1 00:00:01,464 --> 00:00:02,710 - [Voiceover] In the last video, we talked about 2 00:00:02,710 --> 00:00:04,388 the helium nucleus, which contains 3 00:00:04,388 --> 00:00:07,223 two protons and two neutrons. 4 00:00:07,223 --> 00:00:08,919 Protons and neutrons in the nucleus 5 00:00:08,919 --> 00:00:11,148 are called nucleons, and so I'll 6 00:00:11,148 --> 00:00:13,970 use that term a few times in this video. 7 00:00:13,971 --> 00:00:16,204 Here's a picture of the nucleus, 8 00:00:16,204 --> 00:00:18,066 with two protons and two neutrons, 9 00:00:18,066 --> 00:00:19,794 and we know it's stable, 10 00:00:19,794 --> 00:00:22,156 even though we know like charges repel. 11 00:00:22,156 --> 00:00:24,128 And so these two protons are repelling 12 00:00:24,128 --> 00:00:27,442 each other, and that's the electrostatic force. 13 00:00:27,442 --> 00:00:29,498 So let me go ahead and write that here. 14 00:00:29,498 --> 00:00:32,603 The electrostatic force says like charges repel. 15 00:00:32,603 --> 00:00:34,659 We know that this nucleus is stable, 16 00:00:34,659 --> 00:00:36,595 so there must be something else 17 00:00:36,595 --> 00:00:38,371 holding the nucleus together, 18 00:00:38,371 --> 00:00:41,186 which we call the strong force. 19 00:00:41,186 --> 00:00:43,234 So the nuclear strong force is 20 00:00:43,234 --> 00:00:46,975 stronger than the electrostatic force. 21 00:00:46,975 --> 00:00:49,298 The strong force acts only over 22 00:00:49,298 --> 00:00:51,935 short distances though, but it does act 23 00:00:51,935 --> 00:00:53,969 between all nucleons. 24 00:00:53,969 --> 00:00:56,557 For example, a proton-proton interaction 25 00:00:56,557 --> 00:00:59,421 is the same as a proton-neutron interaction, 26 00:00:59,421 --> 00:01:02,710 which is the same as a neutron-neutron interaction. 27 00:01:02,710 --> 00:01:03,580 You can get into much more detail 28 00:01:03,580 --> 00:01:05,193 about the strong force. 29 00:01:05,193 --> 00:01:07,253 That's not really the point of this video. 30 00:01:07,253 --> 00:01:10,671 The point is that this nucleus is stable. 31 00:01:10,671 --> 00:01:12,284 And let's think about why. 32 00:01:12,284 --> 00:01:15,215 We have equal numbers of protons and neutrons, 33 00:01:15,215 --> 00:01:16,892 and so that's interesting. 34 00:01:16,892 --> 00:01:20,140 So let's think about the atomic number, 35 00:01:20,140 --> 00:01:23,011 which tells us the number of protons, 36 00:01:23,011 --> 00:01:25,099 which we represent by Z. 37 00:01:25,099 --> 00:01:27,853 And the number of neutrons we could say is capital N. 38 00:01:27,853 --> 00:01:31,060 So if we're concerned with the ratio, 39 00:01:31,060 --> 00:01:34,465 the ratio of neutrons to protons, 40 00:01:34,465 --> 00:01:37,247 so the N to Z ratio. 41 00:01:37,247 --> 00:01:40,352 In this example, we have two protons and two neutrons. 42 00:01:40,352 --> 00:01:44,660 So two neutrons over two protons is equal to one. 43 00:01:44,660 --> 00:01:47,313 We have N to Z ratio of one. 44 00:01:47,313 --> 00:01:49,833 It turns out that nuclei that have small numbers 45 00:01:49,833 --> 00:01:53,788 of protons, so if we're talking about Z is less than 20, 46 00:01:53,788 --> 00:01:55,768 they have stable nuclei 47 00:01:55,768 --> 00:01:58,228 when the N to Z ratio is equal to one. 48 00:01:58,228 --> 00:02:01,767 So when N over Z is equal to one, 49 00:02:01,767 --> 00:02:04,036 you can say you have a stable nucleus, 50 00:02:04,036 --> 00:02:06,567 so equal numbers of protons and neutrons 51 00:02:06,567 --> 00:02:07,686 turns out to be stable. 