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EN_B00000_S02862_W000028
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3032, "duration": 11.516, "id": "EN_B00000_S02862_W000028", "language": "en", "speaker": "EN_B00000_S02862", "text": " So what happens if you're out here though? So what's happening in the guts of this metal is that Q is still gonna attract negative Q on the inside edge. Even if this metal was...
EN_B00000_S02862_W000028.mp3
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EN_B00000_S02862_W000029
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4111, "duration": 6.364, "id": "EN_B00000_S02862_W000029", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uhm, but what that means is that the outside edge, because this, uh, metal has to have a total charge Q,", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B00000_S02862_W000029.mp3...
EN_B00000_S02862_W000029.mp3
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EN_B00000_S02862_W000030
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.434, "duration": 19.356, "id": "EN_B00000_S02862_W000030", "language": "en", "speaker": "EN_B00000_S02862", "text": " You need to make sure that the outside edge plus the inside edge adds up to q this time. So instead of having positive just q on the outside edge, you're gonna have capital Q p...
EN_B00000_S02862_W000030.mp3
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EN_B00000_S02862_W000031
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4906, "duration": 9.788, "id": "EN_B00000_S02862_W000031", "language": "en", "speaker": "EN_B00000_S02862", "text": " You need to make sure outside edge plus inside edge adds up to the total amount of charge on the metal shell and this inside edge is always going to equal whatever's in here.",...
EN_B00000_S02862_W000031.mp3
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EN_B00000_S02862_W000032
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4393, "duration": 12.764, "id": "EN_B00000_S02862_W000032", "language": "en", "speaker": "EN_B00000_S02862", "text": " So if you had a charge little q inside, you gotta have a charge little q plastered from the metal on this inside edge. So that's, this isn't little negative q regardless of wh...
EN_B00000_S02862_W000032.mp3
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EN_B00000_S02862_W000033
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3263, "duration": 10.172, "id": "EN_B00000_S02862_W000033", "language": "en", "speaker": "EN_B00000_S02862", "text": " And why is the charge all go to the edge? Because like, they repel. You know what I mean? They're trying to get far away from each other as possible. So you go to the edge. Uh...
EN_B00000_S02862_W000033.mp3
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EN_B00000_S02862_W000034
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4968, "duration": 13.308, "id": "EN_B00000_S02862_W000034", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uh, Gaussian surface outside here, you're enclosing little q plus negative little q plus capital Q plus little q. Well, little q and negative q cancel, so you get q plus q tot...
EN_B00000_S02862_W000034.mp3
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EN_B00000_S02862_W000035
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2802, "duration": 4.195, "id": "EN_B00000_S02862_W000035", "language": "en", "speaker": "EN_B00000_S02862", "text": " What if you had a metal shell but there was no charge inside? Well this time, shoot.", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B00000_S02862_W000035.mp3" }
EN_B00000_S02862_W000035.mp3
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EN_B00000_S02862_W000036
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3411, "duration": 10.662, "id": "EN_B00000_S02862_W000036", "language": "en", "speaker": "EN_B00000_S02862", "text": " Inside here, less than A, you got no charge in there. What if you're in a medal? Zero. Always zero. Inside a medal, zero. What if you're outside here? Okay, well the, the meda...
EN_B00000_S02862_W000036.mp3
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EN_B00000_S02862_W000037
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4229, "duration": 8.348, "id": "EN_B00000_S02862_W000037", "language": "en", "speaker": "EN_B00000_S02862", "text": " Okay, so what if it's an insulating charged sphere? Insulating means you can have charge throughout the guts of it. So this is supposed to represent a sphere.", "wav": "EN_B0...
EN_B00000_S02862_W000037.mp3
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EN_B00000_S02862_W000038
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.5122, "duration": 12.988, "id": "EN_B00000_S02862_W000038", "language": "en", "speaker": "EN_B00000_S02862", "text": " With a, with a radius less than capital R, the way you find your Q is that, you know, rho, the charge density, the charge per volume, so that means charge is just the charge d...
EN_B00000_S02862_W000038.mp3
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EN_B00000_S02862_W000039
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.1599, "duration": 11.868, "id": "EN_B00000_S02862_W000039", "language": "en", "speaker": "EN_B00000_S02862", "text": " What volume? Volume of a sphere, because we had a sphere here, and it's little r, you know, little r is the radius of my Gaussian sphere. Just like this is little r, that's li...
EN_B00000_S02862_W000039.mp3
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EN_B00000_S02862_W000040
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3382, "duration": 9.116, "id": "EN_B00000_S02862_W000040", "language": "en", "speaker": "EN_B00000_S02862", "text": " What happens if I'm out here, if my Gaussian surface is bigger? So say I want to know the electric field out here, so I put my Gaussian surface all the way out here with a radi...
