1 00:00:01,000 --> 00:00:03,000 The following content is provided under a Creative 2 00:00:03,000 --> 00:00:05,000 Commons license. Your support will help MIT 3 00:00:05,000 --> 00:00:08,000 OpenCourseWare continue to offer high quality educational 4 00:00:08,000 --> 00:00:13,000 resources for free. To make a donation or to view 5 00:00:13,000 --> 00:00:18,000 additional materials from hundreds of MIT courses, 6 00:00:18,000 --> 00:00:23,000 visit MIT OpenCourseWare at ocw.mit.edu. 7 00:00:23,000 --> 00:00:32,000 Let's try to discuss a bit how things relate to physics. 8 00:00:32,000 --> 00:00:33,000 There are two main things I want to discuss. 9 00:00:33,000 --> 00:00:42,000 One of them is what curl says about force fields and, 10 00:00:42,000 --> 00:00:50,000 in particular,a nice consequence of that concerning 11 00:00:50,000 --> 00:00:56,000 gravitational attraction. More about curl. 12 00:00:56,000 --> 00:01:05,000 If we have a velocity field, then we have seen that the curl 13 00:01:05,000 --> 00:01:16,000 measures the rotation affects. More precisely curl v measures 14 00:01:16,000 --> 00:01:25,000 twice the angular velocity, or maybe I should say the 15 00:01:25,000 --> 00:01:31,000 angular velocity vector because it also includes the axis of 16 00:01:31,000 --> 00:01:38,000 rotation. I should say maybe for the 17 00:01:38,000 --> 00:01:48,000 rotation part of a motion. For example, 18 00:01:48,000 --> 00:01:58,000 just to remind you, I mean we have seen this guy a 19 00:01:58,000 --> 00:02:06,000 couple of times, but if I give you a uniform 20 00:02:06,000 --> 00:02:14,000 rotation motion about the z, axes. 21 00:02:14,000 --> 00:02:19,000 That is a vector field in which the trajectories are going to be 22 00:02:19,000 --> 00:02:23,000 circles centered in the z-axis and our vector field is just 23 00:02:23,000 --> 00:02:26,000 going to be tangent to each of these circles. 24 00:02:26,000 --> 00:02:35,000 And, if you look at it from above, then you will have this 25 00:02:35,000 --> 00:02:42,000 rotation vector field that we have seen many times. 26 00:02:42,000 --> 00:02:48,000 Typically, the velocity vector for this would be minus yi plus 27 00:02:48,000 --> 00:02:53,000 yj times maybe a number that represents how fast we are 28 00:02:53,000 --> 00:02:56,000 spinning, the angular velocity in 29 00:02:56,000 --> 00:03:01,000 gradients per second. And then. 30 00:03:01,000 --> 00:03:06,000 if you compute the curl of this, you will end up with two 31 00:03:06,000 --> 00:03:09,000 omega times k. Now, the other kinds of vector 32 00:03:09,000 --> 00:03:12,000 fields we have seen physically are force fields. 33 00:03:12,000 --> 00:03:17,000 The question is what does the curl of a force field mean? 34 00:03:17,000 --> 00:03:24,000 What can we say about that? The interpretation is a little 35 00:03:24,000 --> 00:03:34,000 bit less obvious, but let's try to get some idea 36 00:03:34,000 --> 00:03:42,000 of what it might be. I want to remind you that if we 37 00:03:42,000 --> 00:03:47,000 have a solid in a force field, we can measure the torque 38 00:03:47,000 --> 00:03:51,000 exerted by the force on the solid. 39 00:03:51,000 --> 00:03:55,000 Maybe first I should remind you about what torque is in space. 40 00:03:55,000 --> 00:03:59,000 Let's say that I have a piece of solid with a mass, 41 00:03:59,000 --> 00:04:03,000 delta m for example, and I have a force that is 42 00:04:03,000 --> 00:04:09,000 being exerted to it. Let's say that maybe my force 43 00:04:09,000 --> 00:04:14,000 might be F times delta m. If you think, 44 00:04:14,000 --> 00:04:16,000 for example, a gravitational field. 