
A thin conducting ring of radius $R$ is given a charge $+Q$. The electric field at the centre $O$ of the…

- $3 \mathrm{E}$ along $\mathrm{KO}$
- E along $O K$
- $E$ along $K O$
- $3 E$ along $O K$
Solution
$\overrightarrow{\mathbf{E}}_{\text {total }}=0$
$\begin{aligned}
\overrightarrow{\mathbf{E}}_{A K B}+\overrightarrow{\mathbf{E}}_{A C D B} & =0 \\
\overrightarrow{\mathbf{E}}_{A C D B} & =-\overrightarrow{\mathbf{E}}_{A K B} \\
\overrightarrow{\mathbf{E}}_{A C D B} & =-\overrightarrow{\mathbf{E}} \text { (along } K O \text {) }
\end{aligned}$
Therefore, the electric field at the centre due to the charge on the part $A C D B$ of the ring is $E$ along $O K$.
Alternative :

The fields at $O$ due to $A C$ and $B D$ cancel each other.
The field due to $C D$ is acting in the direction $O K$ and equal in magnitude to $E$ due to $A K B$.
Asked in: NEET 2008 (Screening)