EN_B00000_S02862_W000040.mp3
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EN_B00000_S02862_W000041
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2678, "duration": 10.428, "id": "EN_B00000_S02862_W000041", "language": "en", "speaker": "EN_B00000_S02862", "text": " Well, you gotta stop your, you know, you multiply by capital R here. The most charge you can have is all of the charge, and all of the charge is the charge density times all o...
EN_B00000_S02862_W000041.mp3
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EN_B00000_S02862_W000042
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4753, "duration": 19.26, "id": "EN_B00000_S02862_W000042", "language": "en", "speaker": "EN_B00000_S02862", "text": " You can't keep acting like you're gonna add charge out here by moving further out. The most charge you get is all the charge and all the charge stops at capital R. So you have ...
EN_B00000_S02862_W000042.mp3
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EN_B00000_S02862_W000043
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4408, "duration": 13.436, "id": "EN_B00000_S02862_W000043", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uhm, what if they didn't give you charge density? What if they gave you just total charge in the sphere? You do it the exact same way. It's just you have to craft your own cha...
EN_B00000_S02862_W000043.mp3
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EN_B00000_S02862_W000044
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3043, "duration": 12.476, "id": "EN_B00000_S02862_W000044", "language": "en", "speaker": "EN_B00000_S02862", "text": " Divided by four-thirds pi. Oh, here's a question. Is it little r or big R? You've got to put big R. Look, if I put total charge, that's supposed to be cute. If I put total cha...
EN_B00000_S02862_W000044.mp3
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EN_B00000_S02862_W000045
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.0501, "duration": 3.141, "id": "EN_B00000_S02862_W000045", "language": "en", "speaker": "EN_B00000_S02862", "text": " So if I really want the charge density, it's total charge over total volume.", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B00000_S02862_W000045.mp3" }
EN_B00000_S02862_W000045.mp3
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EN_B00000_S02862_W000046
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3629, "duration": 17.895, "id": "EN_B00000_S02862_W000046", "language": "en", "speaker": "EN_B00000_S02862", "text": " I could put charge in here divided by volume in there, but I don't know the charge in there. That's the whole point. I want to find the charge in here. I don't know what the c...
EN_B00000_S02862_W000046.mp3
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EN_B00000_S02862_W000047
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.0943, "duration": 6.172, "id": "EN_B00000_S02862_W000047", "language": "en", "speaker": "EN_B00000_S02862", "text": " So that's rho, what do we multiply? Same thing we did by before, you multiply by the like volume you're finding. So if I'm in here,", "wav": "EN_B00000/EN_B00000_S02862/mp3/E...
EN_B00000_S02862_W000047.mp3
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EN_B00000_S02862_W000048
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3653, "duration": 14.396, "id": "EN_B00000_S02862_W000048", "language": "en", "speaker": "EN_B00000_S02862", "text": " My Gaussian surface is less than, you know, has a radii less than capital R. I'm only enclosing this much charge, so I multiply that much volume. This, this whole up, you know...
EN_B00000_S02862_W000048.mp3
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EN_B00000_S02862_W000049
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2494, "duration": 3.292, "id": "EN_B00000_S02862_W000049", "language": "en", "speaker": "EN_B00000_S02862", "text": " What if your Gaussian surface is out here? You want to find the electric field out here?", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B00000_S02862_W000049.mp3" }
EN_B00000_S02862_W000049.mp3
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EN_B00000_S02862_W000050
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2666, "duration": 15.356, "id": "EN_B00000_S02862_W000050", "language": "en", "speaker": "EN_B00000_S02862", "text": " Left hand side's still the same, but now you're enclosing just total Q. So you just plug in total Q. You might be like, wait, can't I, can't I do the same move where I plug in...
EN_B00000_S02862_W000050.mp3
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EN_B00000_S02862_W000051
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.389, "duration": 10.364, "id": "EN_B00000_S02862_W000051", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uhm, what happens if there's a hole in your insulating charged sphere? Sometimes you call this a shell, like if it's got a hole in the middle. This is a sphere, not a tube.", ...
EN_B00000_S02862_W000051.mp3
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EN_B00000_S02862_W000052
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3353, "duration": 7.516, "id": "EN_B00000_S02862_W000052", "language": "en", "speaker": "EN_B00000_S02862", "text": " So it's a sphere, not cylindrical. Uh, if you're given the charge density, well, if you're inside here, you know, you're enclosing no charge, so zero charge.", "wav": "EN_B00...