52 00:02:07,686 --> 00:02:11,586 So for this example, the helium-four nucleus is stable. 53 00:02:11,678 --> 00:02:15,458 Thinking about that, let's look at carbon-14 next. 54 00:02:15,458 --> 00:02:18,098 We have carbon-14, so let's get 55 00:02:18,098 --> 00:02:20,138 a little space right down here. 56 00:02:20,138 --> 00:02:23,178 So carbon-14 atomic number of six. 57 00:02:23,178 --> 00:02:27,395 Therefore, carbon has six protons in the nucleus. 58 00:02:27,830 --> 00:02:29,942 So there are six protons. 59 00:02:29,942 --> 00:02:32,086 Number of neutrons will be 14 minus six, 60 00:02:32,086 --> 00:02:34,582 so eight neutrons. 61 00:02:34,582 --> 00:02:37,478 So what's the neutron to proton ratio? 62 00:02:37,478 --> 00:02:40,676 So what's the N to Z ratio here? 63 00:02:40,676 --> 00:02:42,286 Well the N to Z ratio would be 64 00:02:42,286 --> 00:02:44,637 eight neutrons and six protons, 65 00:02:44,637 --> 00:02:47,952 and obviously that number is greater than one, 66 00:02:47,952 --> 00:02:50,221 so we have an unstable nucleus. 67 00:02:50,221 --> 00:02:53,741 The carbon-14 nucleus is unstable, 68 00:02:53,741 --> 00:02:56,158 it's radioactive, it's going to 69 00:02:56,158 --> 00:02:58,950 undergo spontaneous decay. 70 00:02:58,950 --> 00:03:00,621 It's going to try to get a better 71 00:03:00,621 --> 00:03:03,100 neutron to proton ratio. 72 00:03:03,100 --> 00:03:05,825 So let's look at the nuclear equation 73 00:03:05,825 --> 00:03:10,029 which represents the spontaneous decay of carbon-14. 74 00:03:10,029 --> 00:03:12,944 So here is our nuclear equation. 75 00:03:12,944 --> 00:03:15,865 And when you're writing nuclear equations, 76 00:03:15,865 --> 00:03:19,104 you're representing only the nuclei here, 77 00:03:19,104 --> 00:03:22,064 so for example, on the left side 78 00:03:22,064 --> 00:03:24,383 of my nuclear equation, I have carbon-14, 79 00:03:24,383 --> 00:03:26,543 we're talking about only the nucleus, 80 00:03:26,543 --> 00:03:29,168 so we're talking about six protons 81 00:03:29,168 --> 00:03:31,924 and eight neutrons in the nucleus. 82 00:03:31,924 --> 00:03:33,991 And so let's look and see what happens here. 83 00:03:33,991 --> 00:03:38,020 So carbon-14, the nucleus, the carbon-14 nucleus 84 00:03:38,020 --> 00:03:40,330 is actually going to give off an electron, 85 00:03:40,330 --> 00:03:41,698 and so that's pretty weird, 86 00:03:41,698 --> 00:03:45,688 and we'll talk about more why in the next video. 87 00:03:45,688 --> 00:03:50,688 It's a conversion that's governed by the weak nuclear force. 88 00:03:51,697 --> 00:03:54,637 But we know that an electron has a negative one charge, 89 00:03:54,637 --> 00:03:56,630 and so that's what we're talking about here. 90 00:03:56,630 --> 00:03:58,370 Here for carbon, we have six protons, 91 00:03:58,370 --> 00:04:01,060 let me go and write that, six protons here. 92 00:04:01,060 --> 00:04:02,982 An electron has a negative one charge, 93 00:04:02,982 --> 00:04:06,016 let's write a negative one charge here for the electron. 