45 00:04:16,000 --> 00:04:20,000 The gravitational force is actually the gravitational field 46 00:04:20,000 --> 00:04:24,000 times the mass. I mean you can forget delta m 47 00:04:24,000 --> 00:04:29,000 if you don't like it. And let's say that the position 48 00:04:29,000 --> 00:04:33,000 vector, which should be aiming for the origin, 49 00:04:33,000 --> 00:04:37,000 R is here. And now let's say that maybe 50 00:04:37,000 --> 00:04:42,000 this guy is at the end of some arm or some metal thing and I 51 00:04:42,000 --> 00:04:46,000 want to hold it in place. The force is going to exert a 52 00:04:46,000 --> 00:04:50,000 torque relative to the origin that will try to measure how 53 00:04:50,000 --> 00:04:54,000 much I am trying to swing this guy around the origin. 54 00:04:54,000 --> 00:04:57,000 And, consequently, how much effort I have to exert 55 00:04:57,000 --> 00:05:02,000 if I want to actually maintain its place by just holding it at 56 00:05:02,000 --> 00:05:12,000 the end of the stick here. So the torque is now a vector, 57 00:05:12,000 --> 00:05:27,000 which is just the cross-product of a position vector with a 58 00:05:27,000 --> 00:05:31,000 force. What the torque measures again 59 00:05:31,000 --> 00:05:33,000 is the rotation effects of the force. 60 00:05:33,000 --> 00:05:39,000 And if you remember the principle that the derivative of 61 00:05:39,000 --> 00:05:42,000 velocity, which is acceleration, 62 00:05:42,000 --> 00:05:50,000 is force divided by mass then the derivative of angular 63 00:05:50,000 --> 00:05:58,000 velocity should be angular acceleration which is related to 64 00:05:58,000 --> 00:06:04,000 the torque per unit mass. To just remind you, 65 00:06:04,000 --> 00:06:06,000 if I look at translation motions, 66 00:06:06,000 --> 00:06:13,000 say I am just looking at the point mass so there are no 67 00:06:13,000 --> 00:06:21,000 rotation effects then force divided by mass is acceleration, 68 00:06:21,000 --> 00:06:28,000 which is the derivative of velocity. 69 00:06:28,000 --> 00:06:35,000 And so what I am claiming is that for rotation effects we 70 00:06:35,000 --> 00:06:40,000 have a similar law, which maybe you have seen in 71 00:06:40,000 --> 00:06:43,000 8.01. Well, it is one of the 72 00:06:43,000 --> 00:06:49,000 important things of solid mechanics, which is the torque 73 00:06:49,000 --> 00:06:53,000 of a force divided by the moment of inertia. 74 00:06:53,000 --> 00:06:57,000 I am cheating a little bit here. If you can see how I am 75 00:06:57,000 --> 00:07:00,000 cheating then I am sure you know how to state it correctly. 76 00:07:00,000 --> 00:07:06,000 And if you don't see how I am cheating then let's just ignore 77 00:07:06,000 --> 00:07:09,000 the details. [LAUGHTER] 78 00:07:09,000 --> 00:07:19,000 Is angular acceleration. And angular acceleration is the 79 00:07:19,000 --> 00:07:30,000 derivative of angular velocity. If I think of curl as an 80 00:07:30,000 --> 00:07:35,000 operation, which from a velocity field 81 00:07:35,000 --> 00:07:41,000 gives the angular velocity of its rotation effects, 82 00:07:41,000 --> 00:07:46,000 then you see that the curl of an acceleration field gives the 83 00:07:46,000 --> 00:07:49,000 angular acceleration in the rotation part of the 84 00:07:49,000 --> 00:07:53,000 acceleration effects. And, therefore, 85 00:07:53,000 --> 00:07:59,000 the curl of a force field measures the torque per unit 86 00:07:59,000 --> 00:08:04,000 moment of inertia. It measures how much torque its 87 00:08:04,000 --> 00:08:08,000 force field exerts on a small test solid placed in it. 88 00:08:08,000 --> 00:08:12,000 If you have a small solid somewhere, the curl will just 89 00:08:12,000 --> 00:08:16,000 measure how much your solid starts spinning if you leave it 90 00:08:16,000 --> 00:08:18,000 in this force field. In particular, 91 00:08:18,000 --> 00:08:22,000 a force field with no curl is a force field that does not 92 00:08:22,000 --> 00:08:26,000 generate any rotation motion. That means if you put an object 93 00:08:26,000 --> 00:08:29,000 in there that is completely immobile and you leave it in 94 00:08:29,000 --> 00:08:31,000 that force field, well, of course it might 95 00:08:31,000 --> 00:08:35,000 accelerate in some direction but it won't start spinning. 