EN_B00000_S02862_W000052.mp3
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EN_B00000_S02862_W000053
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3117, "duration": 23.708, "id": "EN_B00000_S02862_W000053", "language": "en", "speaker": "EN_B00000_S02862", "text": " If you're in here with a radii greater than a but less than b, you do it the same as before, you know, charge density times this here would be the volume of this total sphere,...
EN_B00000_S02862_W000053.mp3
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EN_B00000_S02862_W000054
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3672, "duration": 14.812, "id": "EN_B00000_S02862_W000054", "language": "en", "speaker": "EN_B00000_S02862", "text": " Of the charge, which is where the charge is, which is what we want. You multiply by the charge density by that volume. Because, you know, charge density is charge per volume, ...
EN_B00000_S02862_W000054.mp3
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EN_B00000_S02862_W000055
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4152, "duration": 7.772, "id": "EN_B00000_S02862_W000055", "language": "en", "speaker": "EN_B00000_S02862", "text": " That won't give you how much charge there is. So you subtract out the whole. So what this here is giving is the total air, or sorry, total volume of this region here.", "wav"...
EN_B00000_S02862_W000055.mp3
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EN_B00000_S02862_W000056
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2888, "duration": 13.082, "id": "EN_B00000_S02862_W000056", "language": "en", "speaker": "EN_B00000_S02862", "text": " With a r greater than b, uhm, you know, just, you know, stop your, stop your multiplication at little b. You can't get any more charge than the total charge. So what, what thi...
EN_B00000_S02862_W000056.mp3
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EN_B00000_S02862_W000057
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2249, "duration": 4.278, "id": "EN_B00000_S02862_W000057", "language": "en", "speaker": "EN_B00000_S02862", "text": " Total volume meaning like the entire volume of this shell.", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B00000_S02862_W000057.mp3" }
EN_B00000_S02862_W000057.mp3
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EN_B00000_S02862_W000058
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4144, "duration": 19.932, "id": "EN_B00000_S02862_W000058", "language": "en", "speaker": "EN_B00000_S02862", "text": " So multiply the charge density by this total volume, and you'd get the total charge enclosed, which is all the charge. You can't be, this, you should not have a little r here,...
EN_B00000_S02862_W000058.mp3
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EN_B00000_S02862_W000059
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.333, "duration": 9.468, "id": "EN_B00000_S02862_W000059", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uhm, what happens if they gave you Q, not instead? Again, you just craft your own charge density. This one's gonna be a little ugly, you'd be like, okay, well,", "wav": "EN_B0...
EN_B00000_S02862_W000059.mp3
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EN_B00000_S02862_W000060
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2423, "duration": 8.092, "id": "EN_B00000_S02862_W000060", "language": "en", "speaker": "EN_B00000_S02862", "text": " Charge density is the total charge over the total volume, but it's like crap, what's the total volume? It's this mess, remember? This is what we just wrote a minute ago.", "w...
EN_B00000_S02862_W000060.mp3
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EN_B00000_S02862_W000061
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2103, "duration": 13.34, "id": "EN_B00000_S02862_W000061", "language": "en", "speaker": "EN_B00000_S02862", "text": " 4 thirds pi b cubed would be the entire volume of the sphere minus the whole. That's what this is. That's, you know, this is, I'm going to write it as v total. It's this denomi...
EN_B00000_S02862_W000061.mp3
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EN_B00000_S02862_W000062
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.1781, "duration": 3.964, "id": "EN_B00000_S02862_W000062", "language": "en", "speaker": "EN_B00000_S02862", "text": " And then you multiply what you need to multiply by. Obviously if you're inside A, there's no charge.", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B00000_S02862_W000062.mp3" }
EN_B00000_S02862_W000062.mp3
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EN_B00000_S02862_W000063
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2813, "duration": 4.668, "id": "EN_B00000_S02862_W000063", "language": "en", "speaker": "EN_B00000_S02862", "text": " If you're in the guts of this thing, uhm, this is not a metal, so it's not zero, it's insulated.", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B00000_S02862_W000063.mp3" }
EN_B00000_S02862_W000063.mp3
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EN_B00000_S02862_W000064
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4846, "duration": 15.26, "id": "EN_B00000_S02862_W000064", "language": "en", "speaker": "EN_B00000_S02862", "text": " If you're in the guts of this thing, you multiply by the same thing we had before. So this is the exact same expression except we had row here. Now we have to make our own row....
EN_B00000_S02862_W000064.mp3
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EN_B00000_S02862_W000065
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3745, "duration": 10.012, "id": "EN_B00000_S02862_W000065", "language": "en", "speaker": "EN_B00000_S02862", "text": " Surface IF the radii of the Gaussian surface is less than, you know, capital B, but greater than A. So this is just the volume enclosed.", "wav": "EN_B00000/EN_B00000_S02862...
