1 00:00:01,840 --> 00:00:03,760 Welcome back, this is Dr. Ferry. 2 00:00:05,230 --> 00:00:10,090 This lesson will be on a lab demo, The Applications of Inductance. 3 00:00:11,520 --> 00:00:15,890 So far in this module, we've talked about the theoretical aspects. 4 00:00:15,890 --> 00:00:19,410 We've learned how to analyze circuits with capacitors, inductors. 5 00:00:19,410 --> 00:00:23,300 And it's a nice way of ending out this module, is to look at some physical 6 00:00:23,300 --> 00:00:27,595 applications of inductors and capacitors. We've already done a lab demo on 7 00:00:27,595 --> 00:00:31,150 capacitors. So now this time, we'll be doing a lab 8 00:00:31,150 --> 00:00:36,725 demo on the applications of inductors and inductance. 9 00:00:36,725 --> 00:00:40,510 Now let's [INAUDIBLE] look at some applications of inductance. 10 00:00:40,510 --> 00:00:43,465 An inductor is just basically a coil of wire. 11 00:00:43,465 --> 00:00:48,514 Inductors are really common. And they're used in power generation, 12 00:00:48,514 --> 00:00:53,710 inductive sensors, and in inductive actuators. 13 00:00:53,710 --> 00:00:57,680 The basic mechanism to generate electricity is by moving a coil inside of 14 00:00:57,680 --> 00:01:02,160 a magnetic field or by moving the magnetic field [INAUDIBLE] a coil. 15 00:01:02,160 --> 00:01:09,760 A guitar pickup uses, the electric guitar pickup uses this sort of principle. 16 00:01:09,760 --> 00:01:15,870 In that case, the electric guitar pickup has a permanent magnet, as shown here. 17 00:01:15,870 --> 00:01:19,637 We've got a permanent magnet and a coil of wire wrapped around it. 18 00:01:19,637 --> 00:01:25,530 And it generates a magnetic field because of that permanent magnet. 19 00:01:25,530 --> 00:01:30,510 If I take I it in a conductor like a guitar, metal guitar string and I cross 20 00:01:30,510 --> 00:01:35,240 through those lines, I'm going to generate current in this coil. 21 00:01:39,440 --> 00:01:46,270 Now, let's take a look at a kind of a simple experiment to show a homemade 22 00:01:46,270 --> 00:01:49,360 guitar pickup. This is a homemade guitar pickup. 23 00:01:49,360 --> 00:01:54,340 It is just a bunch of wire coiled around, very fine gauge wire, coiled around a 24 00:01:54,340 --> 00:01:58,090 permanent magnet. And it creates magnetic field about it. 25 00:01:58,090 --> 00:02:02,980 And this is a metal guitar string. As I pluck it [SOUND] then it cuts those 26 00:02:02,980 --> 00:02:08,460 magnetic lines and it creates a voltage. Now this line showing out here, this is 27 00:02:08,460 --> 00:02:11,920 connected to oscilloscope. So the only electricity that's going on 28 00:02:11,920 --> 00:02:13,480 here is the one that I'm generating. [SOUND]. 29 00:02:13,480 --> 00:02:22,457 There's no external power supply here. If I look at the oscilloscope, as I pluck 30 00:02:22,457 --> 00:02:25,190 this [SOUND] you can see the generated voltage. 31 00:02:25,190 --> 00:02:31,370 [SOUND]. And that's how guitar pickups work. 32 00:02:31,370 --> 00:02:38,840 They're just sensors made of this induction, inductive element. 33 00:02:38,840 --> 00:02:43,160 Now this is a passive sensor, looking back at this experiment here. 34 00:02:43,160 --> 00:02:45,780 This is a passive sensor. As I said, there's no external power 35 00:02:45,780 --> 00:02:49,280 supply. Active sensors, which have their own 36 00:02:49,280 --> 00:02:55,616 power supply, are often used in metal detectors and in inductive proximity 37 00:02:55,616 --> 00:03:00,331 sensors. Going back to this drawing here, they act 38 00:03:00,331 --> 00:03:06,460 as sensors, have a current flowing through this because of the power supply. 