}>\mathrm{R}$
decreases as $\mathrm{r}$ increases for $\mathrm{r}<\mathrm{R}$ and for $\mathrm{r}>\mathrm{R}$
Mention applications of Gauss’s law.
Obtain the formula for the electric field due to a long thin wire of uniform linear charge density $E$ without using Gauss’s law.
Three infinitely long charged thin sheets are placed as shown in figure. The magnitude of electric field at the point $P$ is $\frac{x \sigma}{\epsilon_0}$. The value of $x$ is_____. (all quantities are measured in $SI$ units).
A conducting sphere of radius $10\, cm$ has unknown charge. If the electric field at a distance $20\, cm$ from the centre of the sphere is $1.2 \times 10^3\, N\, C^{-1}$ and points radially inwards. The net charge on the sphere is
The electric field $E$ is measured at a point $P (0,0, d )$ generated due to various charge distributions and the dependence of $E$ on $d$ is found to be different for different charge distributions. List-$I$ contains different relations between $E$ and $d$. List-$II$ describes different electric charge distributions, along with their locations. Match the functions in List-$I$ with the related charge distributions in List-$II$.
List-$I$ | List-$II$ |
$E$ is independent of $d$ | A point charge $Q$ at the origin |
$E \propto \frac{1}{d}$ | A small dipole with point charges $Q$ at $(0,0, l)$ and $- Q$ at $(0,0,-l)$. Take $2 l \ll d$. |
$E \propto \frac{1}{d^2}$ | An infinite line charge coincident with the x-axis, with uniform linear charge density $\lambda$ |
$E \propto \frac{1}{d^3}$ | Two infinite wires carrying uniform linear charge density parallel to the $x$-axis. The one along ( $y=0$, $z =l$ ) has a charge density $+\lambda$ and the one along $( y =0, z =-l)$ has a charge density $-\lambda$. Take $2 l \ll d$ |
plane with uniform surface charge density |