(a) Define the capacitance of a capacitor. (b) State three factors on which the capacitance of a parallel plate capacitor depends. (c) Derive a formula for ...
(b) State three factors on which the capacitance of a parallel plate capacitor depends.
(c) Derive a formula for the energy W stored in a charged capacitor of capacitance C carrying a charge Q on either plate.
(d) Two capacitors of capacitance 4\(\mu F\) and 6\(\mu F\) are connected in series to a 100V d.c supply. Draw the circuit diagram and calculate the (i) charge on either plate of each capacitor (ii) p.d. across each capacitor; (iii) energy of the combined capacitors.
(a) Capacitance of a capacitor
The capacitance of a capacitor is the ratio of the magnitude of the charge \(Q\) on either plate to the potential difference \(V\) between the plates:
\[ C = \frac{Q}{V} \]
where \(Q\) is the charge (coulomb) and \(V\) is the p.d. (volt). Its SI unit is the farad (F).
(b) Factors affecting the capacitance of a parallel-plate capacitor
The common (overlapping) area \(A\) of the plates, with \(C \propto A\).
The distance of separation \(d\) between the plates, with \(C \propto \dfrac{1}{d}\).
The permittivity \(\varepsilon\) (nature) of the dielectric medium between the plates, with \(C \propto \varepsilon\).
These combine as \(C = \dfrac{\varepsilon A}{d}\).
(c) Energy \(W\) stored in a charged capacitor
When the capacitor already holds a charge \(q\), the p.d. across it is \(v = \dfrac{q}{C}\). To move a further small charge \(dq\) onto the plates the work done is
\[ dW = v\,dq = \frac{q}{C}\,dq \]
The total work to charge the capacitor from \(0\) to the final charge \(Q\) is therefore
\[ W = \int_{0}^{Q} \frac{q}{C}\,dq = \frac{1}{C}\cdot\frac{Q^{2}}{2} = \frac{Q^{2}}{2C} \]
Using \(Q = CV\), the same result may be written as
\[ W = \frac{Q^{2}}{2C} = \frac{1}{2}QV = \frac{1}{2}CV^{2} \]
(d) Two capacitors 4\(\mu\text{F}\) and 6\(\mu\text{F}\) in series across 100 V
Circuit diagram: the two capacitors are joined end to end (in series) in a single loop with the 100 V d.c. supply.
Series circuit: the 4 µF and 6 µF capacitors connected end to end with the 100 V d.c. supply.
Effective (combined) capacitance of capacitors in series:
(i) Charge on either plate of each capacitor. In a series circuit the charge is the same on every capacitor and equals the charge supplied to the combination:
The capacitance of a capacitor is the ratio of the magnitude of the charge \(Q\) on either plate to the potential difference \(V\) between the plates:
\[ C = \frac{Q}{V} \]
where \(Q\) is the charge (coulomb) and \(V\) is the p.d. (volt). Its SI unit is the farad (F).
(b) Factors affecting the capacitance of a parallel-plate capacitor
The common (overlapping) area \(A\) of the plates, with \(C \propto A\).
The distance of separation \(d\) between the plates, with \(C \propto \dfrac{1}{d}\).
The permittivity \(\varepsilon\) (nature) of the dielectric medium between the plates, with \(C \propto \varepsilon\).
These combine as \(C = \dfrac{\varepsilon A}{d}\).
(c) Energy \(W\) stored in a charged capacitor
When the capacitor already holds a charge \(q\), the p.d. across it is \(v = \dfrac{q}{C}\). To move a further small charge \(dq\) onto the plates the work done is
\[ dW = v\,dq = \frac{q}{C}\,dq \]
The total work to charge the capacitor from \(0\) to the final charge \(Q\) is therefore
\[ W = \int_{0}^{Q} \frac{q}{C}\,dq = \frac{1}{C}\cdot\frac{Q^{2}}{2} = \frac{Q^{2}}{2C} \]
Using \(Q = CV\), the same result may be written as
\[ W = \frac{Q^{2}}{2C} = \frac{1}{2}QV = \frac{1}{2}CV^{2} \]
(d) Two capacitors 4\(\mu\text{F}\) and 6\(\mu\text{F}\) in series across 100 V
Circuit diagram: the two capacitors are joined end to end (in series) in a single loop with the 100 V d.c. supply.
Series circuit: the 4 µF and 6 µF capacitors connected end to end with the 100 V d.c. supply.
Effective (combined) capacitance of capacitors in series:
(i) Charge on either plate of each capacitor. In a series circuit the charge is the same on every capacitor and equals the charge supplied to the combination: