00:01
This problem is primarily about y -delta transformations.
00:07
It does use standard understandings of parallel and series resistances.
00:15
But what i've done is i've redrawn the circuit so that i can perform a delta y transformation.
00:24
And so i've turned it upside down.
00:26
That is a big thing to notice is that over here now this is minus and plus because it means now that power source is absorbing power and not supplying power but it allows me then to put them put the resistors in this kind of configuration and that in turn will allow me to transform it into and i'll show you how that's done here in just a moment that will allow me to transform it into a circuit that looks like this, where i have a resistor here and then a resistor here, one there, one there, and then going in now again into the bottom.
01:18
So that i have, in essence, this would be a series and a series.
01:26
So these would be in parallel.
01:28
So this is the big thing that we're going to do first is that transformation.
01:34
I'm going to flip over to another slide to show how that's done.
01:39
So these are the equations for when you have a delta and you're changing it into a y, and it's actually fairly simple and straightforward.
01:50
That you label your resistances r1, r2, and r3.
01:54
You label your corners a, b, and c.
01:58
And that allows you to change it from a delta into a y.
02:05
That hence the name.
02:06
It's not a very creative name necessarily.
02:09
So the resistance here at the top is going to be r1 times r2 and that is over the sum of the three resistances.
02:21
For rb down here, it is r1 and r3 multiplied and then divided by the sum of the resistances.
02:31
For rc, it is r2 and r3.
02:35
So you can see it follows a pattern...