The capacitance \( C \) of the system can be calculated using the formula for capacitance: \[ C = \frac{Q}{V} \] where:
\( Q = 80 \, \mu C = 80 \times 10^{-6} \, C \),
\( V = 16 \, \text{V} \).
Therefore, the capacitance is: \[ C = \frac{80 \times 10^{-6}}{16} = 5 \, \mu F \]
(ii) When the dielectric constant \( k = 3 \) is inserted, the capacitance increases by a factor of \( k \). The new capacitance \( C' \) becomes: \[ C' = kC = 3 \times 5 \, \mu F = 15 \, \mu F \] Since \( Q = C'V' \), and the charge \( Q \) remains the same, the new potential difference \( V' \) is: \[ V' = \frac{Q}{C'} = \frac{80 \times 10^{-6}}{15 \times 10^{-6}} = 5.33 \, \text{V} \]
(iii) The capacitance of the system depends only on the geometry of the conductors and the dielectric constant of the medium between them, not the charges. Therefore, if the charges are doubled, the capacitance remains unchanged. The capacitance will still be \( 5 \, \mu F \), because capacitance is independent of the charge.
A circuit consisting of a capacitor C, a resistor of resistance R and an ideal battery of emf V, as shown in figure is known as RC series circuit.
As soon as the circuit is completed by closing key S₁ (keeping S₂ open) charges begin to flow between the capacitor plates and the battery terminals. The charge on the capacitor increases and consequently the potential difference Vc (= q/C) across the capacitor also increases with time. When this potential difference equals the potential difference across the battery, the capacitor is fully charged (Q = VC). During this process of charging, the charge q on the capacitor changes with time t as
\(q = Q[1 - e^{-t/RC}]\)
The charging current can be obtained by differentiating it and using
\(\frac{d}{dx} (e^{mx}) = me^{mx}\)
Consider the case when R = 20 kΩ, C = 500 μF and V = 10 V.