1 00:00:01,850 --> 00:00:04,490 All righty, let's work through some examples of 2 00:00:04,490 --> 00:00:07,020 finding Thevenin equivalent circuits. 3 00:00:07,020 --> 00:00:08,350 Take a look at this circuit right here. 4 00:00:08,350 --> 00:00:11,610 We want to determine the Thevenin equivalent circuit 5 00:00:11,610 --> 00:00:15,190 between the terminals a and b. 6 00:00:15,190 --> 00:00:17,690 That means we need to find the open circuit voltage and 7 00:00:17,690 --> 00:00:19,980 we need to determine the Thevenin equivalent resistance. 8 00:00:21,020 --> 00:00:26,479 Now, you'll notice the open circuit voltage is the voltage across here, but 9 00:00:26,479 --> 00:00:32,702 because it's open circuit, that means that there's no current flowing through here. 10 00:00:32,702 --> 00:00:36,732 I equals zero, so if there's no current flowing through that resister, 11 00:00:36,732 --> 00:00:39,404 there's no voltage drop across that resister. 12 00:00:39,404 --> 00:00:45,152 And the voltage at the terminals, the open circuit voltage then, 13 00:00:45,152 --> 00:00:50,190 is, in fact, the voltage across this 30 ohm resistor. 14 00:00:51,510 --> 00:00:53,360 Again, because there's no voltage drop here, 15 00:00:53,360 --> 00:00:57,310 the voltage that hit this point is the same as the voltage at this point. 16 00:00:59,000 --> 00:01:03,495 And again, because there's no current going here, the current source here, 17 00:01:03,495 --> 00:01:09,220 0.5 amps flowing is driving these two in series at this point. 18 00:01:10,380 --> 00:01:14,550 And we have then that V open circuit is simply equal 19 00:01:14,550 --> 00:01:19,350 to 0.5 times, 0.5 is the current, 20 00:01:19,350 --> 00:01:25,130 times the 30 ohms is equal to 15 volts. 21 00:01:26,840 --> 00:01:29,330 We now need to determine the Thevenin equivalent resistance, 22 00:01:29,330 --> 00:01:31,250 which we're gonna do in each of the three methods. 23 00:01:31,250 --> 00:01:35,300 Or at least consider whether each of those three different methods will work for 24 00:01:35,300 --> 00:01:36,650 this circuit. 25 00:01:36,650 --> 00:01:41,780 Method one works when we have at least one independent source, which we have here. 26 00:01:42,790 --> 00:01:45,741 Method one involves finding the short circuit current. 27 00:01:47,716 --> 00:01:53,640 And then, forming the ratio, V, open circuit divided by I, short circuit. 28 00:01:53,640 --> 00:01:58,749 So if we short this out, short the terminals, 29 00:01:58,749 --> 00:02:05,590 the current flowing through that short is I, short circuit. 30 00:02:05,590 --> 00:02:10,251 Now, how do we find I, short circuit in this circuit? 31 00:02:10,251 --> 00:02:17,738 Well, by shorting that, out that brings this, the voltage here, down to ground. 32 00:02:17,738 --> 00:02:25,072 We have 0.5 amps flowing into now a node which consists of two resistors, 33 00:02:25,072 --> 00:02:29,783 this 30 ohm resistor and this 5 ohm resistor. 34 00:02:29,783 --> 00:02:33,296 Some of the current's gonna through the 5 ohm resistor, that's our short circuit 35 00:02:33,296 --> 00:02:36,627 current, the rest of the current is gonna come through this 30 ohm resistor. 36 00:02:36,627 --> 00:02:39,090 We have a current divider here. 37 00:02:39,090 --> 00:02:42,600 So using current divider, we can calculate short circuit directly. 38 00:02:42,600 --> 00:02:49,640 I short circuit is equal to 0.5 times, and remember from the current divider, 39 00:02:49,640 --> 00:02:55,740 the term that goes in the numerator is the resistance in the other branch. 40 00:02:55,740 --> 00:03:01,340 So that would be 30 ohms divided by the sum of those two, 41 00:03:01,340 --> 00:03:04,930 30 plus 5 is 35 ohms. 42 00:03:04,930 --> 00:03:10,740 And we get then the short circuit current 43 00:03:10,740 --> 00:03:16,970 is equal to 0.4286, 0.4286 amps. 44 00:03:16,970 --> 00:03:22,098 And then RTh is equal to Voc 45 00:03:22,098 --> 00:03:27,927 divided by Isc, which is 15 46 00:03:27,927 --> 00:03:34,100 divided by 0.4286. 