94 00:04:06,016 --> 00:04:09,650 The carbon-14 nucleus is turning into 95 00:04:09,650 --> 00:04:12,489 the nucleus for nitrogen here. 96 00:04:12,489 --> 00:04:14,522 Let's look at what we have. 97 00:04:14,522 --> 00:04:17,265 Our atomic number is seven, 98 00:04:17,265 --> 00:04:18,697 so we have seven protons, 99 00:04:18,697 --> 00:04:20,579 let's go ahead and write that here. 100 00:04:20,579 --> 00:04:25,579 Seven protons, and 14 minus 7 gives us seven neutrons. 101 00:04:26,623 --> 00:04:28,584 So we look at the mass number here, 102 00:04:28,584 --> 00:04:30,784 so 14 minus seven gives us seven neutrons. 103 00:04:30,784 --> 00:04:34,640 And so that ratio, the ratio of neutrons 104 00:04:34,640 --> 00:04:37,631 to protons is seven over seven, 105 00:04:37,631 --> 00:04:38,975 which is equal to one. 106 00:04:38,975 --> 00:04:43,738 That implies that we have a stable nucleus here. 107 00:04:44,862 --> 00:04:49,148 That's the reason why carbon-14 undergoes radioactive decay. 108 00:04:49,148 --> 00:04:51,862 Let's look at more details about a nuclear equation, 109 00:04:51,862 --> 00:04:53,373 because that's really what I'm most concerned about 110 00:04:53,373 --> 00:04:55,598 here in this video. 111 00:04:56,688 --> 00:04:59,858 The number of nucleons is conserved. 112 00:04:59,858 --> 00:05:01,675 Let's use a different color here. 113 00:05:01,675 --> 00:05:04,009 We have 14 nucleons on the left. 114 00:05:04,009 --> 00:05:06,467 We have six protons and eight neutrons. 115 00:05:06,467 --> 00:05:09,684 And on the right, we also have 14 nucleons, 116 00:05:09,684 --> 00:05:12,053 seven protons and seven neutrons, 117 00:05:12,053 --> 00:05:16,173 so obviously an electron is not a proton or a neutron. 118 00:05:16,173 --> 00:05:20,693 Nucleons are conserved, so we have 14 on the left, 119 00:05:20,693 --> 00:05:24,021 and we have zero plus 14 on the right. 120 00:05:24,021 --> 00:05:25,251 Also charge is conserved, 121 00:05:25,251 --> 00:05:26,748 and so that's what we see down here. 122 00:05:26,847 --> 00:05:29,020 We have six positive charges on the left side. 123 00:05:29,020 --> 00:05:31,079 On the right side, we have one negative charge 124 00:05:31,079 --> 00:05:32,879 and seven positive charges, 125 00:05:32,879 --> 00:05:36,236 so negative one and seven give us plus six, 126 00:05:36,236 --> 00:05:37,340 so we have plus six. 127 00:05:37,340 --> 00:05:39,496 So nucleons are conserved 128 00:05:39,496 --> 00:05:41,961 and charge is conserved in a nuclear equation. 129 00:05:41,961 --> 00:05:43,610 And notice what happened here. 130 00:05:43,610 --> 00:05:45,616 We changed the identity. 131 00:05:45,616 --> 00:05:48,353 We went from carbon to nitrogen, 132 00:05:48,353 --> 00:05:50,345 because we changed the number of protons. 133 00:05:50,345 --> 00:05:53,062 We went from six protons to seven protons, 134 00:05:53,062 --> 00:05:55,828 and so that's the idea of transmutations, 135 00:05:55,828 --> 00:05:59,732 of changing one element into another element. 136 00:06:01,424 --> 00:06:04,618 For nuclei with small numbers of protons, 137 00:06:04,626 --> 00:06:08,975 the N to Z ratio, the ideal one is one to one. 138 00:06:11,343 --> 00:06:12,954 For nuclei with more protons, 139 00:06:12,954 --> 00:06:16,390 it turns out the ratio changes, so let's look at that. 140 00:06:16,390 --> 00:06:18,665 As you increase the number of protons, 141 00:06:18,665 --> 00:06:21,592 the ratio changes for a stable nucleus. 