1 00:00:00,389 --> 00:00:01,654 - [Voiceover] What I wanna do in this video 2 00:00:01,654 --> 00:00:03,384 is give ourselves an introduction 3 00:00:03,384 --> 00:00:07,389 or an intuition for the term Flux in general. 4 00:00:07,389 --> 00:00:09,189 And then think about how it applies 5 00:00:09,189 --> 00:00:12,091 to the idea of magnetic 6 00:00:12,091 --> 00:00:14,646 Magnetic Flux. 7 00:00:14,646 --> 00:00:17,722 So, first of all, when people are just talking about flux, 8 00:00:17,722 --> 00:00:19,417 and this is the easiest way that I know 9 00:00:19,417 --> 00:00:20,427 how to conceptualize it. 10 00:00:20,427 --> 00:00:22,889 They're talking about how much of something 11 00:00:22,889 --> 00:00:26,755 is flowing through a surface in a given amount of time. 12 00:00:26,755 --> 00:00:28,659 So if you imagine that this is, 13 00:00:28,659 --> 00:00:32,827 this is, I'm just defining a volume of air right over here. 14 00:00:32,827 --> 00:00:36,054 And let's say the air is denser near the bottom 15 00:00:36,054 --> 00:00:37,192 of this volume of air, 16 00:00:37,192 --> 00:00:40,722 so there's more air down here 17 00:00:40,722 --> 00:00:42,161 than there is up here, 18 00:00:42,161 --> 00:00:43,322 which is generally true. 19 00:00:43,322 --> 00:00:47,955 Air density goes down as you increase altitude. 20 00:00:47,955 --> 00:00:50,161 So there's very low density up here. 21 00:00:50,161 --> 00:00:51,589 This is in between. 22 00:00:51,589 --> 00:00:53,191 I don't have to draw all the air particles, 23 00:00:53,191 --> 00:00:54,523 but you get the sense. 24 00:00:54,523 --> 00:00:57,750 Lot of air, lot of air down here. 25 00:00:57,750 --> 00:00:59,457 And the air is moving. 26 00:00:59,457 --> 00:01:01,350 And so let's say that the air, 27 00:01:01,350 --> 00:01:04,391 let's say the air is... 28 00:01:04,391 --> 00:01:06,887 Let me do the velocity vectors in a different color. 29 00:01:06,887 --> 00:01:10,951 So, these are some of the velocity vectors of the air. 30 00:01:10,951 --> 00:01:14,852 Let's say the air on this side is moving 31 00:01:14,852 --> 00:01:18,625 is moving at let's say, a medium velocity. 32 00:01:18,625 --> 00:01:20,994 So right over there. 33 00:01:20,994 --> 00:01:23,292 But as we move more in that direction, 34 00:01:23,292 --> 00:01:25,707 the air is moving faster. 35 00:01:25,707 --> 00:01:30,707 So they have larger velocity vectors like that. 36 00:01:31,524 --> 00:01:33,695 We see that in general, all of the air is moving 37 00:01:33,695 --> 00:01:36,388 in that general direction, that's the way I'm drawing it. 38 00:01:36,388 --> 00:01:38,919 And I can draw the velocity vectors over here. 39 00:01:38,919 --> 00:01:40,858 The air is less dense. 40 00:01:40,858 --> 00:01:42,484 But the trend in the velocity vectors, 41 00:01:42,484 --> 00:01:44,225 when I go from the left to the right is 42 00:01:44,225 --> 00:01:45,827 roughly the same. 43 00:01:45,827 --> 00:01:47,859 So that's the flow. 44 00:01:47,859 --> 00:01:50,425 Now I'm just sampling some of the velocity vectors there. 45 00:01:50,425 --> 00:01:51,551 So let's talk about flux. 46 00:01:51,551 --> 00:01:53,026 And the thing about flux, 47 00:01:53,026 --> 00:01:53,850 really of any form, 48 00:01:53,850 --> 00:01:55,487 you have to think about a surface. 49 00:01:55,487 --> 00:01:58,958 So let's imagine you were to put some type of a net. 50 00:01:58,958 --> 00:02:02,348 Let's say you were to put a net right over 51 00:02:02,348 --> 00:02:05,355 right over here, right over here. 52 00:02:05,355 --> 00:02:06,992 And if we think about the flux, 53 00:02:06,992 --> 00:02:08,757 we would say, well how much air 54 00:02:08,757 --> 00:02:12,054 is traveling through that net in a certain amount of time? 55 00:02:12,054 --> 00:02:13,958 We could say how many molecules 56 00:02:13,958 --> 00:02:16,989 are traveling in say, each second. 