96 00:08:35,000 --> 00:08:38,000 While, if you put it in there spinning already in some 97 00:08:38,000 --> 00:08:41,000 direction, it should continue to spin in the same way. 98 00:08:41,000 --> 00:08:50,000 Of course, maybe there will be friction and things like that 99 00:08:50,000 --> 00:08:58,000 which will slow it down but this force field is not responsible 100 00:08:58,000 --> 00:09:05,000 for it. The cool consequence of this is 101 00:09:05,000 --> 00:09:14,000 if a force field F derives from a potential -- That is what we 102 00:09:14,000 --> 00:09:20,000 have seen about conservative forces. 103 00:09:20,000 --> 00:09:23,000 Our main concern so far has been to say if we have a 104 00:09:23,000 --> 00:09:26,000 conservative force field it means that the work of a force 105 00:09:26,000 --> 00:09:29,000 is the change in the energy. And, in particular, 106 00:09:29,000 --> 00:09:32,000 we cannot get energy for free out of it. 107 00:09:32,000 --> 00:09:36,000 And the change in the potential energy is going to be the change 108 00:09:36,000 --> 00:09:40,000 in kinetic energy. You have conservation of energy 109 00:09:40,000 --> 00:09:43,000 principles. There is another thing that we 110 00:09:43,000 --> 00:09:48,000 know now because if a force derives from a potential then 111 00:09:48,000 --> 00:09:53,000 that means its curl is zero. That is the criterion we have 112 00:09:53,000 --> 00:09:58,000 seen for a vector field to derive from a potential. 113 00:09:58,000 --> 00:10:14,000 And if the curl is zero then it means that this force does not 114 00:10:14,000 --> 00:10:23,000 generate any rotation effects. For example, 115 00:10:23,000 --> 00:10:27,000 if you try to understand where the earth comes from, 116 00:10:27,000 --> 00:10:32,000 well, the earth is spinning on itself as it goes around the 117 00:10:32,000 --> 00:10:35,000 sun. And you might wonder where that 118 00:10:35,000 --> 00:10:37,000 comes from. Is that causes by gravitational 119 00:10:37,000 --> 00:10:40,000 attraction? And the answer is no. 120 00:10:40,000 --> 00:10:44,000 Gravitational attraction in itself cannot cause the earth to 121 00:10:44,000 --> 00:10:47,000 start spinning faster or slower, at least if you assume the 122 00:10:47,000 --> 00:10:52,000 earth to be a solid, which actually is false. 123 00:10:52,000 --> 00:10:57,000 I mean basically the reason why the earth is spinning is because 124 00:10:57,000 --> 00:11:01,000 it was formed spinning. It didn't start spinning 125 00:11:01,000 --> 00:11:03,000 because of gravitational effects. 126 00:11:03,000 --> 00:11:08,000 And that is a rather deep purely mathematical consequence 127 00:11:08,000 --> 00:11:12,000 of understanding gravitation in this way. 128 00:11:12,000 --> 00:11:16,000 It is quite spectacular that just by abstract thinking we got 129 00:11:16,000 --> 00:11:17,000 there. What is the truth? 130 00:11:17,000 --> 00:11:21,000 Well, the truth is the earth, the moon and everything is 131 00:11:21,000 --> 00:11:24,000 slightly deformable. And so there is deformation, 132 00:11:24,000 --> 00:11:26,000 friction effects, tidal effects and so on. 133 00:11:26,000 --> 00:11:29,000 And these actually cause rotations to get slightly 134 00:11:29,000 --> 00:11:32,000 synchronized with each other. For example, 135 00:11:32,000 --> 00:11:36,000 if you want to explain why the moon is always showing the same 136 00:11:36,000 --> 00:11:39,000 face to the earth, why the rotation of a moon on 137 00:11:39,000 --> 00:11:43,000 itself is synchronized with its revolution around the earth, 138 00:11:43,000 --> 00:11:47,000 which is actually explained by friction effects over time and 139 00:11:47,000 --> 00:11:50,000 the