142 00:06:21,592 --> 00:06:26,592 The N to Z ratio turns out to be 1.5, 143 00:06:27,053 --> 00:06:30,095 so as you increase in Z, 144 00:06:30,095 --> 00:06:32,807 so as you go above Z is equal to 20. 145 00:06:32,807 --> 00:06:34,326 As you get more and more protons, 146 00:06:34,326 --> 00:06:36,254 you need more neutrons. 147 00:06:36,254 --> 00:06:37,624 You need more neutrons, 148 00:06:37,624 --> 00:06:39,310 and let's think about why. 149 00:06:39,310 --> 00:06:41,382 If I have a bigger nucleus here, 150 00:06:41,382 --> 00:06:44,509 so this is a very poor representation of a nucleus. 151 00:06:44,509 --> 00:06:46,950 I think about two protons, let me use, 152 00:06:46,950 --> 00:06:48,379 I'll use magenta here. 153 00:06:48,379 --> 00:06:52,155 So I'll have two protons really close to each other. 154 00:06:52,155 --> 00:06:56,696 We know that there is a weak electrostatic repulsion here, 155 00:06:56,696 --> 00:06:59,385 and there's a strong nuclear force. 156 00:06:59,385 --> 00:07:04,105 There's a strong nuclear force between those protons. 157 00:07:04,489 --> 00:07:06,522 The strong nuclear force wins, 158 00:07:06,522 --> 00:07:09,633 but this is only when you're talking about short distances. 159 00:07:09,633 --> 00:07:12,625 Remember the strong force acts only over short distances. 160 00:07:12,625 --> 00:07:16,022 So if you have protons that are far away from each other, 161 00:07:16,022 --> 00:07:18,893 so these two protons here are far away from each other, 162 00:07:18,893 --> 00:07:20,738 there's still a repulsive force. 163 00:07:20,738 --> 00:07:23,081 The electrostatic force is still present, 164 00:07:23,081 --> 00:07:24,826 so they're still repelling each other. 165 00:07:24,826 --> 00:07:27,386 But you don't have the strong force any more. 166 00:07:27,386 --> 00:07:29,417 And because you don't have the strong force any more, 167 00:07:29,417 --> 00:07:32,353 eventually as you keep increasing the number of protons, 168 00:07:32,353 --> 00:07:35,304 you're increasing in the electrostatic force, 169 00:07:35,304 --> 00:07:37,381 and you get to a point where you need more 170 00:07:37,381 --> 00:07:39,141 of the strong force, and so you need 171 00:07:39,141 --> 00:07:42,608 to add in more neutrons to balance things out. 172 00:07:42,608 --> 00:07:44,976 So you need to add in more neutrons here, 173 00:07:44,976 --> 00:07:47,409 and that's the reason for this increased ratio. 174 00:07:47,409 --> 00:07:49,465 You need more neutrons as you increase 175 00:07:49,465 --> 00:07:52,614 the number of protons here. 176 00:07:53,289 --> 00:07:57,524 When you get beyond approximately 83, 177 00:07:57,524 --> 00:07:59,654 so let me go ahead and write this down here, 178 00:07:59,654 --> 00:08:01,798 so once you get an atomic 179 00:08:01,798 --> 00:08:04,730 number greater than 83, so bismuth, 180 00:08:04,730 --> 00:08:07,291 the repulsive force of the protons, 181 00:08:07,291 --> 00:08:10,794 this electrostatic repulsive force that we talked about here 182 00:08:10,794 --> 00:08:13,297 is so great that pretty much all 183 00:08:13,297 --> 00:08:15,378 of the nuclei are unstable, 184 00:08:15,378 --> 00:08:17,878 and will undergo radioactive decay. 185 00:08:18,385 --> 00:08:20,142 We'll talk in the next video about 186 00:08:20,142 --> 00:00:00,000 the types of radioactive decay that you might see.