1 00:00:00,000 --> 00:00:00,430 2 00:00:00,430 --> 00:00:02,960 SAL: In the last video we saw all sorts of different types 3 00:00:02,960 --> 00:00:06,630 of isotopes of atoms experiencing radioactive decay 4 00:00:06,630 --> 00:00:10,060 and turning into other atoms or releasing different types 5 00:00:10,060 --> 00:00:10,630 of particles. 6 00:00:10,630 --> 00:00:14,530 But the question is, when does an atom or 7 00:00:14,530 --> 00:00:16,360 nucleus decide to decay? 8 00:00:16,360 --> 00:00:20,820 Let's say I have a bunch of, let's say these are all atoms. 9 00:00:20,820 --> 00:00:24,780 I have a bunch of atoms here. 10 00:00:24,780 --> 00:00:26,970 And let's say we're talking about the type of decay where 11 00:00:26,970 --> 00:00:28,550 an atom turns into another atom. 12 00:00:28,550 --> 00:00:30,500 So your proton number is going to change. 13 00:00:30,500 --> 00:00:31,990 Your atomic number is going to change. 14 00:00:31,990 --> 00:00:35,490 So it could either be beta decay, which would release 15 00:00:35,490 --> 00:00:37,970 electrons from the neutrons and turn them into protons. 16 00:00:37,970 --> 00:00:40,520 Or maybe positron emission turning protons into neutrons. 17 00:00:40,520 --> 00:00:41,890 But that's not what's relevant here. 18 00:00:41,890 --> 00:00:44,070 Let's say we have a collection of atoms. And normally when we 19 00:00:44,070 --> 00:00:48,650 have any small amount of any element, we really have huge 20 00:00:48,650 --> 00:00:50,690 amounts of atoms of that element. 21 00:00:50,690 --> 00:00:54,540 And we've talked about moles and, you know, one gram of 22 00:00:54,540 --> 00:01:05,370 carbon-12-- I'm sorry, 12 grams-- 12 grams of carbon-12 23 00:01:05,370 --> 00:01:07,870 has one mole of carbon-12 in it. 24 00:01:07,870 --> 00:01:10,440 One mole of carbon-12. 25 00:01:10,440 --> 00:01:12,310 And what is one mole of carbon-12? 26 00:01:12,310 --> 00:01:19,170 That's 6.02 times 10 to the 23rd carbon-12 atoms. This is 27 00:01:19,170 --> 00:01:21,680 a ginormous number. 28 00:01:21,680 --> 00:01:24,820 This is more than we can, than my head can really grasp 29 00:01:24,820 --> 00:01:27,110 around how large of a number this is. 30 00:01:27,110 --> 00:01:30,290 And this is only when we have 12 grams. 12 grams is not a 31 00:01:30,290 --> 00:01:31,560 large mass. 32 00:01:31,560 --> 00:01:35,440 For example, one kilogram is about two pounds. 33 00:01:35,440 --> 00:01:37,525 So this is about, what? 34 00:01:37,525 --> 00:01:38,750 I want to say [? 1/50 ?] 35 00:01:38,750 --> 00:01:39,650 of a pound if I'm doing [? it. ?] 36 00:01:39,650 --> 00:01:43,500 But this is not a lot of mass right here. 37 00:01:43,500 --> 00:01:45,810 And pounds is obviously force. 38 00:01:45,810 --> 00:01:46,570 You get the idea. 39 00:01:46,570 --> 00:01:50,240 On Earth, well anywhere, mass is invariant. 40 00:01:50,240 --> 00:01:51,920 This is not a tremendous amount. 41 00:01:51,920 --> 00:01:54,140 So with that said, let's go back to the question of how do 42 00:01:54,140 --> 00:01:55,730 we know if one of these guys are going to 43 00:01:55,730 --> 00:01:56,870 decay in some way. 44 00:01:56,870 --> 00:01:59,710 And maybe not carbon-12, maybe we're talking about carbon-14 45 00:01:59,710 --> 00:02:00,240 or something. 46 00:02:00,240 --> 00:02:02,300 How do we know that they're going to decay? 47 00:02:02,300 --> 00:02:03,440 And the answer is, you don't. 48 00:02:03,440 --> 00:02:05,590 They all have some probability of the decaying. 49 00:02:05,590 --> 00:02:08,389 At any given moment, for a certain type of element or a 50 00:02:08,389 --> 00:02:11,360 certain type of isotope of an element, there's some 51 00:02:11,360 --> 00:02:13,840 probability that one of them will decay. 