gravitational attraction of the earth and the moon. 140 00:11:50,000 --> 00:11:59,000 There is something there, but if you took perfectly 141 00:11:59,000 --> 00:12:09,000 rigid, solid bodies then gravitation would never cause 142 00:12:09,000 --> 00:12:15,000 any rotation effects. Of course that tells us that we 143 00:12:15,000 --> 00:12:20,000 do not know how to answer the question of why is the earth 144 00:12:20,000 --> 00:12:22,000 spinning. That will be left for another 145 00:12:22,000 --> 00:12:31,000 physics class. I don't have a good answer to 146 00:12:31,000 --> 00:12:35,000 that. That was kind of 8.01-ish. 147 00:12:35,000 --> 00:12:40,000 Let me now move forward to 8.02 stuff. 148 00:12:40,000 --> 00:12:54,000 I want to tell you things about electric and magnetic fields. 149 00:12:54,000 --> 00:13:01,000 And, in fact, something that is known as 150 00:13:01,000 --> 00:13:06,000 Maxwell's equations. Just a quick poll. 151 00:13:06,000 --> 00:13:10,000 How many of you have been taking 8.02 or something like 152 00:13:10,000 --> 00:13:13,000 that? OK. That is not very many. 153 00:13:13,000 --> 00:13:15,000 For most of you this is a preview. 154 00:13:15,000 --> 00:13:18,000 If you have been taking 8.02, have you seen Maxwell's 155 00:13:18,000 --> 00:13:20,000 equations, at least part of them? 156 00:13:20,000 --> 00:13:22,000 Yeah. OK. 157 00:13:22,000 --> 00:13:23,000 Then I am sure, in that case, 158 00:13:23,000 --> 00:13:25,000 you know better than me what I am going to talk about because I 159 00:13:25,000 --> 00:13:30,000 am not a physicist. But just in case. 160 00:13:30,000 --> 00:13:35,000 Maxwell's equations govern how electric and magnetic fields 161 00:13:35,000 --> 00:13:39,000 behave, how they are caused by electric charges and their 162 00:13:39,000 --> 00:13:41,000 motions. And, in particular, 163 00:13:41,000 --> 00:13:45,000 they explain a lot of things such as how electric devices 164 00:13:45,000 --> 00:13:49,000 work, but also how electromagnetic waves propagate. 165 00:13:49,000 --> 00:13:54,000 In particular, that explains light and all 166 00:13:54,000 --> 00:13:58,000 sorts of waves. It is thanks to them, 167 00:13:58,000 --> 00:14:02,000 you know, your cell phone, laptops and things like that 168 00:14:02,000 --> 00:14:06,000 work. Anyway. 169 00:14:06,000 --> 00:14:11,000 Hopefully most of you know that the electric field is a vector 170 00:14:11,000 --> 00:14:14,000 field that basically tells you what kind of force will be 171 00:14:14,000 --> 00:14:18,000 exerted on a charged particle that you put in it. 172 00:14:18,000 --> 00:14:23,000 If you have a particle carrying an electric charge then this 173 00:14:23,000 --> 00:14:27,000 vector field will tell you, basically there will be an 174 00:14:27,000 --> 00:14:31,000 electric force which is the charge times E that will be 175 00:14:31,000 --> 00:14:33,000 exerted on that particle. And that is what is 176 00:14:33,000 --> 00:14:36,000 responsible, for example, for the flow of electrons when 177 00:14:36,000 --> 00:14:41,000 you have a voltage difference. Because classically this guy is 178 00:14:41,000 --> 00:14:45,000 a gradient of a potential. And that potential is just 179 00:14:45,000 --> 00:14:50,000 electric voltage. The magnetic field is a little 180 00:14:50,000 --> 00:14:55,000 bit harder to think about if you have never seen it in physics, 181 00:14:55,000 --> 00:15:00,000 but it is what is causing, for example, 182 00:15:00,000 --> 00:15:04,000 magnets to work. Well, basically it is a force 183 00:15:04,000 --> 00:15:09,000 that is also expressed in terms of a vector field usually called 184 00:15:09,000 --> 00:15:12,000 B. Some people call it H but I am 185 00:15:12,000 --> 00:15:15,000 going to use B. And that force tends to cause 186 00:15:15,000 --> 00:15:20,000 it, if you have a moving charged particle, to deflect its 187 00:15:20,000 --> 00:15:24,000 trajectory and start rotating in a magnetic field. 