1 00:00:00,360 --> 00:00:01,800 - [Lecturer] An atomic bomb 2 00:00:01,800 --> 00:00:03,330 and a nuclear power plant 3 00:00:03,330 --> 00:00:05,640 works on the same basic principle, 4 00:00:05,640 --> 00:00:07,770 nuclear fission chain reactions. 5 00:00:07,770 --> 00:00:09,810 But what exactly is this? 6 00:00:09,810 --> 00:00:11,280 And more importantly, 7 00:00:11,280 --> 00:00:13,650 if the same thing is happening inside both a bomb 8 00:00:13,650 --> 00:00:15,030 and a nuclear reactor, 9 00:00:15,030 --> 00:00:18,150 then why doesn't a nuclear reactor just explode like a bomb? 10 00:00:18,150 --> 00:00:19,950 What's the difference? 11 00:00:19,950 --> 00:00:21,840 Well, let's find out. 12 00:00:21,840 --> 00:00:24,090 So what is nuclear fission? 13 00:00:24,090 --> 00:00:26,220 Well, the word fission means breaking. 14 00:00:26,220 --> 00:00:29,100 So nuclear fission is a nuclear reaction 15 00:00:29,100 --> 00:00:33,510 in which a heavy nucleus breaks into smaller nuclei. 16 00:00:33,510 --> 00:00:35,400 But how does it break exactly? 17 00:00:35,400 --> 00:00:38,010 Well, one way is for it to break spontaneously. 18 00:00:38,010 --> 00:00:39,570 It can happen all by itself 19 00:00:39,570 --> 00:00:41,280 without us having to do anything. 20 00:00:41,280 --> 00:00:43,260 But we usually call that radioactivity, 21 00:00:43,260 --> 00:00:46,230 or we sometimes also call it spontaneous fission. 22 00:00:46,230 --> 00:00:48,420 But when we usually say nuclear fission, 23 00:00:48,420 --> 00:00:50,460 we're talking about the ones where we break it 24 00:00:50,460 --> 00:00:55,050 by specifically bombarding it with a neutron. 25 00:00:55,050 --> 00:00:58,290 Think about it, this nucleus is already unstable. 26 00:00:58,290 --> 00:01:00,690 Now you add another neutron to it, 27 00:01:00,690 --> 00:01:02,040 it makes it more unstable, 28 00:01:02,040 --> 00:01:03,540 kind of like pushing it over the edge 29 00:01:03,540 --> 00:01:06,240 and then it breaks into smaller nuclei. 30 00:01:06,240 --> 00:01:07,980 And here when it breaks, 31 00:01:07,980 --> 00:01:10,350 you also end up getting a few neutrons. 32 00:01:10,350 --> 00:01:11,183 You get somewhere between 33 00:01:11,183 --> 00:01:13,200 one to three neutrons usually out. 34 00:01:13,200 --> 00:01:14,850 So let's take an example. 35 00:01:14,850 --> 00:01:19,850 If you take Uranium 235, an isotope of uranium, 36 00:01:20,070 --> 00:01:22,680 and if you bombarded with a neutron, 37 00:01:22,680 --> 00:01:27,680 then it can break into Strontium 94 and Xenon 140. 38 00:01:27,930 --> 00:01:30,150 We don't have to remember the numbers or anything, 39 00:01:30,150 --> 00:01:31,230 don't worry about it. 40 00:01:31,230 --> 00:01:32,910 But my question would be, can we predict 41 00:01:32,910 --> 00:01:35,040 how many neutrons we'll get over here? 42 00:01:35,040 --> 00:01:35,910 Well, we can. 43 00:01:35,910 --> 00:01:36,750 All we have to do, 44 00:01:36,750 --> 00:01:38,100 just like any nuclear reaction, 45 00:01:38,100 --> 00:01:40,200 is to keep track of protons and neutrons. 46 00:01:40,200 --> 00:01:41,880 So if I keep track of protons, let's see, 47 00:01:41,880 --> 00:01:44,340 I have 92 protons on the left hand side. 48 00:01:44,340 --> 00:01:46,200 How many protons do I have on the right hand side? 49 00:01:46,200 --> 00:01:48,117 Well, eight plus four is two, so 12. 50 00:01:48,117 --> 00:01:49,080 So five plus three. 51 00:01:49,080 --> 00:01:50,433 I get 92 over here. 52 00:01:51,420 --> 00:01:53,280 But what about the total number of particles? 53 00:01:53,280 --> 00:01:56,640 Well, I have 235 plus one that is 230... 54 00:01:56,640 --> 00:02:00,750 Oops, that is 236 on the left hand side. 55 00:02:00,750 --> 00:02:02,880 But over here, 94 plus 140. 56 00:02:02,880 --> 00:02:04,590 So I get four. 57 00:02:04,590 --> 00:02:06,120 Nine plus four is 13. 