57 00:02:16,989 --> 00:02:19,694 And so this would have some flux associated with it. 58 00:02:19,694 --> 00:02:20,889 Relative to the air. 59 00:02:20,889 --> 00:02:23,293 But what if we were to take that same net. 60 00:02:23,293 --> 00:02:25,092 And we're assuming it's some type of theoretical net 61 00:02:25,092 --> 00:02:27,658 that actually does not impede the air flow. 62 00:02:27,658 --> 00:02:30,886 But it helps us visualize a surface. 63 00:02:30,886 --> 00:02:34,287 What if we were to move that net a little bit to the right 64 00:02:34,287 --> 00:02:36,308 where the density is the same, 65 00:02:36,308 --> 00:02:39,094 but the particles are just moving faster. 66 00:02:39,094 --> 00:02:41,346 Well now, our flux would increase. 67 00:02:41,346 --> 00:02:44,284 So this is larger flux. 68 00:02:44,284 --> 00:02:46,954 Larger, larger flux. 69 00:02:46,954 --> 00:02:48,719 Why is our flux increase? 70 00:02:48,719 --> 00:02:50,750 Because, well, the density is the same, 71 00:02:50,750 --> 00:02:51,993 but in any given amount of time 72 00:02:51,993 --> 00:02:56,486 I'm gonna have more things going through that surface. 73 00:02:56,486 --> 00:02:58,680 Now what if I were to put that same net 74 00:02:58,680 --> 00:03:00,828 and move it up to this high altitude, 75 00:03:00,828 --> 00:03:02,558 right over here? 76 00:03:02,558 --> 00:03:03,951 That high altitude. 77 00:03:03,951 --> 00:03:07,387 Well, the velocity of the molecules are the same, 78 00:03:07,387 --> 00:03:08,421 and they're going in the same direction. 79 00:03:08,421 --> 00:03:10,127 But there's just fewer of them. 80 00:03:10,127 --> 00:03:12,751 So you're going to have less fewer molecules 81 00:03:12,751 --> 00:03:15,886 traveling through the surface in a given amount of time. 82 00:03:15,886 --> 00:03:17,453 So this is going to have smaller flux. 83 00:03:17,453 --> 00:03:19,787 And this is all relative to my first one. 84 00:03:19,787 --> 00:03:23,676 Smaller, smaller flux. 85 00:03:23,676 --> 00:03:26,555 Now, what if you were to take the same net 86 00:03:26,555 --> 00:03:30,224 and instead of the direction of the air 87 00:03:30,224 --> 00:03:32,360 being perpendicular to the surface, 88 00:03:32,360 --> 00:03:34,323 be normal to the surface, 89 00:03:34,323 --> 00:03:36,122 what if you were to take the net 90 00:03:36,122 --> 00:03:38,525 and reorientate it so that the air is going 91 00:03:38,525 --> 00:03:40,151 in the same direction of the surface. 92 00:03:40,151 --> 00:03:41,950 So what if you were to take the same net 93 00:03:41,950 --> 00:03:44,388 and you were to make it like this. 94 00:03:44,388 --> 00:03:45,758 So that it's the same net. 95 00:03:45,758 --> 00:03:47,384 I know it doesn't look exactly the same. 96 00:03:47,384 --> 00:03:49,323 But it's the same net, 97 00:03:49,323 --> 00:03:50,240 and you're to make it like this. 98 00:03:50,240 --> 00:03:53,026 Well now how much air is traveling through that net 99 00:03:53,026 --> 00:03:54,861 in a given amount of time? 100 00:03:54,861 --> 00:03:56,556 Well now very little to zero air 101 00:03:56,556 --> 00:03:57,960 is gonna be traveling through that net 102 00:03:57,960 --> 00:03:58,889 in any given amount of time. 103 00:03:58,889 --> 00:04:00,422 The air is going along the surface, 104 00:04:00,422 --> 00:04:02,256 not through the surface. 