188 00:15:24,000 --> 00:15:32,000 What it does is not quite as easy as what an electric field 189 00:15:32,000 --> 00:15:35,000 does. Just to give you formulas, 190 00:15:35,000 --> 00:15:39,000 the force caused by the electric field is the charge 191 00:15:39,000 --> 00:15:43,000 times the electric field. And the force caused by the 192 00:15:43,000 --> 00:15:47,000 magnetic field, I am never sure about the sign. 193 00:15:47,000 --> 00:15:52,000 Is that the correct sign? Good. 194 00:15:52,000 --> 00:15:56,000 Now, the question is we need to understand how these fields 195 00:15:56,000 --> 00:16:00,000 themselves are caused by the charged particles that are 196 00:16:00,000 --> 00:16:03,000 placed in them. There are various laws in there 197 00:16:03,000 --> 00:16:11,000 that explain what is going on. Let me focus today on the 198 00:16:11,000 --> 00:16:17,000 electric field. Maxwell's equations actually 199 00:16:17,000 --> 00:16:22,000 tell you about div and curl of these fields. 200 00:16:22,000 --> 00:16:27,000 Let's look at div and curl of the electric field. 201 00:16:27,000 --> 00:16:37,000 The first equation is called the Gauss-Coulomb law. 202 00:16:37,000 --> 00:16:47,000 And it says that the divergence of the electric field is equal 203 00:16:47,000 --> 00:16:51,000 to, so this is a just a physical 204 00:16:51,000 --> 00:16:54,000 constant, and what it is equal to depends 205 00:16:54,000 --> 00:16:57,000 on what units you are using. And this guy rho, 206 00:16:57,000 --> 00:17:01,000 well, it is not the same rho as in spherical coordinates because 207 00:17:01,000 --> 00:17:06,000 physicists somehow pretended they used that letter first. 208 00:17:06,000 --> 00:17:08,000 It is the electric charge density. 209 00:17:08,000 --> 00:17:15,000 It is the amount of electric charge per unit volume. 210 00:17:15,000 --> 00:17:20,000 What this tells you is that divergence of E is caused by the 211 00:17:20,000 --> 00:17:23,000 presence of electric charge. In particular, 212 00:17:23,000 --> 00:17:29,000 if you have an empty region of space or a region where nothing 213 00:17:29,000 --> 00:17:34,000 has electrical charge then E has divergence equal to zero. 214 00:17:34,000 --> 00:17:38,000 Now, that looks like a very abstract strange equation. 215 00:17:38,000 --> 00:17:43,000 I mean it is a partial differential equation satisfied 216 00:17:43,000 --> 00:17:49,000 by the electric field E. And that is not very intuitive 217 00:17:49,000 --> 00:17:56,000 in any way. What is actually more intuitive 218 00:17:56,000 --> 00:18:05,000 is what we get if we apply the divergence theorem to this 219 00:18:05,000 --> 00:18:11,000 equation. If I think now about any closed 220 00:18:11,000 --> 00:18:16,000 surface, and I want to think about the 221 00:18:16,000 --> 00:18:21,000 flux of the electric field out of that surface, 222 00:18:21,000 --> 00:18:24,000 we haven't really thought about what the flux of a force field 223 00:18:24,000 --> 00:18:27,000 does. And I don't want to get into 224 00:18:27,000 --> 00:18:31,000 that because there is no very easy answer in general, 225 00:18:31,000 --> 00:18:35,000 but I am going to explain soon how this can be useful 226 00:18:35,000 --> 00:18:38,000 sometimes. Let's say that we want to find 227 00:18:38,000 --> 00:18:43,000 the flux of the electric field out of a closed surface. 