58 00:02:06,120 --> 00:02:08,640 So one carry over, I get 234. 59 00:02:08,640 --> 00:02:11,070 So there are only 234 particles over here, 60 00:02:11,070 --> 00:02:13,440 which means two particles must have been released. 61 00:02:13,440 --> 00:02:15,180 And these must be two neutrons 62 00:02:15,180 --> 00:02:17,850 because we've already accounted for all the protons. 63 00:02:17,850 --> 00:02:19,050 So that's how I know 64 00:02:19,050 --> 00:02:23,280 that there must be two neutrons released over here. 65 00:02:23,280 --> 00:02:25,500 But you know what's cool about nuclear fission reactions? 66 00:02:25,500 --> 00:02:26,700 For the same reactants, 67 00:02:26,700 --> 00:02:29,430 you could get completely different products altogether. 68 00:02:29,430 --> 00:02:32,940 For example, if we take another uranium 235 69 00:02:32,940 --> 00:02:34,410 and bombard it with another neutron, 70 00:02:34,410 --> 00:02:36,930 look exactly the same reactance, 71 00:02:36,930 --> 00:02:40,320 but this time you might get completely different products. 72 00:02:40,320 --> 00:02:44,280 You might get Barium 141 and say Krypton 92. 73 00:02:44,280 --> 00:02:46,800 Again, we'll get some amount of neutrons, 74 00:02:46,800 --> 00:02:48,090 when you pause the video over here 75 00:02:48,090 --> 00:02:49,650 and try it yourself to figure out 76 00:02:49,650 --> 00:02:52,410 how many number of neutrons we should be getting here. 77 00:02:52,410 --> 00:02:54,000 Alright, again, we can see 78 00:02:54,000 --> 00:02:56,550 the number of protons is balanced. 79 00:02:56,550 --> 00:02:59,490 You have 56 plus 36 is 92. 80 00:02:59,490 --> 00:03:01,350 But how many total particles we have? 81 00:03:01,350 --> 00:03:03,570 We have 236 here again, 82 00:03:03,570 --> 00:03:05,494 this time we have one plus 2, 3, 83 00:03:05,494 --> 00:03:07,280 14 plus nine is 23. 84 00:03:07,280 --> 00:03:09,810 So you get 233, which means look, 85 00:03:09,810 --> 00:03:11,670 three particles are missing. 86 00:03:11,670 --> 00:03:15,630 So this time we'll get three neutrons. 87 00:03:15,630 --> 00:03:17,700 And just like with the fusion reactions, 88 00:03:17,700 --> 00:03:21,060 we will see even here, some energy is released 89 00:03:21,060 --> 00:03:24,030 and energy is released usually as kinetic energy 90 00:03:24,030 --> 00:03:26,460 of the products and the neutrons. 91 00:03:26,460 --> 00:03:28,890 And because energy is released 92 00:03:28,890 --> 00:03:31,680 and remember that energy and mass are equivalent, 93 00:03:31,680 --> 00:03:34,500 we will find that the mass of the products 94 00:03:34,500 --> 00:03:38,370 will be smaller than the mass of the reactants. 95 00:03:38,370 --> 00:03:41,760 And just by figuring out the difference in the mass, 96 00:03:41,760 --> 00:03:43,800 you can figure out how much energy was released. 97 00:03:43,800 --> 00:03:45,360 That difference in the mass is basically 98 00:03:45,360 --> 00:03:46,740 what got released as energy. 99 00:03:46,740 --> 00:03:48,330 Again, something that we've seen before 100 00:03:48,330 --> 00:03:50,520 in the nuclear fusion reactions, very similar. 101 00:03:50,520 --> 00:03:53,790 Now, can any heavy nucleus give you fission reactions? 102 00:03:53,790 --> 00:03:55,860 No, that can't happen. 103 00:03:55,860 --> 00:03:58,605 The ones that do, we call them fissile nuclei. 104 00:03:58,605 --> 00:04:01,230 So uranium 235 is fissile 105 00:04:01,230 --> 00:04:03,390 because it does undergo fission reaction 106 00:04:03,390 --> 00:04:05,430 and gives you energy. 107 00:04:05,430 --> 00:04:08,970 But if you consider another isotope of uranium, 108 00:04:08,970 --> 00:04:13,920 which is say Uranium 92, 238, 109 00:04:13,920 --> 00:04:16,593 turns out it is non-fissile. 110 00:04:18,030 --> 00:04:21,510 It does not undergo nuclear fission easily. 