105 00:04:02,256 --> 00:04:04,857 So this one, let's just say that 106 00:04:04,857 --> 00:04:06,157 all the air is going exactly 107 00:04:06,157 --> 00:04:07,492 in the same direction as the surface, 108 00:04:07,492 --> 00:04:09,361 so nothing is going through the surface. 109 00:04:09,361 --> 00:04:11,753 We would say that this one has zero, 110 00:04:11,753 --> 00:04:13,390 zero flux. 111 00:04:13,390 --> 00:04:15,724 Now let's say that this theoretical net 112 00:04:15,724 --> 00:04:17,500 that actually does not impede the air flow, 113 00:04:17,500 --> 00:04:19,184 let's say we can stretch it or contract it. 114 00:04:19,184 --> 00:04:20,995 So if we stretch that net, 115 00:04:20,995 --> 00:04:23,421 in the same, let's say we were to do it, 116 00:04:23,421 --> 00:04:26,022 let's say we were to stretch it up like this. 117 00:04:26,022 --> 00:04:27,891 So it becomes a bigger net. 118 00:04:27,891 --> 00:04:29,783 So it becomes a bigger net like this. 119 00:04:29,783 --> 00:04:31,954 Well now this thing's gonna have larger flux 120 00:04:31,954 --> 00:04:33,650 because there's just more area. 121 00:04:33,650 --> 00:04:35,449 There's more to flow through. 122 00:04:35,449 --> 00:04:37,725 So now, if you said for this surface, 123 00:04:37,725 --> 00:04:39,222 you're gonna have a larger flux 124 00:04:39,222 --> 00:04:40,627 because there's just gonna be more air 125 00:04:40,627 --> 00:04:42,024 is going to go through that 126 00:04:42,024 --> 00:04:44,017 in any given unit of time. 127 00:04:44,017 --> 00:04:45,120 So as you can see, 128 00:04:45,120 --> 00:04:46,850 when we think about how much of something 129 00:04:46,850 --> 00:04:48,951 just flux in the traditional sense. 130 00:04:48,951 --> 00:04:50,856 How much of something goes through a surface 131 00:04:50,856 --> 00:04:52,493 in a given unit of time. 132 00:04:52,493 --> 00:04:56,057 It depends in this case, the density of the substance. 133 00:04:56,057 --> 00:04:57,949 It depends on 134 00:04:57,949 --> 00:04:59,528 it's velocity. 135 00:04:59,528 --> 00:05:00,921 Both the magnitude of the velocity 136 00:05:00,921 --> 00:05:02,326 and the direction of the velocity. 137 00:05:02,326 --> 00:05:03,824 We see if we orient the surface 138 00:05:03,824 --> 00:05:05,786 or if we oriented the velocity. 139 00:05:05,786 --> 00:05:08,154 So it's not going normal to the surface, 140 00:05:08,154 --> 00:05:09,385 perpendicular to the surface. 141 00:05:09,385 --> 00:05:11,986 Well then, we can have our flux go down. 142 00:05:11,986 --> 00:05:13,414 And you can have things in between. 143 00:05:13,414 --> 00:05:15,295 You can have a net. 144 00:05:15,295 --> 00:05:17,291 Let's say we took that same original net. 145 00:05:17,291 --> 00:05:20,554 But the direction of the air is neither normal 146 00:05:20,554 --> 00:05:22,760 nor exactly in the same direction of the surface. 147 00:05:22,760 --> 00:05:25,418 Well this flux is going to be in between, 148 00:05:25,418 --> 00:05:27,590 is going to be in between that original flux. 149 00:05:27,590 --> 00:05:29,250 And this one right over here. 150 00:05:29,250 --> 00:05:32,117 There's gonna be air flowing through. 151 00:05:32,117 --> 00:05:35,020 There is going to be air 152 00:05:35,020 --> 00:05:37,226 flowing through 153 00:05:37,226 --> 00:05:39,060 the actual surface. 154 00:05:39,060 --> 00:05:41,951 But it's not going exactly normal to the surface. 155 00:05:41,951 --> 00:05:44,052 And as we will explore later 156 00:05:44,052 --> 00:05:45,655 when we get a little bit more mathy into it. 157 00:05:45,655 --> 00:05:47,756 We actually care about the component 158 00:05:47,756 --> 00:05:50,426 of the vector of the air that is exactly normal 159 00:05:50,426 --> 00:05:53,027 when we eventually calculate flux. 160 00:05:53,027 --> 00:05:54,792 But this flux is gonna be some place in between 161 00:05:54,792 --> 00:05:56,986 this one and the zero flux 162 00:05:56,986 --> 00:05:59,993 because the air isn't going exactly perpendicular. 