228 00:18:43,000 --> 00:18:47,000 Then, by the divergence theorem, 229 00:18:47,000 --> 00:18:53,000 that is equal to the triple integral of a region inside of 230 00:18:53,000 --> 00:18:57,000 div E dV, which is by the equation one 231 00:18:57,000 --> 00:19:00,000 over epsilon zero, that is this constant, 232 00:19:00,000 --> 00:19:06,000 times the triple integral of rho dV. 233 00:19:06,000 --> 00:19:09,000 But now, if I integrate the charge density over the entire 234 00:19:09,000 --> 00:19:12,000 region, then what I will get is 235 00:19:12,000 --> 00:19:17,000 actually the total amount of electric charge inside the 236 00:19:17,000 --> 00:19:28,000 region. That is the electric charge in 237 00:19:28,000 --> 00:19:31,000 D. This one tells us, 238 00:19:31,000 --> 00:19:34,000 in a more concrete way, how electric charges placed in 239 00:19:34,000 --> 00:19:38,000 here influence the electric field around them. 240 00:19:38,000 --> 00:19:40,000 In particular, one application of that is if 241 00:19:40,000 --> 00:19:43,000 you want to study capacitors. Capacitors are these things 242 00:19:43,000 --> 00:19:46,000 that store energy by basically you have two plates, 243 00:19:46,000 --> 00:19:49,000 one that contains positive charge and a negative charge. 244 00:19:49,000 --> 00:19:52,000 Then you have a voltage between these plates. 245 00:19:52,000 --> 00:19:57,000 And, basically, that can provide electrical 246 00:19:57,000 --> 00:20:03,000 energy to power maybe an electric circuit. 247 00:20:03,000 --> 00:20:06,000 That is not really a battery because it doesn't store energy 248 00:20:06,000 --> 00:20:08,000 in large enough amounts. But, for example, 249 00:20:08,000 --> 00:20:11,000 that is why when you switch your favorite gadget off it 250 00:20:11,000 --> 00:20:14,000 doesn't actually go off immediately but somehow you see 251 00:20:14,000 --> 00:20:18,000 things dimming progressively. There is a capacitor in there. 252 00:20:18,000 --> 00:20:20,000 If you want to understand how the voltage and the charge 253 00:20:20,000 --> 00:20:23,000 relate to each other, the voltage is obtained by 254 00:20:23,000 --> 00:20:26,000 integrating the electric field from one plate to the other 255 00:20:26,000 --> 00:20:29,000 plate. And the charges in the plates 256 00:20:29,000 --> 00:20:34,000 are what causes the electric field between the plates. 257 00:20:34,000 --> 00:20:37,000 That is how you can get the relation between voltage and 258 00:20:37,000 --> 00:20:41,000 charge in these guys. That is an example of 259 00:20:41,000 --> 00:20:44,000 application of that. Now, of course, 260 00:20:44,000 --> 00:20:49,000 if you haven't seen any of this then maybe it is a little bit 261 00:20:49,000 --> 00:20:54,000 esoteric, but that will tell you part of what you will see in 262 00:20:54,000 --> 00:20:59,000 8.02. Questions? 263 00:20:59,000 --> 00:21:07,000 I see some confused faces. Well, don't worry. 264 00:21:07,000 --> 00:21:14,000 It will make sense some day. [LAUGHTER] 265 00:21:14,000 --> 00:21:23,000 The next one I want to tell you about is Faraday's law. 266 00:21:23,000 --> 00:21:25,000 In case you are confused, Maxwell's equations, 267 00:21:25,000 --> 00:21:29,000 there are four equations in the set of Maxwell's equations and 268 00:21:29,000 --> 00:21:31,000 most of them don't carry Maxwell's name. 269 00:21:31,000 --> 00:21:40,000 That is a quirky feature. That one tells you about the 270 00:21:40,000 --> 00:21:44,000 curl of the electric field. Now, depending on your 271 00:21:44,000 --> 00:21:46,000 knowledge, you might start telling me that 272 00:21:46,000 --> 00:21:50,000 the curl of the electric field has to be zero because it is the 273 00:21:50,000 --> 00:21:52,000 gradient of the electric potential. 274 00:21:52,000 --> 00:21:54,000 I told you this stuff about voltage. 275 00:21:54,000 --> 00:21:58,000 Well, that doesn't account for the fact that sometimes you can 276 00:21:58,000 --> 00:22:02,000 create voltage out of nowhere using magnetic fields. 