52 00:02:13,840 --> 00:02:16,790 That, you know, maybe this guy will decay this second. 53 00:02:16,790 --> 00:02:19,750 And then nothing happens for a long time, a long time, and 54 00:02:19,750 --> 00:02:22,600 all of a sudden two more guys decay. 55 00:02:22,600 --> 00:02:25,530 And so, like everything in chemistry, and a lot of what 56 00:02:25,530 --> 00:02:28,310 we're starting to deal with in physics and quantum mechanics, 57 00:02:28,310 --> 00:02:29,920 everything is probabilistic. 58 00:02:29,920 --> 00:02:32,570 I mean, maybe if we really got in detail on the 59 00:02:32,570 --> 00:02:34,900 configurations of the nucleus, maybe we could get a little 60 00:02:34,900 --> 00:02:36,990 bit better in terms of our probabilities, but we don't 61 00:02:36,990 --> 00:02:39,040 know what's going on inside of the nucleus, so all we can do 62 00:02:39,040 --> 00:02:42,630 is ascribe some probabilities to something reacting. 63 00:02:42,630 --> 00:02:46,040 Now you could say, OK, what's the probability of any given 64 00:02:46,040 --> 00:02:48,430 molecule reacting in one second? 65 00:02:48,430 --> 00:02:49,520 Or you could define it that way. 66 00:02:49,520 --> 00:02:52,320 But we're used to dealing with things on the macro level, on 67 00:02:52,320 --> 00:02:56,950 dealing with, you know, huge amounts of atoms. So what we 68 00:02:56,950 --> 00:02:59,220 do is we come up with terms that help us get our head 69 00:02:59,220 --> 00:03:00,200 around this. 70 00:03:00,200 --> 00:03:02,680 And one of those terms is the term half-life. 71 00:03:02,680 --> 00:03:06,930 72 00:03:06,930 --> 00:03:12,480 And let me erase this stuff down here. 73 00:03:12,480 --> 00:03:15,780 So I have a description, and we're going to hopefully get 74 00:03:15,780 --> 00:03:17,325 an intuition of what half-life means. 75 00:03:17,325 --> 00:03:20,730 So I wrote a decay reaction right here, 76 00:03:20,730 --> 00:03:22,780 where you have carbon-14. 77 00:03:22,780 --> 00:03:26,180 It decays into nitrogen-14. 78 00:03:26,180 --> 00:03:27,740 And we could just do a little bit of review. 79 00:03:27,740 --> 00:03:31,100 You go from six protons to seven protons. 80 00:03:31,100 --> 00:03:32,430 Your mass changes the same. 81 00:03:32,430 --> 00:03:34,870 So one of the neutrons must have turned into a proton and 82 00:03:34,870 --> 00:03:36,130 that is what happened. 83 00:03:36,130 --> 00:03:39,590 And it does that by releasing an electron, which is also 84 00:03:39,590 --> 00:03:40,630 call a beta particle. 85 00:03:40,630 --> 00:03:44,130 We could have written this as minus 1 charge. 86 00:03:44,130 --> 00:03:45,710 Relatively zero mass. 87 00:03:45,710 --> 00:03:47,455 It does have some mass, but they write zero. 88 00:03:47,455 --> 00:03:48,820 This is kind of notation. 89 00:03:48,820 --> 00:03:51,130 So this is beta decay. 90 00:03:51,130 --> 00:03:53,480 Beta decay, this is just a review. 91 00:03:53,480 --> 00:03:56,070 But the way we think about half-life is, people have 92 00:03:56,070 --> 00:04:01,260 studied carbon and they said, look, if I start off with 10 93 00:04:01,260 --> 00:04:08,450 grams-- if I have just a block of carbon that's 10 grams. If 94 00:04:08,450 --> 00:04:12,840 I wait carbon-14's half-life-- this is a 95 00:04:12,840 --> 00:04:14,300 specific isotope of carbon. 96 00:04:14,300 --> 00:04:19,890 Remember, isotopes, if there's carbon, can come in 12, with 97 00:04:19,890 --> 00:04:22,970 an atomic mass number of 12, or with 14, or I mean, there's 98 00:04:22,970 --> 00:04:24,790 different isotopes of different elements. 