EN_B00000_S02862_W000065.mp3
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EN_B00000_S02862_W000066
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3279, "duration": 13.21, "id": "EN_B00000_S02862_W000066", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uhm, this is the total volume and total charge, which is charge density. And then if you're outside the whole thing, it's kind of easy. You're enclosing the total charge. So th...
EN_B00000_S02862_W000066.mp3
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EN_B00000_S02862_W000067
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.362, "duration": 14.012, "id": "EN_B00000_S02862_W000067", "language": "en", "speaker": "EN_B00000_S02862", "text": " What happens if your charge density is not uniform? Well, then you gotta do an integral. So the idea is you're like, okay, crap. You know, the total charge is the charge densit...
EN_B00000_S02862_W000067.mp3
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EN_B00000_S02862_W000068
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.361, "duration": 5.372, "id": "EN_B00000_S02862_W000068", "language": "en", "speaker": "EN_B00000_S02862", "text": " What if my charge density is not constant or uniform? Well, you could say like the little bit of charge.", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B00000_S02862_W000068.mp3"...
EN_B00000_S02862_W000068.mp3
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EN_B00000_S02862_W000069
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.433, "duration": 18.716, "id": "EN_B00000_S02862_W000069", "language": "en", "speaker": "EN_B00000_S02862", "text": " Within any little, like, chunk, you know what I mean? In that little chunk, if you make it infinitesimally small, an infinitesimally small volume, well, the charge density can'...
EN_B00000_S02862_W000069.mp3
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EN_B00000_S02862_W000070
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2301, "duration": 7.063, "id": "EN_B00000_S02862_W000070", "language": "en", "speaker": "EN_B00000_S02862", "text": " And now we can just integrate both sides and I can say that my q is going to be the integral of rho dv. This is always true.", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B0000...
EN_B00000_S02862_W000070.mp3
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EN_B00000_S02862_W000071
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2803, "duration": 17.792, "id": "EN_B00000_S02862_W000071", "language": "en", "speaker": "EN_B00000_S02862", "text": " It's just a matter of like, what would you put in for dV? So this is what I'm doing up here. I'm saying, okay, Q enclosed. This whole numerator is Q enclosed. Uhm, I'm taking ...
EN_B00000_S02862_W000071.mp3
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EN_B00000_S02862_W000072
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.1869, "duration": 10.971, "id": "EN_B00000_S02862_W000072", "language": "en", "speaker": "EN_B00000_S02862", "text": " Now take a differential of that, what's going to happen, the 3 is going to come down, it's going to cancel out the other 3, you're going to end up with 4 pi r squared and then...
EN_B00000_S02862_W000072.mp3
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EN_B00000_S02862_W000073
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3646, "duration": 17.755, "id": "EN_B00000_S02862_W000073", "language": "en", "speaker": "EN_B00000_S02862", "text": " You know, dv over dr, if this is the volume right here, four-thirds pi r cubed is gonna be, the three comes down, you get four pi r squared. And then just move the dr over and...
EN_B00000_S02862_W000073.mp3
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EN_B00000_S02862_W000074
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2996, "duration": 7.069, "id": "EN_B00000_S02862_W000074", "language": "en", "speaker": "EN_B00000_S02862", "text": " It's only true if it's got spherical symmetry, that is to say that changing this angle isn't gonna change the charge density.", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B000...
EN_B00000_S02862_W000074.mp3
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EN_B00000_S02862_W000075
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.497, "duration": 8.251, "id": "EN_B00000_S02862_W000075", "language": "en", "speaker": "EN_B00000_S02862", "text": " And changing this as a muthal angle doesn't change the charge density. So this is dV if the only variation that's occurring is in radius, so.", "wav": "EN_B00000/EN_B00000_S02...
EN_B00000_S02862_W000075.mp3
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EN_B00000_S02862_W000076
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4054, "duration": 11.739, "id": "EN_B00000_S02862_W000076", "language": "en", "speaker": "EN_B00000_S02862", "text": " The only variable that the charge density depends on is radius, like how far out you're going. Which is almost always what the case is. If you wanted to do it with these angle...
EN_B00000_S02862_W000076.mp3
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EN_B00000_S02862_W000077
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3557, "duration": 13.627, "id": "EN_B00000_S02862_W000077", "language": "en", "speaker": "EN_B00000_S02862", "text": " AP test or any introductory class. So this is your integral row DV. What do you integrate from? From zero in this case, because there was charge from here all the way to littl...
EN_B00000_S02862_W000077.mp3
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EN_B00000_S02862_W000078
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.1995, "duration": 17.245, "id": "EN_B00000_S02862_W000078", "language": "en", "speaker": "EN_B00000_S02862", "text": " And you integrate this, so this is little r, that contributes, you can't pull that out, you can pull the 4 out, you can pull the pi out, but the r, little r stays in there. An...