277 00:22:02,000 --> 00:22:05,000 And, in fact, you have a failure of 278 00:22:05,000 --> 00:22:09,000 conservativity of the electric force if you have a magnetic 279 00:22:09,000 --> 00:22:12,000 field. What this one says is the curl 280 00:22:12,000 --> 00:22:17,000 of E is not zero but rather it is the derivative of the 281 00:22:17,000 --> 00:22:21,000 magnetic field with respect to time. 282 00:22:21,000 --> 00:22:26,000 More precisely it tells you that what you might have learned 283 00:22:26,000 --> 00:22:31,000 about electric fields deriving from electric potential becomes 284 00:22:31,000 --> 00:22:35,000 false if you have a variable magnetic field. 285 00:22:35,000 --> 00:22:41,000 And just to tell you again that is a strange partial 286 00:22:41,000 --> 00:22:47,000 differential equation relating these two vector fields. 287 00:22:47,000 --> 00:22:51,000 To make sense of it one should use Stokes' theorem. 288 00:22:51,000 --> 00:22:56,000 If we apply Stokes' theorem to compute the work done by the 289 00:22:56,000 --> 00:23:00,000 electric field around a closed curve, 290 00:23:00,000 --> 00:23:04,000 that means you have a wire in there and you want to find the 291 00:23:04,000 --> 00:23:07,000 voltage along the wire. Now there is a strange thing 292 00:23:07,000 --> 00:23:10,000 because classically you would say, well, if I just have a wire 293 00:23:10,000 --> 00:23:13,000 with nothing in it there is no voltage on it. 294 00:23:13,000 --> 00:23:18,000 Well, a small change in plans. If you actually have a varying 295 00:23:18,000 --> 00:23:23,000 magnetic field that passes through that wire then that will 296 00:23:23,000 --> 00:23:31,000 actually generate voltage in it. That is how a transformer works. 297 00:23:31,000 --> 00:23:34,000 When you plug your laptop into the wall circuit, 298 00:23:34,000 --> 00:23:36,000 you don't actually feed it directly 110 volts, 299 00:23:36,000 --> 00:23:40,000 120 volts or whatever. There is a transformer in there. 300 00:23:40,000 --> 00:23:45,000 What the transformer does it takes some input voltage and 301 00:23:45,000 --> 00:23:49,000 passes that through basically a loop of wire. 302 00:23:49,000 --> 00:23:53,000 Not much seems to be happening. But now you have another loops 303 00:23:53,000 --> 00:23:56,000 of wire that is intertwined with it. 304 00:23:56,000 --> 00:23:59,000 Somehow the magnetic field generated by it, 305 00:23:59,000 --> 00:24:03,000 and it has to be a donating current. 306 00:24:03,000 --> 00:24:06,000 The donating current varies over time in the first wire. 307 00:24:06,000 --> 00:24:09,000 That generates a magnetic field that varies over time, 308 00:24:09,000 --> 00:24:13,000 so that causes 2B by 2t and that causes curl of the electric 309 00:24:13,000 --> 00:24:15,000 field. And the curl of the electric 310 00:24:15,000 --> 00:24:18,000 field will generate voltage between these two guys. 311 00:24:18,000 --> 00:24:21,000 And that is how a transformer works. 312 00:24:21,000 --> 00:24:25,000 It uses Stokes' theorem. More precisely, 313 00:24:25,000 --> 00:24:28,000 how do we find the voltage between these two points? 314 00:24:28,000 --> 00:24:32,000 Well, let's close the loop and let's try to figure out the 315 00:24:32,000 --> 00:24:37,000 voltage inside this loop. To find a voltage along a 316 00:24:37,000 --> 00:24:42,000 closed curve places in a varying magnetic field, 317 00:24:42,000 --> 00:24:47,000 we have to do the line integral along a closed curve of the 318 00:24:47,000 --> 00:24:51,000 electric field. And you should think of this as 319 00:24:51,000 --> 00:24:54,000 the voltage generated in this circuit. 320 00:24:54,000 --> 00:25:05,000 That will be the flux for this surface bounded by the curve of 321 00:25:05,000 --> 00:25:11,000 curl E dot dS. That is what Stokes' theorem 322 00:25:11,000 --> 00:25:14,000 says. And now if you combine that 323 00:25:14,000 --> 00:25:21,000 with Faraday's law you end up with the flux trough S of minus 324 00:25:21,000 --> 00:25:25,000 dB over dt. And, of course, you could take, 325 00:25:25,000 --> 00:25:27,000 if your loop doesn't move over time, 326 00:25:27,000 --> 00:25:31,000 I mean there is a different story if you start somehow 327 00:25:31,000 --> 00:25:34,000 taking your wire and somehow moving it inside the field. 