ELECTRIC POTENTIAL AND CAPACITANCE

Short Question Answers

Q1. Derive an expression for the electric potential due to a point charge.

Ans. capacitors_series_connection

Consider a point charge $+q$ at the origin as shown in the figure. Work done for $dx$ is $dW$.$$\therefore dW=-Fdx\cos\theta$$$$dW=-Fdx\quad ( \because \cos\theta =1)$$
The total work done in bringing a test positive charge $q_{\circ}$ from infinity to the point $P$ $$W=-\:\int_{\infty}^{r} \frac{1}{4\pi\varepsilon_{\circ}}\frac{qq_{\circ}}{x^{2}}dx$$$$W=-\:\frac{1}{4\pi\varepsilon_{\circ}}\int_{\infty}^{r} \frac{1}{x^{2}}dx$$ $$W=-\:\frac{qq_{\circ}}{4\pi\varepsilon_{\circ}} \left [ \frac{-1}{x} \right ]_{\infty}^{r} $$$$W=-\:\frac{qq_{\circ}}{4\pi\varepsilon_{\circ}} \left [ \frac{-1}{r} +\frac{-1}{\infty} \right ] $$$$W= \frac{1}{4\pi\varepsilon_{\circ}} \frac{qq_{\circ}}{r} $$$$\frac{W}{q_{\circ}}= \frac{1}{4\pi\varepsilon_{\circ}} \frac{q}{r} $$$$\therefore \text{Potential}\:\: V = \frac{1}{4\pi\varepsilon_{\circ}} \frac{q}{r} $$


Q2. Derive an expression for the capacitance of a parallel plate capacitor

Ans. parallel_plate_capacitor

$A$ is a area of each plate, $d$ is separation between the two parallel plates. $q$ and $–q$ are charges on each plate surface charged density on $\sigma=\frac{q}{A}$.In the inner region between the plates, the electric flelds due to the two charged plates$$E=\frac{\sigma}{2\varepsilon_0}+\frac{\sigma}{2\varepsilon_0}=\frac{\sigma}{\varepsilon_0}=\frac{q}{\varepsilon_0A}$$parallel plates in capacitor behave like equipotential surfaces.
 $\therefore $Potential $V=Ed$ $$V=\frac{q}{\varepsilon_0A}d$$$$\frac{V}{q}=\frac{q}{\varepsilon_0A}$$$$ \frac{1}{C}=\frac{d}{\varepsilon_0A}$$$$ C=\frac{\varepsilon_0A}{d}$$The above equation represents capacitance of a parallel plate capacitor.


Q3. Explain series combination of capacitors. Derive the formula for equivalent capacitance in each combination

Ans. Series combination: In series combination first capacitor second plate is connected to second capacitor first plate and second capacitor second plate is connected to third capacitor first plate and so on first capacitor first plate and last capacitor second plate is connected to opposite terminals of a battery.

capacitors_series_connection

Three capacitors of capacities $C_1, C_2$ and $C_3$ are connected in series combination as shown in the figure.In series combination the charge on each capacitor will be same but potential is different. $V_1=\frac{q}{C_1},V_2=\frac{q}{C_2},V_3=\frac{q}{C_3} $and $ V=\frac{q}{C}$
Total potential difference across the series combination is $$V = V_1 + V_2 + V_3$$ $$\frac{q}{C}=\frac{q}{C_1}+\frac{q}{C_2}+\frac{q}{C_3} $$$$\frac{1}{C}=\frac{1}{C_1}+\frac{1}{C_2}+\frac{1}{C_3} $$
The above equation represents equivalent capacitance in series combination


Q4. Explain parallel combination of capacitors. Derive the formula for equivalent capacitance in each combination.

Ans. Parallel combination: If the first plates of all the capacitors connected to common terminal and second plates of all the capacitors connected to common
terminal and these terminals are connected to oppositeterminals of the battery

capacitors_parallel_connection

Three capacitors of capacities $C_1, C_2$ and $C_3$ are connected in parallel combination as shown in the figure.In parallel combination the potential on each capacitor will be same but charge is different.
 $q_1={V}{C_1},q_2= {V}{C_2},q_3= {V}{C_3} $and $ Q={V}{C}$.
Total charge in the parallel combination is $$Q = q_1 + q_2 + q_3$$ $${V}{C}={V}{C_1}+{V}{C_2}+ {V}{C_3} $$$$ {C}= {C_1}+ {C_2}+ {C_3} $$
The above equation represents equivalent capacitance in parallel combination