111 00:04:21,510 --> 00:04:23,100 And if you're wondering why certain nuclei 112 00:04:23,100 --> 00:04:26,640 are fissile and others are not, 113 00:04:26,640 --> 00:04:27,630 well, it has something to do 114 00:04:27,630 --> 00:04:29,460 with energy and stability. 115 00:04:29,460 --> 00:04:31,320 Well, turns out for uranium, 116 00:04:31,320 --> 00:04:32,850 when it undergoes fission, 117 00:04:32,850 --> 00:04:34,710 you end up getting more stable products 118 00:04:34,710 --> 00:04:36,630 and therefore energy is released. 119 00:04:36,630 --> 00:04:39,180 Turns out that's not the case for Uranium 238, 120 00:04:39,180 --> 00:04:41,100 or at least that's not very easy to happen. 121 00:04:41,100 --> 00:04:43,350 But of course we'll not dive too much into it. 122 00:04:43,350 --> 00:04:45,390 But a big question now we could ask ourselves is 123 00:04:45,390 --> 00:04:47,670 how much energy do we get out of it? 124 00:04:47,670 --> 00:04:50,100 Well, if you look at a single reaction, 125 00:04:50,100 --> 00:04:52,590 of course we'll get a tiny amount of energy. 126 00:04:52,590 --> 00:04:55,290 But if you want to get usable amount, 127 00:04:55,290 --> 00:04:58,680 then we will require lots and lots of reactions. 128 00:04:58,680 --> 00:05:00,870 But how do we do that practically? 129 00:05:00,870 --> 00:05:02,730 Because nuclear fission 130 00:05:02,730 --> 00:05:07,620 requires you to bombard a nucleus with neutron. 131 00:05:07,620 --> 00:05:09,390 So how do we ensure we get lots 132 00:05:09,390 --> 00:05:11,730 and lots of reactions like this? 133 00:05:11,730 --> 00:05:13,980 Well, the answer is right in front of us. 134 00:05:13,980 --> 00:05:15,690 Since each nuclear fission reaction 135 00:05:15,690 --> 00:05:17,400 gives us a few neutrons, 136 00:05:17,400 --> 00:05:19,230 if we can ensure that these neutrons 137 00:05:19,230 --> 00:05:23,400 go and hit other uranium 235 atoms, nuclei, sorry, 138 00:05:23,400 --> 00:05:25,560 then they will again undergo fission 139 00:05:25,560 --> 00:05:26,970 and give you more neutrons 140 00:05:26,970 --> 00:05:29,340 and each cause even more fission reaction. 141 00:05:29,340 --> 00:05:30,780 Here's the way we can show that. 142 00:05:30,780 --> 00:05:33,300 So let me just go to the next page. 143 00:05:33,300 --> 00:05:34,290 Here we go. 144 00:05:34,290 --> 00:05:36,600 So if you have one neutron that bombards 145 00:05:36,600 --> 00:05:40,770 with a uranium 235 giving you energy, fission reaction, 146 00:05:40,770 --> 00:05:42,690 giving you energy and some neutrons. 147 00:05:42,690 --> 00:05:44,970 Now if these neutrons could go 148 00:05:44,970 --> 00:05:49,230 and hit even more of these urine 235, 149 00:05:49,230 --> 00:05:51,180 then you'll get even more energy 150 00:05:51,180 --> 00:05:53,065 and this thing can keep on going 151 00:05:53,065 --> 00:05:54,872 and you can see very quickly 152 00:05:54,872 --> 00:05:56,730 this will keep increasing. 153 00:05:56,730 --> 00:05:59,310 You'll have one fission, then you have three fission, 154 00:05:59,310 --> 00:06:01,620 and then you'll have nine and so on and so forth. 155 00:06:01,620 --> 00:06:03,120 So the amount of fission happening per second 156 00:06:03,120 --> 00:06:04,680 would just keep increasing. 157 00:06:04,680 --> 00:06:09,420 This is what we call a chain reaction. 158 00:06:09,420 --> 00:06:12,090 Nuclear chain reactions can be quite devastating. 159 00:06:12,090 --> 00:06:14,220 You start with very few reactions per second, 160 00:06:14,220 --> 00:06:17,940 but very quickly, very rapidly, that number increases. 161 00:06:17,940 --> 00:06:19,680 And within a short amount of time, 162 00:06:19,680 --> 00:06:22,890 you can release tremendous amount of energy. 163 00:06:22,890 --> 00:06:27,390 That is the whole idea behind atomic bombs. 