EN_B00000_S02862_W000078.mp3
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EN_B00000_S02862_W000079
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3798, "duration": 19.1, "id": "EN_B00000_S02862_W000079", "language": "en", "speaker": "EN_B00000_S02862", "text": " What if your r is greater than big R? Just stop your integral there. You know, just integrate all the way to the edge. That's it. You got all of it. Don't go any farther than th...
EN_B00000_S02862_W000079.mp3
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EN_B00000_S02862_W000080
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4539, "duration": 9.596, "id": "EN_B00000_S02862_W000080", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uhm, what would happen if you had a hole in your sphere? This time it's a shell. Well obviously if you're in here, you're gonna have zero, because you're enclosing zero charge....
EN_B00000_S02862_W000080.mp3
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EN_B00000_S02862_W000081
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.34, "duration": 16.764, "id": "EN_B00000_S02862_W000081", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uh, what would happen if you're in the guts of this thing? It's not a metal, so you can't say it's zero. You do the exact same integral you did before. Integral rho dv. But just...
EN_B00000_S02862_W000081.mp3
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EN_B00000_S02862_W000082
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2527, "duration": 15.237, "id": "EN_B00000_S02862_W000082", "language": "en", "speaker": "EN_B00000_S02862", "text": " And then what if you're outside the whole thing? Well, you integrate from A to B. That includes, you know, the whole thing. So you go from A all the way to B. That gives you y...
EN_B00000_S02862_W000082.mp3
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EN_B00000_S02862_W000083
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4908, "duration": 19.196, "id": "EN_B00000_S02862_W000083", "language": "en", "speaker": "EN_B00000_S02862", "text": " And of course, okay, you divide both sides by 4 pi r squared, that gives you e. Typically you're trying to find e in these cases. So as a, those are almost all the spherical c...
EN_B00000_S02862_W000083.mp3
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EN_B00000_S02862_W000084
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.5163, "duration": 11.452, "id": "EN_B00000_S02862_W000084", "language": "en", "speaker": "EN_B00000_S02862", "text": " You know, circumference here times height gives you this area here? And you might be like, shouldn't we add pi r squared plus pi r squared? No, because look, the electric fiel...
EN_B00000_S02862_W000084.mp3
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EN_B00000_S02862_W000085
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4501, "duration": 14.012, "id": "EN_B00000_S02862_W000085", "language": "en", "speaker": "EN_B00000_S02862", "text": " So the electric field pierces this area here, but, you know, there's no flux if the electric field doesn't pierce your area. So if this is running along the surface, it's not ...
EN_B00000_S02862_W000085.mp3
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EN_B00000_S02862_W000086
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3736, "duration": 14.332, "id": "EN_B00000_S02862_W000086", "language": "en", "speaker": "EN_B00000_S02862", "text": " Yes, they have an area, but there's no electric flux through them. The flux is only through this like, you know, toilet paper roll part, not the end cap part. So the only part...
EN_B00000_S02862_W000086.mp3
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EN_B00000_S02862_W000087
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3452, "duration": 8.444, "id": "EN_B00000_S02862_W000087", "language": "en", "speaker": "EN_B00000_S02862", "text": " You know, length times height gives you the area of this thing. So that's your area. This is gonna be the same area for every single cylindrical problem. Always 2 pi little r h...
EN_B00000_S02862_W000087.mp3
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EN_B00000_S02862_W000088
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2503, "duration": 18.421, "id": "EN_B00000_S02862_W000088", "language": "en", "speaker": "EN_B00000_S02862", "text": " This is my Gaussian surface. What if I had a line of charge? And let's say the charge was lambda. What does lambda mean? Lambda is the amount of charge per length instead of c...
EN_B00000_S02862_W000088.mp3
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EN_B00000_S02862_W000089
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4014, "duration": 16.892, "id": "EN_B00000_S02862_W000089", "language": "en", "speaker": "EN_B00000_S02862", "text": " So, how much charge would I enclose here? Well, it's like all of this charge, how much is that? Lambda times the length of it, but I called my length of the cylinder h, so it'...
EN_B00000_S02862_W000089.mp3
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EN_B00000_S02862_W000090
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4014, "duration": 7.1, "id": "EN_B00000_S02862_W000090", "language": "en", "speaker": "EN_B00000_S02862", "text": " Infinitely long charge density so that you can say the E always points straight out and you never get any of these weird edge effects.", "wav": "EN_B00000/EN_B00000_S02862/mp3/...