99 00:04:24,790 --> 00:04:28,860 And the atomic number defines the carbon, 100 00:04:28,860 --> 00:04:30,040 because it has six protons. 101 00:04:30,040 --> 00:04:31,440 Carbon-12 has six protons. 102 00:04:31,440 --> 00:04:34,090 Carbon-14 has six protons. 103 00:04:34,090 --> 00:04:35,490 But they have a different number of neutrons. 104 00:04:35,490 --> 00:04:37,440 So when you have the same element with varying number of 105 00:04:37,440 --> 00:04:39,110 neutrons, that's an isotope. 106 00:04:39,110 --> 00:04:44,080 So the carbon-14 version, or this isotope of carbon, let's 107 00:04:44,080 --> 00:04:46,940 say we start with 10 grams. If they say that it's half-life 108 00:04:46,940 --> 00:04:51,930 is 5,740 years, that means that if on day one we start 109 00:04:51,930 --> 00:04:57,090 off with 10 grams of pure carbon-14, after 5,740 years, 110 00:04:57,090 --> 00:04:59,200 half of this will have turned into 111 00:04:59,200 --> 00:05:01,980 nitrogen-14, by beta decay. 112 00:05:01,980 --> 00:05:05,270 And you might say, oh OK, so maybe-- let's see, let me make 113 00:05:05,270 --> 00:05:08,230 nitrogen magenta, right there-- so you might say, OK, 114 00:05:08,230 --> 00:05:11,660 maybe that half turns into nitrogen. 115 00:05:11,660 --> 00:05:14,520 And I've actually seen this drawn this way in some 116 00:05:14,520 --> 00:05:17,200 chemistry classes or physics classes, and my immediate 117 00:05:17,200 --> 00:05:19,470 question is how does this half know that it 118 00:05:19,470 --> 00:05:20,690 must turn into nitrogen? 119 00:05:20,690 --> 00:05:24,860 And how does this half know that it must stay as carbon? 120 00:05:24,860 --> 00:05:26,550 And the answer is they don't know. 121 00:05:26,550 --> 00:05:29,480 And it really shouldn't be drawn this way. 122 00:05:29,480 --> 00:05:30,760 So let me redraw it. 123 00:05:30,760 --> 00:05:37,010 So this is our original block of our carbon-14. 124 00:05:37,010 --> 00:05:41,230 What happens over that 5,740 years is that, 125 00:05:41,230 --> 00:05:45,000 probabilistically, some of these guys just start turning 126 00:05:45,000 --> 00:05:53,550 into nitrogen randomly, at random points. 127 00:05:53,550 --> 00:05:59,340 And over 5,740 years, you determine that there's a 50% 128 00:05:59,340 --> 00:06:03,000 chance that any one of these carbon atoms will turn into a 129 00:06:03,000 --> 00:06:03,950 nitrogen atom. 130 00:06:03,950 --> 00:06:08,600 So that after 5,740 years, the half-life of carbon, a 50% 131 00:06:08,600 --> 00:06:10,470 chance that any of the guys that are carbon 132 00:06:10,470 --> 00:06:11,450 will turn to nitrogen. 133 00:06:11,450 --> 00:06:15,890 So if you go back after a half-life, half of the atoms 134 00:06:15,890 --> 00:06:19,120 will now be nitrogen. 135 00:06:19,120 --> 00:06:22,350 So now you have, after one half-life-- So 136 00:06:22,350 --> 00:06:24,420 let's ignore this. 137 00:06:24,420 --> 00:06:27,550 So we started with this. 138 00:06:27,550 --> 00:06:29,200 All 10 grams were carbon. 139 00:06:29,200 --> 00:06:32,410 10 grams of c-14. 140 00:06:32,410 --> 00:06:36,110 This is after one half-life. 141 00:06:36,110 --> 00:06:41,400 And now we have five grams of c-14. 142 00:06:41,400 --> 00:06:47,140 And we have five grams of nitrogen-14. 143 00:06:47,140 --> 00:06:48,330 Fair enough. 144 00:06:48,330 --> 00:06:51,210 Let's think about what happens after another half-life. 145 00:06:51,210 --> 00:06:56,470 Well we said that during a half-life, 5,740 years in the 146 00:06:56,470 --> 00:06:59,280 case of carbon-14-- all different elements have a 147 00:06:59,280 --> 00:07:02,040 different half-life, if they're radioactive-- over 148 00:07:02,040 --> 00:07:06,180 5,740 years there's a 50%-- and if I just look at any one 149 00:07:06,180 --> 00:07:09,810 atom-- there's a 50% chance it'll decay. 