A parallel plate capacitor has a uniform electric field \(E\) in the space between the plates. If the distance between the plates is \(d\) and the area of each plate is \(A,\) the energy stored in the capacitor is:
| 1. | \(\dfrac{E^2 Ad}{\varepsilon_0}\) | 2. | \(\dfrac{1}{2}\varepsilon_0E^2 Ad\) |
| 3. | \(\varepsilon_0EAd\) | 4. | \(\dfrac{1}{2}\varepsilon_0E^2 \) |
| 1. | \(QV\) | 2. | \(\dfrac{Q}{V}\) |
| 3. | \(\dfrac{QV}{2}\) | 4. | \(\dfrac{Q}{2V}\) |
| 1. | \(\dfrac{1}{2} \varepsilon_{o} \dfrac{V^{2}}{d^{2}}\) | 2. | \(\dfrac{1}{2 \varepsilon_{o}} \dfrac{V^{2}}{d^{2}}\) |
| 3. | \(\dfrac{1}{2} C V^{2}\) | 4. | \(\dfrac{Q^{2}}{2 C}\) |