EN_B00000_S02862_W000090.mp3
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EN_B00000_S02862_W000091
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3333, "duration": 5.5, "id": "EN_B00000_S02862_W000091", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uhm, so that's the easiest one. Lambda times L gives you the charging close. What if it's an insulating cylinder?", "wav": "EN_B00000/EN_B00000_S02862/mp3/EN_B00000_S02862_W000...
EN_B00000_S02862_W000091.mp3
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EN_B00000_S02862_W000092
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4, "duration": 13.596, "id": "EN_B00000_S02862_W000092", "language": "en", "speaker": "EN_B00000_S02862", "text": " Shoot, you know how to deal with this. Uh, rho is charge per volume, so that means charge is rho times volume. What's the volume inside of this Gaussian surface? Remember, the le...
EN_B00000_S02862_W000092.mp3
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EN_B00000_S02862_W000093
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2817, "duration": 10.972, "id": "EN_B00000_S02862_W000093", "language": "en", "speaker": "EN_B00000_S02862", "text": " But I need to multiply by volume to get my charge in here. What's the volume of the cylinder? It's just pi r squared, area of the end cap, times h. So the length of this cylin...
EN_B00000_S02862_W000093.mp3
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EN_B00000_S02862_W000094
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4715, "duration": 19.516, "id": "EN_B00000_S02862_W000094", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uhm, and that's if I'm inside my Gaussian surface has a radius less than capital R. What if my Gaussian surface has a radius greater than capital R. I draw a Gaussian surface ...
EN_B00000_S02862_W000094.mp3
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EN_B00000_S02862_W000095
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4119, "duration": 10.524, "id": "EN_B00000_S02862_W000095", "language": "en", "speaker": "EN_B00000_S02862", "text": " Pi big R squared times H. This would be the total volume. This would give you the total charge. Even though on the left hand side here I'm still little r. Little r is the radi...
EN_B00000_S02862_W000095.mp3
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EN_B00000_S02862_W000096
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3297, "duration": 10.965, "id": "EN_B00000_S02862_W000096", "language": "en", "speaker": "EN_B00000_S02862", "text": " And this is the R you use to find the charge inside. So these do not have to be the same. And then you divide by 2 pi R H. Again, the H cancels. The H is basically always gonn...
EN_B00000_S02862_W000096.mp3
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EN_B00000_S02862_W000097
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2844, "duration": 12.86, "id": "EN_B00000_S02862_W000097", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uh, what happens if it's, uh, non-uniform? You guys know how to do this now. You say, like, q is the integral of rho dv, just like we got over here, except dv for a cylinder is...
EN_B00000_S02862_W000097.mp3
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EN_B00000_S02862_W000098
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4106, "duration": 14.204, "id": "EN_B00000_S02862_W000098", "language": "en", "speaker": "EN_B00000_S02862", "text": " You know, this is the area of a cylinder, sorry, the volume of a cylinder, pi r squared h. So if you take a differential of that, the two comes down, you get two pi r, and the...
EN_B00000_S02862_W000098.mp3
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EN_B00000_S02862_W000099
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2619, "duration": 8.988, "id": "EN_B00000_S02862_W000099", "language": "en", "speaker": "EN_B00000_S02862", "text": " Of a cylindrical symmetry, again, assuming there's no angular dependence here. The only, the only variation happens because of the radius.", "wav": "EN_B00000/EN_B00000_S0286...
EN_B00000_S02862_W000099.mp3
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EN_B00000_S02862_W000100
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3399, "duration": 15.228, "id": "EN_B00000_S02862_W000100", "language": "en", "speaker": "EN_B00000_S02862", "text": " That's basically every problem you're gonna meet. So you integrate rho dv for a cylinder. If your radii, if you want to know the electric field inside here, your radii is gonn...
EN_B00000_S02862_W000100.mp3
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EN_B00000_S02862_W000101
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3602, "duration": 20.827, "id": "EN_B00000_S02862_W000101", "language": "en", "speaker": "EN_B00000_S02862", "text": " What if you're outside the whole thing? You gotta include all the charge, which means you just stop integrating at the edge, because at the edge, that's including all the char...
EN_B00000_S02862_W000101.mp3
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EN_B00000_S02862_W000102
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3404, "duration": 10.812, "id": "EN_B00000_S02862_W000102", "language": "en", "speaker": "EN_B00000_S02862", "text": " What would happen if there was a hole inside? Easy, just like, you know. Oh, well there's no integral here. If your row is just uniform, okay fine, have row times, same deal."...
EN_B00000_S02862_W000102.mp3
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EN_B00000_S02862_W000103
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3892, "duration": 11.9, "id": "EN_B00000_S02862_W000103", "language": "en", "speaker": "EN_B00000_S02862", "text": " Total volume, but subtract out the whole. This right here is just an expression for the volume of the whole. So just subtract out that whole and you get what the answer is. And ...
