1. | \(\dfrac{3}{5}\) | 2. | \(\dfrac{4}{5}\) |
3. | \(\dfrac{3}{4}\) | 4. | \(\dfrac{4}{3}\) |
The charge flowing through a resistance \(R\) is given by
\(q = A\sin\omega t+B\cos\omega t\)
The heat produced in the resistance over a very long time \(\Delta t\) (much greater than \(T = \dfrac{2\pi}{\omega}\)) is:
1. | \(\omega^{2}\left(A^{2}+B^{2}\right) R \Delta t\) |
2. | \(\omega^{2}\left(A^{2}-B^{2}\right) R \Delta t\) |
3. | \(\dfrac{1}{2} \omega^{2}\left(A^{2}+B^{2}\right) R \Delta t\) |
4. | \(\dfrac{1}{2} \omega^{2}\left(A^{2}-B^{2}\right) R \Delta t\) |