00:01
One of the most straightforward circuits to deal with in an ac setting is a household circuit where everything is in parallel and one in which you only have resistors.
00:15
What is true in such a case is that the average power that is dissipated by each resistor is the rms current, root mean square current, going through the resistor.
00:31
And i'll put this as a delta v.
00:34
Rms, indicating that it is an amplitude of some sort.
00:40
So let's take a look at an example.
00:43
Well, before we do the example, i do want to point out that the voltage through a resistor is in phase with the current through it.
00:55
And we have the omslaw relationship that irms is equal to delta v.
01:07
Rms divided by the resistance.
01:12
So as an example, let's take a look at the circuit above with three light bulbs, which can be essentially treated as light as resistors.
01:28
They aren't perfect resistors because they do change resistance as they heat up, but we'll assume that they've been lit for a while and have stabilized.
01:41
But we know the power average used by each light bulb, so that is usually what is given stamped on the light bulb.
01:50
So we'll call them bulbs 1, 2, and 3, just so we have a distinction there.
01:58
But bulb number 1, we can think about the current through it is simply the power 150 watts, divided by 120 volts.
02:13
So that's 1 .25 amps.
02:15
And likewise for bulb number two.
02:20
What is true is that the current going through each of those bulbs and i'll show it's a straight line, but of course it's oscillating.
02:31
It's also 150 watts divided by 120 volts.
02:40
Whereas for the third bulb, we simply do the same thing, but with 100 watts.
02:58
And that goes intuitively with the idea that the higher wattage bulb is going to have to have more current going through it...