EN_B00000_S02862_W000103.mp3
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EN_B00000_S02862_W000104
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2099, "duration": 8.764, "id": "EN_B00000_S02862_W000104", "language": "en", "speaker": "EN_B00000_S02862", "text": " If your Gaussian surface is out here, fine, just only go to b squared, right, you can't have any more charge than the total charge, and then you still subtract out the whole, s...
EN_B00000_S02862_W000104.mp3
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EN_B00000_S02862_W000105
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4445, "duration": 12.371, "id": "EN_B00000_S02862_W000105", "language": "en", "speaker": "EN_B00000_S02862", "text": " So you want to make sure that you're only including charge where there is charge. So if you're multiplying row by a volume, make sure you're only multiplying by the volume whe...
EN_B00000_S02862_W000105.mp3
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EN_B00000_S02862_W000106
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2531, "duration": 16.252, "id": "EN_B00000_S02862_W000106", "language": "en", "speaker": "EN_B00000_S02862", "text": " And if it was a charge density, this one's almost easier. Just integrate from the inner radius to the, wherever you're at. So if there's a hole, just don't start at zero. Don'...
EN_B00000_S02862_W000106.mp3
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EN_B00000_S02862_W000107
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3164, "duration": 8.828, "id": "EN_B00000_S02862_W000107", "language": "en", "speaker": "EN_B00000_S02862", "text": " Last one, here we go. That was cylindrical. The last possibility really is just planar symmetry and this one's almost the easiest. So say you have an infinite plane.", "wav":...
EN_B00000_S02862_W000107.mp3
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EN_B00000_S02862_W000108
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.0925, "duration": 10.332, "id": "EN_B00000_S02862_W000108", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uh, the electric field is just going to be pointing straight out of there, up on the top, assuming it's positive, and down on the bottom, because field points away from a posi...
EN_B00000_S02862_W000108.mp3
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EN_B00000_S02862_W000109
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.1946, "duration": 9.948, "id": "EN_B00000_S02862_W000109", "language": "en", "speaker": "EN_B00000_S02862", "text": " What would Gauss's law look like? You draw, you draw something. It doesn't have to be a square. It could be like a, it could be another little cylinder, but it's got to be orie...
EN_B00000_S02862_W000109.mp3
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EN_B00000_S02862_W000110
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4312, "duration": 16.444, "id": "EN_B00000_S02862_W000110", "language": "en", "speaker": "EN_B00000_S02862", "text": " Uhm, and since your electric field points this way and that way, you're gonna get electric flux through the top face and the bottom face. You get none through the sides. So it...
EN_B00000_S02862_W000110.mp3
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EN_B00000_S02862_W000111
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4215, "duration": 10.716, "id": "EN_B00000_S02862_W000111", "language": "en", "speaker": "EN_B00000_S02862", "text": " Is around the top face, is through the top face and the bottom face. But there's two of them, that's why I have 2a here. Whatever your area was of the top one and the bottom o...
EN_B00000_S02862_W000111.mp3
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EN_B00000_S02862_W000112
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3806, "duration": 7.452, "id": "EN_B00000_S02862_W000112", "language": "en", "speaker": "EN_B00000_S02862", "text": " Now, you might be like, what do I write as the areas at height times width? It doesn't matter, cause watch, the total charging closed.", "wav": "EN_B00000/EN_B00000_S02862/mp...
EN_B00000_S02862_W000112.mp3
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EN_B00000_S02862_W000113
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.0978, "duration": 14.14, "id": "EN_B00000_S02862_W000113", "language": "en", "speaker": "EN_B00000_S02862", "text": " By this, it's gotta be closed up. So the sides don't matter in terms of like the flux, but you have to imagine it because the sides matter in terms of finding out how much char...
EN_B00000_S02862_W000113.mp3
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EN_B00000_S02862_W000114
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3101, "duration": 8.956, "id": "EN_B00000_S02862_W000114", "language": "en", "speaker": "EN_B00000_S02862", "text": " How much charge is that? Well, the surface charge density is just charge per area, so charge would be surface charge density times area.", "wav": "EN_B00000/EN_B00000_S02862/...
EN_B00000_S02862_W000114.mp3
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EN_B00000_S02862_W000115
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2586, "duration": 5.692, "id": "EN_B00000_S02862_W000115", "language": "en", "speaker": "EN_B00000_S02862", "text": " And surface charge density times area is how much charge you've got enclosed there. You might be like, how come it's not times two?", "wav": "EN_B00000/EN_B00000_S02862/mp3/E...
