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Q. A non-conducting sphere of radius $R$ has a positive charge $Q$ uniformly distributed over its entire volume. A smaller, concentric, spherical volume of radius $r(r< R)$ is scooped out of the sphere. The magnitude of the electric field $E$ at a point inside the body at a distance $x$ from the centre is $(r$ $ < x< R)$ is $(K=1)\left(4 \pi \in_0\right)=$ constant $)$ :

Electric Charges and Fields

Solution:

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Charge of the remaining part after scooped out of the sphere
$=Q-\frac{Q}{\frac{4}{3} \pi R^3} \times \frac{4}{3} \pi R^3$
$=Q\left(1-\frac{r 3}{R^3}\right)=\frac{Q\left(R^3-r^3\right)}{R^3}$
Now charge of the part $r <\ldots . .< x$
$=\frac{Q\left(1-\frac{r 3}{R^3}\right)}{\frac{4}{5} \pi\left(R^3-r^3\right)} \times \frac{4}{3} \pi\left(x^2-r^3\right)=\frac{Q}{R^3}\left(x^3-r^3\right)=Q^1$
Now field at $P =K \frac{Q^1}{x^2}=\frac{K}{x^2}$
$\frac{Q}{R^3}\left(x^3-r^3\right)=\frac{K Q}{x^2}\left(\frac{x^3-r^3}{R^3}\right)$