164 00:06:27,390 --> 00:06:29,910 What makes atomic bombs so much more devastating 165 00:06:29,910 --> 00:06:32,010 compared to traditional regular bombs 166 00:06:32,010 --> 00:06:33,990 is that we are dealing with nuclear energy, 167 00:06:33,990 --> 00:06:35,700 which is hoarders of magnitude higher 168 00:06:35,700 --> 00:06:37,320 than the chemical energy 169 00:06:37,320 --> 00:06:38,700 that we get from traditional bombs. 170 00:06:38,700 --> 00:06:40,590 So a small amount of fissile material 171 00:06:40,590 --> 00:06:44,880 can give you a lot of energy, but that's not it. 172 00:06:44,880 --> 00:06:45,780 That's not it. 173 00:06:45,780 --> 00:06:47,730 You see, the products of nuclear fission reactions 174 00:06:47,730 --> 00:06:50,100 are usually radioactive, 175 00:06:50,100 --> 00:06:52,590 which means even after the explosion is done, 176 00:06:52,590 --> 00:06:54,360 the whole area is contaminated 177 00:06:54,360 --> 00:06:56,070 with radioactive isotopes now, 178 00:06:56,070 --> 00:06:58,530 which can further cause damage for ears to come, 179 00:06:58,530 --> 00:07:00,480 making that whole area inhabitable. 180 00:07:00,480 --> 00:07:03,480 So yeah, atomic bombs are really destructive. 181 00:07:03,480 --> 00:07:05,370 But on the flip side, if you're using this 182 00:07:05,370 --> 00:07:07,170 to generate electricity, let's say, 183 00:07:07,170 --> 00:07:09,300 then we'll get way more energy 184 00:07:09,300 --> 00:07:11,400 compared to what we get from fossil fuels. 185 00:07:11,400 --> 00:07:13,770 Because again, there we are dealing with chemical energy. 186 00:07:13,770 --> 00:07:16,410 And of course, another advantage of using nuclear energy 187 00:07:16,410 --> 00:07:18,300 is that in fossil fuels, 188 00:07:18,300 --> 00:07:20,160 because you're using combustion reactions, 189 00:07:20,160 --> 00:07:23,130 there is CO2 that is released into the atmosphere. 190 00:07:23,130 --> 00:07:24,480 None of that happens over here. 191 00:07:24,480 --> 00:07:26,490 But now this brings us to the original question. 192 00:07:26,490 --> 00:07:28,320 How do we use chain reactions 193 00:07:28,320 --> 00:07:29,850 in nuclear power reactors 194 00:07:29,850 --> 00:07:31,080 to generate electricity? 195 00:07:31,080 --> 00:07:34,320 Wouldn't they just explore just like an atomic bomb? 196 00:07:34,320 --> 00:07:36,270 So what's the big difference? 197 00:07:36,270 --> 00:07:39,480 Well, the big difference is over here, 198 00:07:39,480 --> 00:07:40,620 when it comes to bombs, 199 00:07:40,620 --> 00:07:42,420 we are using uncontrolled chain reaction. 200 00:07:42,420 --> 00:07:44,340 Whatever we just saw right now, 201 00:07:44,340 --> 00:07:46,440 it's a about uncontrolled chain reaction. 202 00:07:46,440 --> 00:07:48,090 But when it comes to power... 203 00:07:48,090 --> 00:07:49,650 When it comes to nuclear reactors, 204 00:07:49,650 --> 00:07:51,840 we use controlled chain reactions. 205 00:07:51,840 --> 00:07:54,000 How do you control chain reactions, you ask? 206 00:07:54,000 --> 00:07:55,710 Well, one of the most common ways 207 00:07:55,710 --> 00:07:58,500 is by absorbing a lot of neutrons. 208 00:07:58,500 --> 00:08:01,380 So imagine we absorbed a lot of neutrons like this. 209 00:08:01,380 --> 00:08:03,420 Then look, by absorbing neutrons, 210 00:08:03,420 --> 00:08:05,580 you are controlling how many further 211 00:08:05,580 --> 00:08:07,230 fission reactions are happening. 212 00:08:07,230 --> 00:08:09,360 This way you can control it, 213 00:08:09,360 --> 00:08:13,860 you can ensure that the energy is released in a steady rate. 214 00:08:13,860 --> 00:08:17,670 And that's how you can get controlled chain reaction. 215 00:08:17,670 --> 00:08:19,380 But there's another major difference. 216 00:08:19,380 --> 00:08:20,580 Remember how we said earlier 217 00:08:20,580 --> 00:08:23,280 that uranium 238 is non fissile? 218 00:08:23,280 --> 00:08:25,500 Well, it turns out if you take a uranium ore 219 00:08:25,500 --> 00:08:28,293 then most of it is actually uranium 238. 