1 00:00:03,290 --> 00:00:09,590 Now we'll be starting Module 3. Going back to our concept map, we have 2 00:00:09,590 --> 00:00:14,760 finished the background module, the module on resistive circuits and now 3 00:00:14,760 --> 00:00:17,940 we're starting the module on reactive circuits. 4 00:00:17,940 --> 00:00:25,115 I'd like to stop and give you some background or some way of comparing 5 00:00:25,115 --> 00:00:29,610 resistive circuits to reactive circuits to teach you or motivate you why we 6 00:00:29,610 --> 00:00:33,100 want to study reactive circuits, and how it differs from resistive circuits. 7 00:00:34,280 --> 00:00:37,599 To do that, I'm going to show a experimental result. 8 00:00:39,000 --> 00:00:45,074 This is a display from an oscilloscope. Oscilloscope is a measuring device that 9 00:00:45,074 --> 00:00:51,595 shows voltages. Along the horizontal axis is time. 10 00:00:51,595 --> 00:00:57,361 So each division is a division in time. This particular one is milli-, in 11 00:00:57,361 --> 00:01:02,770 milliseconds, 1 millisecond [UNKNOWN] per division. 12 00:01:02,770 --> 00:01:08,490 The vertical axis is voltage. The green line shows the voltage source 13 00:01:08,490 --> 00:01:15,170 to resistive network. And in this case, it's going up and down. 14 00:01:15,170 --> 00:01:21,960 So here, it's at 1 volt, and then it goes down to minus 1 volt for 2.5 15 00:01:21,960 --> 00:01:25,660 milliseconds. Then it goes up to plus 1 volt and then 16 00:01:25,660 --> 00:01:30,690 back down to minus 1 volt. This is what's called the square wave. 17 00:01:30,690 --> 00:01:35,372 The blue line is the voltage across one of the resistors in that circuit. 18 00:01:35,372 --> 00:01:41,990 Notice how the voltage across the resistor is exactly in line and looks 19 00:01:41,990 --> 00:01:47,475 exactly the same as the voltage source except for the fact that it's scaled. 20 00:01:47,475 --> 00:01:51,415 And that's what it happens in a static circuit. 21 00:01:51,415 --> 00:01:57,580 The voltage output exactly matches the form, the shape of the voltage input. 22 00:01:57,580 --> 00:02:05,370 Now, a reactive circuit is different. In a reactor circuit, I've got, in this 23 00:02:05,370 --> 00:02:10,640 particular case, a capacitor in there. The voltage source looks the same but the 24 00:02:10,640 --> 00:02:14,830 response across any of the elements in that circuit looks different. 25 00:02:14,830 --> 00:02:17,480 It doesn't exactly match the shape. It's got some. 26 00:02:18,500 --> 00:02:23,830 Behavior to it. So this is equivalent, let's say in a 27 00:02:23,830 --> 00:02:28,670 physical system, having an object, a physical object. 28 00:02:28,670 --> 00:02:31,280 And it's got object, it's got inertia to it. 29 00:02:31,280 --> 00:02:34,220 And we want to push that object up to a certain speed. 30 00:02:34,220 --> 00:02:37,300 Well it takes you a while to get up to speed. 31 00:02:37,300 --> 00:02:38,800 And that's equivalent to what's happening here. 32 00:02:38,800 --> 00:02:42,095 It takes it a while to get up to the, the correct voltage. 33 00:02:42,095 --> 00:02:45,605 It doesn't happen instantaneously. And that's the difference between a 34 00:02:45,605 --> 00:02:50,220 resistive and a reactive circuit. And that basic behavior allows us to do a 35 00:02:50,220 --> 00:02:56,160 lot of very interesting designs in our circuit, so it has a lot of interesting 36 00:02:56,160 --> 00:02:58,620 behaviors. So, it's important for us to understand 37 00:02:58,620 --> 00:03:01,860 those behaviors. And to understand those behaviors, we're 38 00:03:01,860 --> 00:03:03,850 going to have to look at differential equations. 39 00:03:03,850 --> 00:03:07,930 And we'll give you some very basic background in differential equations 40 00:03:07,930 --> 00:03:15,480 during this module. Bringing back up the concept map. 41 00:03:15,480 --> 00:03:19,110 We've done the background in resistive circuits, and we're pulling some of those 42 00:03:19,110 --> 00:03:22,350 concepts forward into the reactive circuit module. 43 00:03:23,830 --> 00:03:29,060 In particular, the definitions of current and voltage, voltage sources, and current 44 00:03:29,060 --> 00:03:32,465 sources, and resistance were pulling forward from the background module. 45 00:03:32,465 --> 00:03:37,970 From the resistive circuit module, We're going to be utilizing those methods to 46 00:03:37,970 --> 00:03:41,596 obtain circuit equations. That includes Kirchhoff's Current Law, 47 00:03:41,596 --> 00:03:46,100 Kirchhoff's Voltage Law, mesh, node, and Thevenin equivalence. 48 00:03:46,100 --> 00:03:51,010 Everyone of those methods that we've already used are pertinent to the 49 00:03:51,010 --> 00:03:56,510 reactive circuits. The particular concepts we're going 50 00:03:56,510 --> 00:04:01,914 through in reactive circuits are capacitors and inductors, differential 51 00:04:01,914 --> 00:04:06,140 equations and I'm not assuming that you know differential equations by now. 52 00:04:06,140 --> 00:04:11,956 I'm only going to be using enough material to introduce to how to solve RC 53 00:04:11,956 --> 00:04:14,239 circuits and RL circuits.