39 00:03:06,460 --> 00:03:08,510 So they've got current flowing through this. 40 00:03:08,510 --> 00:03:11,500 And that generates this electric field or magnetic field. 41 00:03:11,500 --> 00:03:16,200 And, in fact, if you have a changing voltage or, changing current through 42 00:03:16,200 --> 00:03:18,510 here, it's going to have a changing magnetic field. 43 00:03:19,790 --> 00:03:23,790 When that comes in contact with a metallic object, it interacts with this 44 00:03:23,790 --> 00:03:28,180 field, which then changes the current flow in the coil. 45 00:03:28,180 --> 00:03:32,500 And there's a circuitry attached to that that detects that change in the current. 46 00:03:32,500 --> 00:03:38,930 A very common inductive sensor that you'll see in applications is metal 47 00:03:38,930 --> 00:03:41,974 detectors. Metal detectors of the kind of portable 48 00:03:41,974 --> 00:03:46,380 type that you can find metal on beaches, but also metal detectors that are in 49 00:03:46,380 --> 00:03:50,390 stores and events when you have to walk through the metal detector to get in. 50 00:03:50,390 --> 00:03:55,620 It's just a magnetic field that you're walking through, and the metal disrupts 51 00:03:55,620 --> 00:03:59,110 that magnetic field which then, again, disrupts the current generating that 52 00:03:59,110 --> 00:04:05,210 magnetic field. A very common inductive sensor in 53 00:04:05,210 --> 00:04:09,182 mechanical systems is a linear variable differential transformer, an LVDT. 54 00:04:09,182 --> 00:04:14,400 That's that's a case where I've got a primary coil and in addition, I'm going 55 00:04:14,400 --> 00:04:17,420 to have a secondary coil. And this is used to measure linear 56 00:04:17,420 --> 00:04:25,640 displacement in mechanical applications. Now, inductive actuators, are ones that 57 00:04:25,640 --> 00:04:28,930 drive mechanical devices. They rely on the principle of 58 00:04:28,930 --> 00:04:32,898 electromagnet, which is again a coil with a current flowing through it. 59 00:04:32,898 --> 00:04:38,780 If I just have just the basic coil with a current flowing through it, it generates 60 00:04:38,780 --> 00:04:41,920 a magnetic field. The stronger the current, the stronger 61 00:04:41,920 --> 00:04:44,900 the magnetic field. And that means I've created a magnet, an 62 00:04:44,900 --> 00:04:50,760 electromagnet. [SOUND] This is an example of 63 00:04:50,760 --> 00:04:53,290 electromagnet. I've got two leads here. 64 00:04:53,290 --> 00:04:59,700 I hook up these leads to a power supply and inside here is a coil of, of wire. 65 00:04:59,700 --> 00:05:03,890 And this, when they, current going through that coil gets large enough, the 66 00:05:03,890 --> 00:05:06,272 magnetic field gets large enough, it becomes a magnet. 67 00:05:06,272 --> 00:05:12,010 A solenoid is a electromagnet which has a core that goes into it. 68 00:05:13,530 --> 00:05:19,630 And that core is pulled in when the electromagnet, magnetic field gets large 69 00:05:19,630 --> 00:05:22,590 enough. So when the current gets large enough, 70 00:05:22,590 --> 00:05:25,030 magnetic field gets strong enough, it pulls this in. 71 00:05:26,280 --> 00:05:28,450 Now this right here is just a mechanical spring. 72 00:05:28,450 --> 00:05:32,460 And it's used to provide a restoring force because when the current gets low 73 00:05:32,460 --> 00:05:39,390 enough then the magnetic field drops, but I need a restoring force to push it back 74 00:05:39,390 --> 00:05:42,900 out. So the magnetic, the magnetic field pulls 75 00:05:42,900 --> 00:05:46,495 it in. The spring pushes it back out. 76 00:05:46,495 --> 00:05:52,884 [SOUND] Let's see the operation of a magnetic, of a solenoid. 77 00:05:52,884 --> 00:05:58,560 Solenoids are often times used as valves to open and close valves. 