00:01
So for this problem, we have the same setup as an earlier problem.
00:06
So make sure to refer to that problem because we're going to use that result for this one.
00:12
The only difference for this new one is that now we have a battery.
00:18
So there's a battery here of 90 volts.
00:21
And when the switch closes, we're going to have not a discharging capacitor, but a charging capacitor.
00:27
However, the result for the current is going to be identical.
00:36
It's actually the exact same formula.
00:37
So this is what we found for the current in the small loop.
00:46
What we found was n -mu -0 -b over 2 -p times the lawn of 1 plus a over c times i over rc times i over rc, times 1 over r small, where now i is 5 .00 amps, and r small was 15 oms.
01:19
So it's the exact same result because the exact same physics is involved.
01:27
D -i -d -t is still going to be i over rc, so it doesn't matter that it's charging versus discharging, because you'll see when you take the derivative that the exact same functional form is found.
01:43
So when you take the derivative of 1 minus e to the negative t over r not c, that's still 1 over r0c times e to the negative t over r not c.
02:00
So it's the exact same formula.
02:05
So once you substitute in the given numbers, you should find that this is 1 .83 times 10 to the minus 3 amperes.
02:18
Again, so refer to the problem that's referenced in this question to see where this formula comes from, but the point is it's the exact same formula...