150 00:07:09,810 --> 00:07:14,380 So if we go to another half-life, if we go another 151 00:07:14,380 --> 00:07:19,330 half-life from there, I had five grams of carbon-14. 152 00:07:19,330 --> 00:07:23,591 So let me actually copy and paste this one. 153 00:07:23,591 --> 00:07:25,350 This is what I started with. 154 00:07:25,350 --> 00:07:28,030 155 00:07:28,030 --> 00:07:31,115 Now after another half-life-- you can ignore all my little, 156 00:07:31,115 --> 00:07:33,390 actually let me erase some of this up here. 157 00:07:33,390 --> 00:07:36,260 Let me clean it up a little bit. 158 00:07:36,260 --> 00:07:39,380 After one one half-life, what happens? 159 00:07:39,380 --> 00:07:43,900 Well I now am left with five grams of carbon-14. 160 00:07:43,900 --> 00:07:48,230 Those five grams of carbon-14, every one of those atoms still 161 00:07:48,230 --> 00:07:54,150 has, over the next-- whatever that number was, 5,740 years-- 162 00:07:54,150 --> 00:07:57,300 after 5,740 years, all of those once 163 00:07:57,300 --> 00:07:58,740 again have a 50% chance. 164 00:07:58,740 --> 00:08:01,650 And by the law of large numbers, half of them will 165 00:08:01,650 --> 00:08:03,840 have converted into nitrogen-14. 166 00:08:03,840 --> 00:08:08,530 So we'll have even more conversion into nitrogen-14. 167 00:08:08,530 --> 00:08:11,240 So now half of that five grams. So now we're only left 168 00:08:11,240 --> 00:08:16,250 with 2.5 grams of c-14. 169 00:08:16,250 --> 00:08:17,690 And how much nitrogen-14? 170 00:08:17,690 --> 00:08:20,320 Well we have another two and a half went to nitrogen. 171 00:08:20,320 --> 00:08:26,190 So now we have seven and a half grams of nitrogen-14. 172 00:08:26,190 --> 00:08:32,730 And we could keep going further into the future, and 173 00:08:32,730 --> 00:08:38,539 after every half-life, 5,740 years, we will have half of 174 00:08:38,539 --> 00:08:39,620 the carbon that we started. 175 00:08:39,620 --> 00:08:40,710 But we'll always have an 176 00:08:40,710 --> 00:08:42,630 infinitesimal amount of carbon. 177 00:08:42,630 --> 00:08:43,700 But let me ask you a question. 178 00:08:43,700 --> 00:08:46,600 Let's say I'm just staring at one carbon atom. 179 00:08:46,600 --> 00:08:48,610 Let's say I just have this one carbon atom. 180 00:08:48,610 --> 00:08:51,080 You know, I've got its nucleus, with its c-14. 181 00:08:51,080 --> 00:08:53,780 So it's got its six protons. 182 00:08:53,780 --> 00:08:55,400 1, 2, 3, 4, 5, 6. 183 00:08:55,400 --> 00:08:58,910 It's got its eight neutrons. 184 00:08:58,910 --> 00:09:00,756 It's got its six electrons. 185 00:09:00,756 --> 00:09:04,870 1, 2, 3, 4, 5, 6, whatever. 186 00:09:04,870 --> 00:09:06,800 What's going to happen? 187 00:09:06,800 --> 00:09:13,130 What's going to happen after one second? 188 00:09:13,130 --> 00:09:15,180 Well, I don't know. 189 00:09:15,180 --> 00:09:18,320 It'll probably still be carbon, but there's some 190 00:09:18,320 --> 00:09:21,580 probability that after one second it will have already 191 00:09:21,580 --> 00:09:24,000 turned into nitrogen-14. 192 00:09:24,000 --> 00:09:29,710 What's going to happen after one billion years? 193 00:09:29,710 --> 00:09:31,960 Well, after one billion years I'll say, well you know, it'll 194 00:09:31,960 --> 00:09:35,660 probably have turned into nitrogen-14 at that point, but 195 00:09:35,660 --> 00:09:36,620 I'm not sure. 196 00:09:36,620 --> 00:09:39,690 This might be the one ultra-stable nucleus that just 197 00:09:39,690 --> 00:09:41,740 happened to, kind of, go against the 198 00:09:41,740 --> 00:09:43,960 odds and stay carbon-14. 