1 00:00:00,830 --> 00:00:04,520 Now let's talk about admittance and how to use it in current dividers. 2 00:00:04,520 --> 00:00:08,160 Remember that resistance is a value that's given in ohms. 3 00:00:08,160 --> 00:00:12,200 It's inverse, 1 over R is called admittance. 4 00:00:12,200 --> 00:00:17,620 We usually use G to represent that and it's given in inverse ohms or 5 00:00:17,620 --> 00:00:23,500 ohms to the -1, or 1 over ohms, and sometimes we call that Mhos. 6 00:00:23,500 --> 00:00:26,040 Kinda see it's ohms backwards. 7 00:00:26,040 --> 00:00:31,230 So admittance, right here is one over the resistance. 8 00:00:31,230 --> 00:00:32,790 We use that in a lot of good math. 9 00:00:32,790 --> 00:00:37,960 For example, remember that if we have resistors in series, R1, R2, and 10 00:00:37,960 --> 00:00:43,420 R3, that if we want to have the total resistance 11 00:00:43,420 --> 00:00:48,514 over this region, R = R1 + R2 + R3. 12 00:00:49,710 --> 00:00:56,520 If we had values that were in parallel, then we had to handle that differently. 13 00:00:56,520 --> 00:01:00,810 One very easy way of handling that is to put admittances in parallel. 14 00:01:03,950 --> 00:01:09,990 If we use values G1, G2, and G3, then we can say 15 00:01:09,990 --> 00:01:16,260 that the entire admittance G, from this point a to this point b, 16 00:01:16,260 --> 00:01:22,217 so G from a to b = G1 + G2 + G3. 17 00:01:23,320 --> 00:01:28,610 So it's very handy to add up resistors in parallel by treating them as admittances 18 00:01:28,610 --> 00:01:29,910 instead of as resistors. 19 00:01:31,520 --> 00:01:34,580 Now let's do a current divider using resistance. 20 00:01:34,580 --> 00:01:37,180 Remember that when we've got a current divider like this, 21 00:01:37,180 --> 00:01:41,710 we first have to combine two of the resistors in parallel. 22 00:01:41,710 --> 00:01:46,740 Let's say that what I want to find is I1, so I would combine these in parallel. 23 00:01:46,740 --> 00:01:51,911 This would be equal to R2 times R3 over R2 + R3. 24 00:01:51,911 --> 00:01:54,146 Then if I wanted to find I1, 25 00:01:54,146 --> 00:02:00,620 that would be equal to I0 times the resistors that it's not going through. 26 00:02:00,620 --> 00:02:05,604 Which is this R2 times R3 over R2 + R3 27 00:02:05,604 --> 00:02:09,417 divided by all the resistors, 28 00:02:09,417 --> 00:02:14,119 which is R1 + R2R3 over R2 + R3. 29 00:02:15,560 --> 00:02:18,590 That's how we handle a current divider using resistance. 30 00:02:18,590 --> 00:02:21,180 But if we wanted to use admittance instead, 31 00:02:21,180 --> 00:02:23,370 here's the way that we can do that. 32 00:02:23,370 --> 00:02:28,793 We don't even need to combine this into series and parallel, 33 00:02:28,793 --> 00:02:34,737 we're just going to be able to say that I1 = Io times the admittance 34 00:02:34,737 --> 00:02:39,559 that it is going through, divided by G1 + G2 + G3. 35 00:02:39,559 --> 00:02:43,347 That's really a lot easier than what we did on the previous page, so 36 00:02:43,347 --> 00:02:47,800 I'm gonna say this is a really cool way of doing current dividers. 37 00:02:47,800 --> 00:02:51,450 I'm going to show you how similar that is to doing voltage dividers. 38 00:02:51,450 --> 00:02:57,777 If we have, so this is a voltage divider, if we have resistors in series, 39 00:02:57,777 --> 00:03:02,790 R1, R2, and R3, let's say that I wanted to find V1. 40 00:03:02,790 --> 00:03:09,759 Then V1 would be equal to, this is the total voltage across here, 41 00:03:09,759 --> 00:03:14,380 V0 times R1, divided by R1 + R2 + R3. 42 00:03:14,380 --> 00:03:19,970 You can see the form of these two equations is equivalent except, 43 00:03:19,970 --> 00:03:26,480 that one is handling parallel admittances, the other is handling series resistances. 44 00:03:26,480 --> 00:03:32,070 Now let's do an example just with numbers, let's do a resistive current divider 45 00:03:33,940 --> 00:03:39,500 like this with 1 ohm, a 2 ohm, and a 3 ohm resistor. 46 00:03:39,500 --> 00:03:44,630 And let's say that I want to find I1 given that I have 10 amps 47 00:03:44,630 --> 00:03:47,900 of current going in, that is I0. 48 00:03:47,900 --> 00:03:52,009 So we will first of all need to convert this two admittances and 49 00:03:52,009 --> 00:03:58,873 what we would have Is 1 divided by 3 mhos, 50 00:03:58,873 --> 00:04:05,280 1 divided by 2 mhos and 1 divided by 1 mhos. 51 00:04:05,280 --> 00:04:10,490 And again, we're looking for I1 with an I0 of 10 amps going in. 52 00:04:10,490 --> 00:04:14,363 So what we would say is, I1 = 10 amps, 53 00:04:14,363 --> 00:04:20,785 that's the I0 value times the admittance that it is going through, 54 00:04:20,785 --> 00:04:26,340 1 mho, divided by the sum of all of the other admittances. 55 00:04:28,880 --> 00:04:30,880 And that's our I1 value. 56 00:04:30,880 --> 00:04:35,520 That's really very simple, whole lot simpler than doing it with resistances.