47 00:03:34,100 --> 00:03:39,155 Which, when we get the calculator out on that, you'll find that equals 35 ohms. 48 00:03:42,080 --> 00:03:45,143 So, method 1. 49 00:03:45,143 --> 00:03:50,166 Method 2, let's clear this up just a little bit. 50 00:03:50,166 --> 00:03:50,838 All righty, 51 00:03:50,838 --> 00:03:54,768 now let's use method 2 to determine the Thevenin equivalent resistance. 52 00:03:54,768 --> 00:04:00,038 In method 2, which works if you have, 53 00:04:00,038 --> 00:04:04,200 only, independent sources. 54 00:04:05,320 --> 00:04:07,930 Method two, you deactivate the sources. 55 00:04:07,930 --> 00:04:10,390 In this case, we have an independent current source. 56 00:04:10,390 --> 00:04:12,770 We turn the independent current source to zero. 57 00:04:12,770 --> 00:04:17,457 And, that is effectively, open circuiting this branch, 58 00:04:17,457 --> 00:04:23,094 which means that there will be no current flowing through this branch. 59 00:04:23,094 --> 00:04:27,362 Such that as we look back in to the circuit, 60 00:04:27,362 --> 00:04:33,661 this is just hanging unconnected and does not enter into this. 61 00:04:33,661 --> 00:04:36,352 Effectively, we have, because this is open circuit here, 62 00:04:36,352 --> 00:04:38,639 this is effectively an infinite resistance here. 63 00:04:39,840 --> 00:04:46,150 And we see coming back into this then, the 5 ohms in series with the 35. 64 00:04:46,150 --> 00:04:47,843 So method 2, 65 00:04:52,796 --> 00:05:00,782 We get that R Thevenin is simply the 30 + 5 ohms = 35 ohms, 66 00:05:00,782 --> 00:05:04,864 same value we got for method 1. 67 00:05:04,864 --> 00:05:06,592 Now, let's take a look at method 3. 68 00:05:06,592 --> 00:05:12,062 Method 3 works regardless of the types of sources that we have, 69 00:05:12,062 --> 00:05:17,344 but in method 3, we do deactivate the independent sources. 70 00:05:17,344 --> 00:05:19,777 So once again, we have this independent current source. 71 00:05:19,777 --> 00:05:23,240 By deactivating it, we open the circuit. 72 00:05:23,240 --> 00:05:28,185 And then, method 3 says that we apply a test voltage, 73 00:05:28,185 --> 00:05:33,238 which then forces a test current into the AB terminals, 74 00:05:33,238 --> 00:05:39,497 and we then algebraically work to make the ratio of V test over I test. 75 00:05:39,497 --> 00:05:44,476 So method 3 then Is form the ratio V 76 00:05:44,476 --> 00:05:49,988 test over I test to give us R Thevenin. 77 00:05:49,988 --> 00:05:55,286 All righty, with that open circuit, this is a simple situation. 78 00:05:55,286 --> 00:06:00,987 I, going in here, we can write a KVL loop going 79 00:06:00,987 --> 00:06:05,969 around this loop in the direction of IT. 80 00:06:05,969 --> 00:06:12,450 So KVL, we have then, minus v test going in the direction of current flow. 81 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. 82 00:06:21,180 --> 00:06:27,325 That's a plus sign, 30 I sub t, the sum of those terms equals zero. 83 00:06:27,325 --> 00:06:30,349 Let's bring in V test over to the other side of the positive V test, 84 00:06:30,349 --> 00:06:31,378 factor out the I test. 85 00:06:31,378 --> 00:06:38,500 We had I test x 5 + 30 is 35 = V test. 86 00:06:38,500 --> 00:06:42,972 Divide both sides by I test, that gives us our R Thevenin, 87 00:06:42,972 --> 00:06:47,557 which is equal to the ratio of V test over I test = 35 ohms. 88 00:06:47,557 --> 00:06:52,837 So we get the same results in any one of the three methods, 89 00:06:52,837 --> 00:06:55,478 and we then, can or now can, 90 00:06:58,746 --> 00:07:03,966 Draw our Thevenin equivalent circuit, where V Thevenin 91 00:07:03,966 --> 00:07:09,523 is equal to 15 volts, and R Thevenin is equal to 35 ohms. 92 00:07:11,296 --> 00:07:14,359 Notice that the original circuit had a current source. 93 00:07:15,720 --> 00:07:20,260 But the Thevenin Equivalent Circuit replaces that source and 94 00:07:20,260 --> 00:07:24,500 all of the resistance, the effects of the resistance within this circuit, 95 00:07:25,600 --> 00:07:30,840 are represented by a single voltage source and the Thevenin Equivalent resistance.