A capacitor of capacitance ‘C’ is charged to a potential ‘V’ and disconnected from the battery. Now if the space between the plates is completely filled with a substance of dielectric constant ‘K’, the final charge and the final potential on the capacitor are respectively:
\( KCV \) and \( \frac{V}{K} \)
\( CV \) and \( \frac{V}{K} \)
\( \frac{CV}{K} \) and \( KV \)
\( \frac{CV}{K} \) and \( \frac{V}{K} \)
Step 1: Understanding the Effect of Dielectric on a Disconnected Capacitor Since the capacitor is disconnected from the battery, its charge remains constant. The charge on the capacitor is given by: \[ Q = C V \] Step 2: Effect of Introducing the Dielectric When a dielectric material with dielectric constant \( K \) is introduced, the capacitance of the capacitor increases as: \[ C' = K C \] However, since the charge remains constant, the new potential \( V' \) across the capacitor is given by: \[ V' = \frac{Q}{C'} = \frac{CV}{KC} = \frac{V}{K} \] Thus, the final charge remains \( CV \), and the new potential is \( \frac{V}{K} \).
A parallel plate capacitor has two parallel plates which are separated by an insulating medium like air, mica, etc. When the plates are connected to the terminals of a battery, they get equal and opposite charges, and an electric field is set up in between them. This electric field between the two plates depends upon the potential difference applied, the separation of the plates and nature of the medium between the plates.
Match the following: