WEBVTT 00:00:01.850 --> 00:00:04.490 All righty, let's work through some examples of 00:00:04.490 --> 00:00:07.020 finding Thevenin equivalent circuits. 00:00:07.020 --> 00:00:08.350 Take a look at this circuit right here. 00:00:08.350 --> 00:00:11.610 We want to determine the Thevenin equivalent circuit 00:00:11.610 --> 00:00:15.190 between the terminals a and b. 00:00:15.190 --> 00:00:17.690 That means we need to find the open circuit voltage and 00:00:17.690 --> 00:00:19.980 we need to determine the Thevenin equivalent resistance. 00:00:21.020 --> 00:00:26.479 Now, you'll notice the open circuit voltage is the voltage across here, but 00:00:26.479 --> 00:00:32.702 because it's open circuit, that means that there's no current flowing through here. 00:00:32.702 --> 00:00:36.732 I equals zero, so if there's no current flowing through that resister, 00:00:36.732 --> 00:00:39.404 there's no voltage drop across that resister. 00:00:39.404 --> 00:00:45.152 And the voltage at the terminals, the open circuit voltage then, 00:00:45.152 --> 00:00:50.190 is, in fact, the voltage across this 30 ohm resistor. 00:00:51.510 --> 00:00:53.360 Again, because there's no voltage drop here, 00:00:53.360 --> 00:00:57.310 the voltage that hit this point is the same as the voltage at this point. 00:00:59.000 --> 00:01:03.495 And again, because there's no current going here, the current source here, 00:01:03.495 --> 00:01:09.220 0.5 amps flowing is driving these two in series at this point. 00:01:10.380 --> 00:01:14.550 And we have then that V open circuit is simply equal 00:01:14.550 --> 00:01:19.350 to 0.5 times, 0.5 is the current, 00:01:19.350 --> 00:01:25.130 times the 30 ohms is equal to 15 volts. 00:01:26.840 --> 00:01:29.330 We now need to determine the Thevenin equivalent resistance, 00:01:29.330 --> 00:01:31.250 which we're gonna do in each of the three methods. 00:01:31.250 --> 00:01:35.300 Or at least consider whether each of those three different methods will work for 00:01:35.300 --> 00:01:36.650 this circuit. 00:01:36.650 --> 00:01:41.780 Method one works when we have at least one independent source, which we have here. 00:01:42.790 --> 00:01:45.741 Method one involves finding the short circuit current. 00:01:47.716 --> 00:01:53.640 And then, forming the ratio, V, open circuit divided by I, short circuit. 00:01:53.640 --> 00:01:58.749 So if we short this out, short the terminals, 00:01:58.749 --> 00:02:05.590 the current flowing through that short is I, short circuit. 00:02:05.590 --> 00:02:10.251 Now, how do we find I, short circuit in this circuit? 00:02:10.251 --> 00:02:17.738 Well, by shorting that, out that brings this, the voltage here, down to ground. 00:02:17.738 --> 00:02:25.072 We have 0.5 amps flowing into now a node which consists of two resistors, 00:02:25.072 --> 00:02:29.783 this 30 ohm resistor and this 5 ohm resistor. 00:02:29.783 --> 00:02:33.296 Some of the current's gonna through the 5 ohm resistor, that's our short circuit 00:02:33.296 --> 00:02:36.627 current, the rest of the current is gonna come through this 30 ohm resistor. 00:02:36.627 --> 00:02:39.090 We have a current divider here. 00:02:39.090 --> 00:02:42.600 So using current divider, we can calculate short circuit directly. 00:02:42.600 --> 00:02:49.640 I short circuit is equal to 0.5 times, and remember from the current divider, 00:02:49.640 --> 00:02:55.740 the term that goes in the numerator is the resistance in the other branch. 00:02:55.740 --> 00:03:01.340 So that would be 30 ohms divided by the sum of those two, 00:03:01.340 --> 00:03:04.930 30 plus 5 is 35 ohms. 00:03:04.930 --> 00:03:10.740 And we get then the short circuit current 00:03:10.740 --> 00:03:16.970 is equal to 0.4286, 0.4286 amps. 00:03:16.970 --> 00:03:22.098 And then RTh is equal to Voc 00:03:22.098 --> 00:03:27.927 divided by Isc, which is 15 00:03:27.927 --> 00:03:34.100 divided by 0.4286. 