163 00:05:59,993 --> 00:06:03,221 Well that's just the more basic, 164 00:06:03,221 --> 00:06:05,914 or for me the more intuitive notion of flux. 165 00:06:05,914 --> 00:06:08,747 But what do we mean by magnetic, 166 00:06:08,747 --> 00:06:10,988 by magnetic flux? 167 00:06:10,988 --> 00:06:13,461 Well, like regular flux, 168 00:06:13,461 --> 00:06:17,652 we're still dealing with how things are kind of, 169 00:06:17,652 --> 00:06:19,753 you could say going through a surface. 170 00:06:19,753 --> 00:06:22,516 But instead of thinking about air particles or 171 00:06:22,516 --> 00:06:24,920 water molecules or things like that, 172 00:06:24,920 --> 00:06:27,555 we're gonna be thinking about a magnetic field. 173 00:06:27,555 --> 00:06:29,424 So let me draw a surface. 174 00:06:29,424 --> 00:06:31,955 So I have, I have a little bar magnet. 175 00:06:31,955 --> 00:06:34,718 This is the north side, this is the south side. 176 00:06:34,718 --> 00:06:36,588 We see our field lines. 177 00:06:36,588 --> 00:06:39,119 And then I've drawn a couple of the magnetic 178 00:06:39,119 --> 00:06:41,821 field vectors in white there. 179 00:06:41,821 --> 00:06:44,955 And let's say that we have a surface. 180 00:06:44,955 --> 00:06:46,906 We have a surface like this. 181 00:06:48,276 --> 00:06:49,890 And so, for this surface 182 00:06:49,890 --> 00:06:51,886 when we think about the flux 183 00:06:51,886 --> 00:06:54,592 we wanna care about... 184 00:06:54,592 --> 00:06:57,993 things are actually moving when we think about magnetic flux 185 00:06:57,993 --> 00:07:00,292 we aren't actually thinking about actual 186 00:07:00,292 --> 00:07:02,928 physical things moving through the surface. 187 00:07:02,928 --> 00:07:04,390 The way we did when we thought about, 188 00:07:04,390 --> 00:07:06,457 I guess you could say, traditional or more, 189 00:07:06,457 --> 00:07:08,152 or flow-based flux. 190 00:07:08,152 --> 00:07:09,789 But it's a similar idea. 191 00:07:09,789 --> 00:07:12,552 We care about the component 192 00:07:12,552 --> 00:07:14,027 of the magnetic field. 193 00:07:14,027 --> 00:07:16,047 And the density of the magnetic field 194 00:07:16,047 --> 00:07:19,007 that is normal to this surface. 195 00:07:19,007 --> 00:07:21,562 So let's say that this has a given flux. 196 00:07:21,562 --> 00:07:24,394 So let's call that, and the notation is phy. 197 00:07:24,394 --> 00:07:27,494 And, that's the flux of the magnetic field. 198 00:07:27,494 --> 00:07:29,851 And once again, it's based on, 199 00:07:29,851 --> 00:07:33,624 it's based on the strength of the magnetic field 200 00:07:33,624 --> 00:07:38,624 and specially the component of the magnetic field vectors 201 00:07:38,849 --> 00:07:41,078 that are perpendicular, 202 00:07:41,078 --> 00:07:44,317 that are perpendicular to this actual surface. 203 00:07:44,317 --> 00:07:46,790 So this would have one magnetic flux. 204 00:07:46,790 --> 00:07:49,356 But if I were to take the same surface 205 00:07:49,356 --> 00:07:51,190 and make it parallel, 206 00:07:51,190 --> 00:07:55,393 make it parallel to the magnetic field vecotrs 207 00:07:55,393 --> 00:07:57,761 instead of being normal or... 208 00:07:57,761 --> 00:07:59,584 Now the magnetic field vectors are parallel to it 209 00:07:59,584 --> 00:08:00,687 instead of being normal. 