78 00:05:58,560 --> 00:06:03,140 Now this is one that I've got hooked up to a power supply and I'm going to turn 79 00:06:03,140 --> 00:06:05,705 this. Let me hold my finger on it to, because 80 00:06:05,705 --> 00:06:09,230 it's going to move. I'm increasing the voltage this and, 81 00:06:09,230 --> 00:06:15,324 thereby, increasing the current. [SOUND] And this one I got to about 14, 82 00:06:15,324 --> 00:06:19,180 15 volts. It reached half an amp, which is quite a 83 00:06:19,180 --> 00:06:21,920 bit. And the half an amp, it's large enough, a 84 00:06:21,920 --> 00:06:25,870 strong enough magnetic field, that it pulled that shaft inward. 85 00:06:25,870 --> 00:06:29,600 If I drop the current, the [INAUDIBLE] voltage and current through this, 86 00:06:29,600 --> 00:06:37,830 [BLANK_AUDIO] at some point in time the, the spring force is large enough to pull 87 00:06:37,830 --> 00:06:41,820 it back out. So that is a solenoid, oftentimes used 88 00:06:41,820 --> 00:06:50,595 as, to open and close valves. [SOUND] Another example of an 89 00:06:50,595 --> 00:06:54,950 electromagnet is in a loudspeaker. This is a cross-sectional area of a 90 00:06:54,950 --> 00:06:58,735 loudspeaker. It's cut in half. 91 00:06:58,735 --> 00:07:04,260 And this is a coil that's in there. So the coil is also cut in half. 92 00:07:04,260 --> 00:07:09,760 You can see the inside of the coil. So the coil of wire is right there. 93 00:07:09,760 --> 00:07:12,936 You can see it, a full one looking right there. 94 00:07:12,936 --> 00:07:19,680 And there's a diaphragm or cone attached to the electromagnet. 95 00:07:19,680 --> 00:07:24,830 And the electromagnet reverses polarity depending on how you, what the current is 96 00:07:24,830 --> 00:07:27,020 like going through these coils, through the coil. 97 00:07:27,020 --> 00:07:31,930 It reverses polarity, pushing against or pulling the diaphragm towards a 98 00:07:31,930 --> 00:07:37,770 [INAUDIBLE] permanent magnet. So as you reverse the polarity of the 99 00:07:37,770 --> 00:07:43,070 current going through that, that, coil, it's going to push or pull this speaker 100 00:07:43,070 --> 00:07:47,538 inward and outward, this diaphragm. And, therefore, it creates the sound. 101 00:07:47,538 --> 00:07:55,060 So that's a good application of of inductance. 102 00:07:55,060 --> 00:08:01,330 So we've looked at inductance with respect to sensors, as well as actuators. 103 00:08:04,440 --> 00:08:09,580 In summary, we discussed the energy exchange in inductors, from mechanical 104 00:08:09,580 --> 00:08:13,130 energy to electrical, and from electrical to mechanical energy. 105 00:08:14,900 --> 00:08:20,110 And that was done all through inductors. We also shared that moving a conductor in 106 00:08:20,110 --> 00:08:25,240 a magnetic field induces current. And changing current in a coiled wire 107 00:08:25,240 --> 00:08:31,860 causes a magnetic field. And we use these properties to be able to 108 00:08:31,860 --> 00:08:37,010 build applications with inductance. We looked at passive sensing, such as, in 109 00:08:37,010 --> 00:08:40,350 a guitar pickup. We looked at active sensing, such as 110 00:08:40,350 --> 00:08:43,518 metal detector. And we also looked at actuation through 111 00:08:43,518 --> 00:08:46,180 the, the usage of solenoids with speakers. 112 00:08:46,180 --> 00:08:52,508 I like to remind people to go to the forum and ask questions as you need, 113 00:08:52,508 --> 00:08:59,676 answer questions that other people, post. And you might want to start a new forum 114 00:08:59,676 --> 00:09:06,790 topic that is applications of inductors and capacitors that you're familiar with. 115 00:09:06,790 --> 00:09:08,100 Thank you and I'll see you online.