328 00:25:34,000 --> 00:25:37,000 But if you don't do that, if it is the field that is 329 00:25:37,000 --> 00:25:40,000 moving then you just can take the dB by dt outside. 330 00:25:40,000 --> 00:25:48,000 But let's not bother. Again, what this equation tells 331 00:25:48,000 --> 00:25:52,000 you is that if the magnetic field changes over time then it 332 00:25:52,000 --> 00:25:55,000 creates, just out of nowhere, and electric field. 333 00:25:55,000 --> 00:26:09,000 And that electric field can be used to power up things. 334 00:26:09,000 --> 00:26:11,000 I don't really claim that I have given you enough details to 335 00:26:11,000 --> 00:26:15,000 understand how they work, but basically these equations 336 00:26:15,000 --> 00:26:20,000 are the heart of understanding how things like capacitors and 337 00:26:20,000 --> 00:26:23,000 transformers work. And they also explain a lot of 338 00:26:23,000 --> 00:26:25,000 other things, but I will leave that to your 339 00:26:25,000 --> 00:26:28,000 physics teachers. Just for completeness, 340 00:26:28,000 --> 00:26:33,000 I will just give you the last two equations in that. 341 00:26:33,000 --> 00:26:37,000 I am not even going to try to explain them too much. 342 00:26:37,000 --> 00:26:42,000 One of them says that the divergence of the magnetic field 343 00:26:42,000 --> 00:26:45,000 is zero, which somehow is fortunate 344 00:26:45,000 --> 00:26:49,000 because otherwise you would run into trouble trying to 345 00:26:49,000 --> 00:26:53,000 understand surface independence when you apply Stokes' theorem 346 00:26:53,000 --> 00:26:58,000 in here. And the last one tells you how 347 00:26:58,000 --> 00:27:04,000 the curl of the magnetic field is caused by motion of charged 348 00:27:04,000 --> 00:27:09,000 particles. In fact, let's say that the 349 00:27:09,000 --> 00:27:16,000 curl of B is given by this kind of formula, well, 350 00:27:16,000 --> 00:27:23,000 J is what is called the vector of current density. 351 00:27:23,000 --> 00:27:30,000 It measures the flow of electrically charged particles. 352 00:27:30,000 --> 00:27:34,000 You get this guy when you start taking charged particles, 353 00:27:34,000 --> 00:27:38,000 like electrons maybe, and moving them around. 354 00:27:38,000 --> 00:27:40,000 And, of course, that is actually part of how 355 00:27:40,000 --> 00:27:44,000 transformers work because I have told you running the AC through 356 00:27:44,000 --> 00:27:46,000 the first loop generates a magnetic field. 357 00:27:46,000 --> 00:27:49,000 Well, how does it do that? It is thanks to this equation. 358 00:27:49,000 --> 00:27:52,000 If you have a current passing in the loop that causes a 359 00:27:52,000 --> 00:27:54,000 magnetic field and, in turn, for the other equation 360 00:27:54,000 --> 00:27:59,000 that causes an electric field, which in turn causes a current. 361 00:27:59,000 --> 00:28:08,000 It is all somehow intertwined in a very intricate way and is 362 00:28:08,000 --> 00:28:15,000 really remarkable how well that works in practice. 363 00:28:15,000 --> 00:28:17,000 I think that is basically all I wanted to say about 8.02. 364 00:28:17,000 --> 00:28:23,000 I don't want to put your physics teachers out of a job. 365 00:28:23,000 --> 00:28:24,000 [LAUGHTER] If you haven't seen any of this 366 00:28:24,000 --> 00:28:26,000 before, I understand that this is 367 00:28:26,000 --> 00:28:28,000 probably not detailed enough to be really understandable, 368 00:28:28,000 --> 00:28:32,000 but hopefully it will make you a bit curious about that and 369 00:28:32,000 --> 00:28:36,000 prompt you to take that class someday and maybe even remember 370 00:28:36,000 --> 00:28:39,000 how it relates to 18.02.