00:03:34.100 --> 00:03:39.155 Which, when we get the calculator out on that, you'll find that equals 35 ohms. 00:03:42.080 --> 00:03:45.143 So, method 1. 00:03:45.143 --> 00:03:50.166 Method 2, let's clear this up just a little bit. 00:03:50.166 --> 00:03:50.838 All righty, 00:03:50.838 --> 00:03:54.768 now let's use method 2 to determine the Thevenin equivalent resistance. 00:03:54.768 --> 00:04:00.038 In method 2, which works if you have, 00:04:00.038 --> 00:04:04.200 only, independent sources. 00:04:05.320 --> 00:04:07.930 Method two, you deactivate the sources. 00:04:07.930 --> 00:04:10.390 In this case, we have an independent current source. 00:04:10.390 --> 00:04:12.770 We turn the independent current source to zero. 00:04:12.770 --> 00:04:17.457 And, that is effectively, open circuiting this branch, 00:04:17.457 --> 00:04:23.094 which means that there will be no current flowing through this branch. 00:04:23.094 --> 00:04:27.362 Such that as we look back in to the circuit, 00:04:27.362 --> 00:04:33.661 this is just hanging unconnected and does not enter into this. 00:04:33.661 --> 00:04:36.352 Effectively, we have, because this is open circuit here, 00:04:36.352 --> 00:04:38.639 this is effectively an infinite resistance here. 00:04:39.840 --> 00:04:46.150 And we see coming back into this then, the 5 ohms in series with the 35. 00:04:46.150 --> 00:04:47.843 So method 2, 00:04:52.796 --> 00:05:00.782 We get that R Thevenin is simply the 30 + 5 ohms = 35 ohms, 00:05:00.782 --> 00:05:04.864 same value we got for method 1. 00:05:04.864 --> 00:05:06.592 Now, let's take a look at method 3. 00:05:06.592 --> 00:05:12.062 Method 3 works regardless of the types of sources that we have, 00:05:12.062 --> 00:05:17.344 but in method 3, we do deactivate the independent sources. 00:05:17.344 --> 00:05:19.777 So once again, we have this independent current source. 00:05:19.777 --> 00:05:23.240 By deactivating it, we open the circuit. 00:05:23.240 --> 00:05:28.185 And then, method 3 says that we apply a test voltage, 00:05:28.185 --> 00:05:33.238 which then forces a test current into the AB terminals, 00:05:33.238 --> 00:05:39.497 and we then algebraically work to make the ratio of V test over I test. 00:05:39.497 --> 00:05:44.476 So method 3 then Is form the ratio V 00:05:44.476 --> 00:05:49.988 test over I test to give us R Thevenin. 00:05:49.988 --> 00:05:55.286 All righty, with that open circuit, this is a simple situation. 00:05:55.286 --> 00:06:00.987 I, going in here, we can write a KVL loop going 00:06:00.987 --> 00:06:05.969 around this loop in the direction of IT. 00:06:05.969 --> 00:06:12.450 So KVL, we have then, minus v test going in the direction of current flow. 00:06:12.450 --> 00:06:19.354 We have then a voltage drop of plus five I sub t coming on down here plus 30. 00:06:21.180 --> 00:06:27.325 That's a plus sign, 30 I sub t, the sum of those terms equals zero. 00:06:27.325 --> 00:06:30.349 Let's bring in V test over to the other side of the positive V test, 00:06:30.349 --> 00:06:31.378 factor out the I test. 00:06:31.378 --> 00:06:38.500 We had I test x 5 + 30 is 35 = V test. 00:06:38.500 --> 00:06:42.972 Divide both sides by I test, that gives us our R Thevenin, 00:06:42.972 --> 00:06:47.557 which is equal to the ratio of V test over I test = 35 ohms. 00:06:47.557 --> 00:06:52.837 So we get the same results in any one of the three methods, 00:06:52.837 --> 00:06:55.478 and we then, can or now can, 00:06:58.746 --> 00:07:03.966 Draw our Thevenin equivalent circuit, where V Thevenin 00:07:03.966 --> 00:07:09.523 is equal to 15 volts, and R Thevenin is equal to 35 ohms. 00:07:11.296 --> 00:07:14.359 Notice that the original circuit had a current source. 00:07:15.720 --> 00:07:20.260 But the Thevenin Equivalent Circuit replaces that source and 00:07:20.260 --> 00:07:24.500 all of the resistance, the effects of the resistance within this circuit, 00:07:25.600 --> 00:07:30.840 are represented by a single voltage source and the Thevenin Equivalent resistance.