210 00:08:00,687 --> 00:08:02,452 So now our flux is zero. 211 00:08:02,452 --> 00:08:05,494 So this would have zero, or pretty close to zero. 212 00:08:05,494 --> 00:08:07,386 So approximately zero 213 00:08:07,386 --> 00:08:09,279 magnetic flux. 214 00:08:09,279 --> 00:08:11,020 Magnetic flux. 215 00:08:11,020 --> 00:08:12,251 Flux. 216 00:08:12,251 --> 00:08:14,120 Now if I were to take this surface 217 00:08:14,120 --> 00:08:15,560 and instead of orienting this way 218 00:08:15,560 --> 00:08:17,986 I just moved it further away. 219 00:08:17,986 --> 00:08:19,588 So instead of putting in here 220 00:08:19,588 --> 00:08:21,353 I would take it all the way out here 221 00:08:21,353 --> 00:08:25,393 where the magnetic field is weaker. 222 00:08:25,393 --> 00:08:26,856 Where the magnetic field is weaker. 223 00:08:26,856 --> 00:08:29,225 So we have a weaker magnetic field out here. 224 00:08:29,225 --> 00:08:30,757 The flux would also decrease. 225 00:08:30,757 --> 00:08:32,659 So it has a lot of the same properties 226 00:08:32,659 --> 00:08:34,216 as this more physical flux 227 00:08:34,217 --> 00:08:35,818 that we were talking about before. 228 00:08:35,818 --> 00:08:37,082 But instead of talking about, say, 229 00:08:37,082 --> 00:08:39,057 the velocity of the air molecules, 230 00:08:39,058 --> 00:08:42,054 no, the velocity vectors of the air molecules 231 00:08:42,054 --> 00:08:43,888 and how those relate to the surface, 232 00:08:43,888 --> 00:08:48,393 here we're talking about the magnetic field vectors. 233 00:08:48,393 --> 00:08:50,691 And how those relate to the surface. 234 00:08:50,691 --> 00:08:54,720 But the metaphor, the analogy is still the same. 235 00:08:54,720 --> 00:08:57,054 If they are perpendicular, you have larger flux. 236 00:08:57,054 --> 00:08:59,515 If they are going in the same direction, 237 00:08:59,515 --> 00:09:01,721 you might have zero or very little. 238 00:09:01,721 --> 00:09:03,590 You might have very little flux. 239 00:09:03,590 --> 00:09:07,154 If you have a weak magnetic field out here, 240 00:09:07,154 --> 00:09:08,292 the flux is going to be lower 241 00:09:08,292 --> 00:09:11,694 than if you have a strong magnetic field. 242 00:09:11,694 --> 00:09:12,855 That's analogous to, 243 00:09:12,855 --> 00:09:15,386 when you had high density and high velocity, 244 00:09:15,386 --> 00:09:16,883 that was a lot of flux. 245 00:09:16,883 --> 00:09:18,683 Versus low density or low velocity 246 00:09:18,683 --> 00:09:20,657 that is lower flux. 247 00:09:20,657 --> 00:09:23,884 And also, we can increase the total surface. 248 00:09:23,884 --> 00:09:25,394 So if we stretch that surface 249 00:09:25,394 --> 00:09:27,356 or we had a larger surface right over here, 250 00:09:27,356 --> 00:09:29,956 the flux through this surface is gonna be larger 251 00:09:29,956 --> 00:09:31,814 than the flux through this surface. 252 00:09:31,814 --> 00:09:33,521 Let's say this surface is analogous 253 00:09:33,521 --> 00:09:36,121 to a surface like this right over here. 254 00:09:36,121 --> 00:09:38,792 Let's say that the magnetic field is symmetric on both sides 255 00:09:38,792 --> 00:09:40,742 so the flux through this surface 256 00:09:40,742 --> 00:09:42,588 and this surface would be the same. 257 00:09:42,588 --> 00:09:44,260 So if you were to stretch it out 258 00:09:44,260 --> 00:09:46,222 to be a larger surface, 259 00:09:46,222 --> 00:09:49,821 well now you just have more of the magnetic field 260 00:09:49,821 --> 00:09:52,991 that is now normal to the surface. 261 00:09:52,991 --> 00:09:55,254 So hopefully this gives you at least a beginning ideas 262 00:09:55,254 --> 00:09:57,751 of the notion of magnetic flux. 263 00:09:57,751 --> 00:09:59,086 And how it relates to, 264 00:09:59,086 --> 00:00:00,000 I guess you could think of more physical flux.