00:01
The average power that is delivered to the circuit is equal to the rms voltage times the rms current times the cosine of the phase.
00:16
But now remember that the rms voltage is equal to the rms current times the impedance.
00:26
Then the rms current is equal to the voltage divided by the impedance.
00:34
And therefore, the average power can be written as v rms squared divided by the impedance times the cosine of the phase.
00:46
But the cosine of the phase is equal to the resistance divided by the impedance.
00:51
And the average power is equal to the rmass voltage squared divided by the impedance squared times the resistance.
00:59
In the first item, the circuit is driven at resonance.
01:05
Then, remember that at resonance, both reactances are equal, and therefore the impedance is equal to the resistance.
01:20
Then, in this case, the average power is equal to the rms voltage squared divided by the resistance.
01:31
And this is equal to 21 .5 squared divided by 20, which is approximately 23 .1 watts.
01:46
On the next item, the frequency of the circuit is equal to two times the resonant frequency, and the resonant frequency is equal to 1 divided by the square root of l times c.
02:01
Then this is the frequency of the circuit.
02:05
The impedance is equal to the square root of r squared plus the difference between both reactances squared.
02:18
Before plugging anything in this equation, let us take a look at the reactances.
02:24
The capacity reactance is equal to 1 divided by the frequency times the capacitance...