The plates of a parallel plate capacitor are of area \(A\), distance apart \(x\) and are at a potential difference \(V\). A slab of dielectric of uniform thickness \(t\) and relative permittivity \(\varepsilon_{1}\) is inserted between the plates. Find the change in electric energy of the capacitor if the plates are (a) isolated and (b) maintained at their initial potential difference by a battery.

Short Answer

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Question: Calculate the change in electric energy of a parallel plate capacitor (a) when the plates are isolated, and (b) when the plates are maintained at their initial potential difference by a battery, after inserting a dielectric with thickness 't' and dielectric constant '\(\varepsilon_{1}\)'.

Step by step solution

01

(a) Change in electric energy when plates are isolated

Step 1: Calculate the initial capacitance without the dielectric \(C_{0} = \varepsilon_{0} A / x\) Step 2: Calculate the capacitance with the dielectric for the isolated case \(C_{1} = \varepsilon_{1} A / (x - t)\) Step 3: Calculate the initial electric energy without the dielectric \(E_{0} = \frac{1}{2} C_{0} V^2\) Step 4: Calculate the final electric energy with the dielectric for the isolated case \(E_{1} = \frac{1}{2} C_{1} V^2\) Step 5: Calculate the change in electric energy for the isolated case \(\Delta E = E_{1} - E_{0}\)
02

(b) Change in electric energy when plates are maintained at initial potential difference

Step 1: Calculate the initial capacitance without the dielectric (same as before) \(C_{0} = \varepsilon_{0} A / x\) Step 2: Calculate the capacitance with the dielectric for the maintained potential difference case \(C_{2} = \varepsilon_{0} A / (x - \frac{t}{\varepsilon_{1}})\) Step 3: Calculate the initial electric energy without the dielectric (same as before) \(E_{0} = \frac{1}{2} C_{0} V^2\) Step 4: Calculate the final electric energy with the dielectric for the maintained potential difference case \(E_{2} = \frac{1}{2} C_{2} V^2\) Step 5: Calculate the change in electric energy for the maintained potential difference case \(\Delta E = E_{2} - E_{0}\)

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