EN_B00000_S02862_W000115.mp3
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EN_B00000_S02862_W000116
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4614, "duration": 17.18, "id": "EN_B00000_S02862_W000116", "language": "en", "speaker": "EN_B00000_S02862", "text": " And, uh, this is your flux. So the A would end up canceling. This is why I said it doesn't matter. Write it as pi r-squared if you make this a circle. Write it as height times ...
EN_B00000_S02862_W000116.mp3
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EN_B00000_S02862_W000117
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.223, "duration": 13.244, "id": "EN_B00000_S02862_W000117", "language": "en", "speaker": "EN_B00000_S02862", "text": " outside of this surface doesn't vary with distance. Get as far away from this infinite plane as you want and the electric field is constant, uniform up here. It doesn't die off...
EN_B00000_S02862_W000117.mp3
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EN_B00000_S02862_W000118
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3179, "duration": 13.02, "id": "EN_B00000_S02862_W000118", "language": "en", "speaker": "EN_B00000_S02862", "text": " They're like, what's e as a function of r away from this, you know, call this r or something. It's just a constant value. It just freaks me out. Uhm, but you know, it's an infi...
EN_B00000_S02862_W000118.mp3
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EN_B00000_S02862_W000119
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4122, "duration": 14.716, "id": "EN_B00000_S02862_W000119", "language": "en", "speaker": "EN_B00000_S02862", "text": " So if your plane is really big compared to the distance you are away from it, this would be an approximate value, but you're never gonna meet an infinite plane out there excep...
EN_B00000_S02862_W000119.mp3
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EN_B00000_S02862_W000120
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2736, "duration": 6.684, "id": "EN_B00000_S02862_W000120", "language": "en", "speaker": "EN_B00000_S02862", "text": " Doesn't matter how far away it is, just, just make sure you know which way the fields go. If they go opposite, they cancel. If they go in the same direction, they add up.", "...
EN_B00000_S02862_W000120.mp3
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EN_B00000_S02862_W000121
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4573, "duration": 11.676, "id": "EN_B00000_S02862_W000121", "language": "en", "speaker": "EN_B00000_S02862", "text": " You need to have two times this. Uhm, okay, so just a quick recap here. You know, what you put in this right hand side is either like a Q or you multiply a row times a volume....
EN_B00000_S02862_W000121.mp3
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EN_B00000_S02862_W000122
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.4193, "duration": 11.932, "id": "EN_B00000_S02862_W000122", "language": "en", "speaker": "EN_B00000_S02862", "text": " Or, you might have to integrate rho dv. If it's spherical, you're gonna be like, okay, integral rho dv, dv for spherical was 4 pi r squared dr, that was for spherical.", "wa...
EN_B00000_S02862_W000122.mp3
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EN_B00000_S02862_W000123
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.3476, "duration": 17.893, "id": "EN_B00000_S02862_W000123", "language": "en", "speaker": "EN_B00000_S02862", "text": " dv for the cylindrical case, and this was dv for the spherical case. How do you figure those out? Remember just write down the volume. Would be pi r squared h. Take a derivati...
EN_B00000_S02862_W000123.mp3
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EN_B00000_S02872_W000000
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.1833, "duration": 8.319, "id": "EN_B00000_S02872_W000000", "language": "en", "speaker": "EN_B00000_S02872", "text": " It was so good. And John picked it. He just started smiling. And it was like, yeaah, yeaah. Ah, the perfect cutaway.", "wav": "EN_B00000/EN_B00000_S02872/mp3/EN_B00000_S02872...
EN_B00000_S02872_W000000.mp3
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EN_B00000_S02882_W000000
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2442, "duration": 12.156, "id": "EN_B00000_S02882_W000000", "language": "en", "speaker": "EN_B00000_S02882", "text": " Nintendo promised so much and delivered so little when it originally released back on the Nintendo Switch a few years ago. It's since seen price drops every single day and als...
EN_B00000_S02882_W000000.mp3
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EN_B00000_S02882_W000001
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.2775, "duration": 13.141, "id": "EN_B00000_S02882_W000001", "language": "en", "speaker": "EN_B00000_S02882", "text": " Her interjections come far too frequently and her delivery of the character is like something out of Desperate Housewives. It feels incredibly at odds with the science fiction...
EN_B00000_S02882_W000001.mp3
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EN_B00000_S02882_W000002
hf://datasets/amphion/Emilia-Dataset@bcaad00d13e7c101485990a46e88f5884ffed3fc/EN/EN-B000002.tar
{ "dnsmos": 3.0099, "duration": 12.54, "id": "EN_B00000_S02882_W000002", "language": "en", "speaker": "EN_B00000_S02882", "text": " As far as gameplay and controls go, Generic doesn't even come close. To summarize the game in a single sentence, move into a space, kill all of the enemies, move on to the next...
EN_B00000_S02882_W000002.mp3
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