00:03
Let's consider a scenario in which we have a battery with a certain internal resistance and electromotive force.
00:17
Another unusual looking at me.
00:20
Can't erase right now.
00:22
Secondical issues.
00:28
The fact that the battery is useful information.
00:33
We're not given the electromotive force in strict a sense, but we are told it's the variable.
00:40
Epsilon.
00:43
Same goes for internal resistance, not technically given it.
00:56
We're right an equal sign actually, but i'm overcommitted because i can't always right now.
01:04
We're also told that on external resistance is equal to 25 oms, the current is equal to 0 .665 ampers.
01:29
And that when r2 is equal to 55 oms, the current is equal to 0 .45 .5.
01:45
By ampiers.
01:51
Now, we are commissioned to find the electromotive force.
02:04
I think it would be helpful to review the definition of electromotive force.
02:08
The electromotive force is strictly a term used to refer to, say, some other energy source, say chemical energy.
02:18
That's been transferred into electrical units.
02:25
So it's like chemical energy into voltage.
02:29
But if for our intents and purposes, electromotive force is simply a voltage.
02:37
So whatever you give an electromotive force or a battery, you should consider it as follows.
02:48
Crew drawing of battery.
02:52
So this is the positive side.
02:53
This is the negative side.
02:56
You expect that to correspond to an internal voltage.
02:59
Of course, positive and negative.
03:02
Recalled at the larger end of this symbol, with that symbol in there, it's positive, whereas the smaller end is negative.
03:16
I do believe i forgot something.
03:18
There is an internal resistance.
03:24
We'll call that lowercase r.
03:28
Whereas this voltage, that's the electromagnet of force, or simply epsilon.
03:36
We're asked to consider a circuit in which this battery is connected to a resistor.
03:51
We'll call this uppercase r.
03:58
Now, let's assume the current is going this way.
04:08
In which case, the current goes towards the positive end of the resistor.
04:14
Simply by convention, hopefully the brainwashing has been working for you guys, so you may recall this.
04:25
So we want to find both epsilon and lowercase r, as you recall.
04:30
We are given uppercase r for two different scenarios and the corresponding current...