Opus_723
- 175
- 3
Homework Statement
Assume the current in a series RLC circuit is given by I = ACω(sin(ωt) + \frac{α}{ω}cos(ωt))e^{-αt}.
Calculate the energy stored in the circuit at t=0. Then calculate the energy stored in the circuit one-quarter cycle later, at t=\frac{\pi}{2ω}.
Verfiy that the difference is equal to the energy dissipated in the resistor R during this interval.
For this problem, assume the damping is slight, that is, that \frac{α}{ω} << 1, and neglect quantities proportional to α^{2}.
The Attempt at a Solution
I'm pretty sure I have the first part right, since it seems like a straightforward use of \frac{CV^{2}}{2} + \frac{LI^{2}}{2}. A couple of e^{-αt}'s simplify to 1 when you plug in 0 and \frac{\pi}{2ω} for t since \frac{α}{ω} << 1.
But for the next part, I think they're asking me to integrate I^{2}Rdt over the interval, and I am not seeing how to approach that integral. Expanding the equation for I to get I^{2} just makes a mess no matter what small terms I ignore. I don't know if I'm just being clumsy with my math or if I'm approaching it wrong. I even tried using complex numbers to represent the power but I ended up with a nonsensical answer. Any advice on tackling this part of the problem?