220 00:08:29,130 --> 00:08:31,950 That means you cannot directly use a uranium ore 221 00:08:31,950 --> 00:08:35,400 either as a bomb or as a fuel for nuclear power plant. 222 00:08:35,400 --> 00:08:37,500 This means we have to take it through a process 223 00:08:37,500 --> 00:08:40,440 where we increase the amount of fissile material. 224 00:08:40,440 --> 00:08:42,540 And this process is called enrichment. 225 00:08:42,540 --> 00:08:44,100 And the big difference is 226 00:08:44,100 --> 00:08:46,680 if you're using a fuel for... 227 00:08:46,680 --> 00:08:48,570 You're using it for a bomb, 228 00:08:48,570 --> 00:08:51,240 then we would want a lot of enrichment. 229 00:08:51,240 --> 00:08:53,940 In fact, we'd want about 90% enriched. 230 00:08:53,940 --> 00:08:54,870 And that makes sense 231 00:08:54,870 --> 00:08:56,527 because you would want 232 00:08:56,527 --> 00:08:57,360 as many fission reactions happening 233 00:08:57,360 --> 00:08:58,770 as possible per second 234 00:08:58,770 --> 00:09:01,410 so that the whole thing explodes immediately. 235 00:09:01,410 --> 00:09:03,210 But when it comes to nuclear reactors, 236 00:09:03,210 --> 00:09:04,380 nuclear power plants, 237 00:09:04,380 --> 00:09:06,930 you see we have only about three to 5% enrichment. 238 00:09:06,930 --> 00:09:08,760 That means a single Uranium 235 239 00:09:08,760 --> 00:09:11,970 is surrounded by a lot of non-fissile materials. 240 00:09:11,970 --> 00:09:13,598 That's why you will... 241 00:09:13,598 --> 00:09:18,180 That's why the nuclear fuel will not explode like a bomb 242 00:09:18,180 --> 00:09:20,190 because it's not enriched as much 243 00:09:20,190 --> 00:09:21,600 as you would need for a bomb. 244 00:09:21,600 --> 00:09:24,630 So anyways, by using controlled chain reaction, 245 00:09:24,630 --> 00:09:27,960 we get energy as the kinetic energy of these products, 246 00:09:27,960 --> 00:09:29,820 which is then used to heat up water. 247 00:09:29,820 --> 00:09:31,860 And then the process is very similar 248 00:09:31,860 --> 00:09:33,960 to how any other power plant works. 249 00:09:33,960 --> 00:09:37,110 The heated water produces high pressure steam 250 00:09:37,110 --> 00:09:38,730 that turns turbines, 251 00:09:38,730 --> 00:09:40,950 and that's how you eventually get electricity. 252 00:09:40,950 --> 00:09:42,750 And then that hot steam 253 00:09:42,750 --> 00:09:45,150 is cooled in a cooling tower. 254 00:09:45,150 --> 00:09:48,300 And in the process a lot of water vapor is produced 255 00:09:48,300 --> 00:09:50,010 and that is released over here. 256 00:09:50,010 --> 00:09:52,050 I'm mentioning this because I used to think 257 00:09:52,050 --> 00:09:54,270 that this itself was a nuclear reactor 258 00:09:54,270 --> 00:09:56,340 and it was producing a lot of smoke, 259 00:09:56,340 --> 00:09:58,800 radioactive smoke, which could be dangerous 260 00:09:58,800 --> 00:10:00,240 because it's going into the atmosphere. 261 00:10:00,240 --> 00:10:01,920 But none of that 'cause first of all, 262 00:10:01,920 --> 00:10:03,270 this is just a cooling tower, 263 00:10:03,270 --> 00:10:05,430 and what is it releasing is water vapor. 264 00:10:05,430 --> 00:10:07,200 And that water never comes in contact 265 00:10:07,200 --> 00:10:09,060 with any of the radioactive material 266 00:10:09,060 --> 00:10:10,050 that you have over here. 267 00:10:10,050 --> 00:10:11,220 So it's not dangerous, 268 00:10:11,220 --> 00:10:15,480 but there will be radioactive products left over, 269 00:10:15,480 --> 00:10:18,660 radioactive waste inside the nuclear power plants, 270 00:10:18,660 --> 00:10:21,000 and that needs to be safely disposed. 271 00:10:21,000 --> 00:10:22,950 And that is a challenge that scientists 272 00:10:22,950 --> 00:10:25,683 and engineers are actively working on today.