199 00:09:43,960 --> 00:09:46,390 So after one half-life, if you're just looking at one 200 00:09:46,390 --> 00:09:52,280 atom after 5,740 years, you don't know whether this turned 201 00:09:52,280 --> 00:09:53,120 into a nitrogen or not. 202 00:09:53,120 --> 00:09:56,690 This exact atom, you just know that it had a 50% chance of 203 00:09:56,690 --> 00:09:57,950 turning into a nitrogen. 204 00:09:57,950 --> 00:10:02,130 Now, if you look at it over a huge number of atoms. I mean, 205 00:10:02,130 --> 00:10:04,340 if you start approaching, you know, Avogadro's number or 206 00:10:04,340 --> 00:10:06,350 anything larger-- I erased that. 207 00:10:06,350 --> 00:10:08,460 Then all of a sudden you can use the law of large numbers 208 00:10:08,460 --> 00:10:11,850 and say, OK, on average, if each of those atoms must have 209 00:10:11,850 --> 00:10:16,220 had a 50% chance, and if I have gazillions of them, half 210 00:10:16,220 --> 00:10:18,530 of them will have turned into nitrogen. 211 00:10:18,530 --> 00:10:20,520 I don't know which half, but half of them 212 00:10:20,520 --> 00:10:21,890 will turn into it. 213 00:10:21,890 --> 00:10:25,770 So you might get a question like, I start with, oh I don't 214 00:10:25,770 --> 00:10:32,860 know, let's say I start with 80 grams of something with, 215 00:10:32,860 --> 00:10:36,580 let's just call it x, and it has a half-life of two years. 216 00:10:36,580 --> 00:10:38,020 I'm just making up this compound. 217 00:10:38,020 --> 00:10:39,720 A two-year half-life. 218 00:10:39,720 --> 00:10:43,740 219 00:10:43,740 --> 00:10:46,200 And then let's say we go into a time machine and we look 220 00:10:46,200 --> 00:10:50,670 back at our sample, and let's say we only have 10 grams of 221 00:10:50,670 --> 00:10:51,760 our sample left. 222 00:10:51,760 --> 00:10:55,000 And we want to know how much time has passed by. 223 00:10:55,000 --> 00:10:58,360 So 10 grams left of x. 224 00:10:58,360 --> 00:11:00,710 How much time, you know, x is decaying the whole time, how 225 00:11:00,710 --> 00:11:02,540 much time has passed? 226 00:11:02,540 --> 00:11:04,380 Well let's think about it. 227 00:11:04,380 --> 00:11:12,300 We're starting at time, 0 with 80 grams. After two years, how 228 00:11:12,300 --> 00:11:13,400 much are we going to have left? 229 00:11:13,400 --> 00:11:16,980 We're going to have 40 grams. So t equals 2. 230 00:11:16,980 --> 00:11:19,160 But after two more years, how many are we going to have? 231 00:11:19,160 --> 00:11:22,540 We're going to have 20 grams. So this is t equals 3 I'm 232 00:11:22,540 --> 00:11:24,650 sorry, this is t equals 4 years. 233 00:11:24,650 --> 00:11:31,400 And then after two more years, I'll only have half of that 234 00:11:31,400 --> 00:11:31,940 left again. 235 00:11:31,940 --> 00:11:34,620 So now I'm only going to have 10 grams left. 236 00:11:34,620 --> 00:11:35,590 And that's where I am. 237 00:11:35,590 --> 00:11:37,390 And this is t equals 6. 238 00:11:37,390 --> 00:11:39,630 So if you know you have some compound. 239 00:11:39,630 --> 00:11:42,210 You're starting off with 80 grams. You know it has a 240 00:11:42,210 --> 00:11:43,030 two-year half-life. 241 00:11:43,030 --> 00:11:44,340 You get in a time machine. 242 00:11:44,340 --> 00:11:47,130 And then you didn't build your time machine well. 243 00:11:47,130 --> 00:11:49,080 You don't know how well it calibrates against time. 244 00:11:49,080 --> 00:11:50,900 You just look at your sample. 245 00:11:50,900 --> 00:11:52,470 You say, oh, I only have 10 grams left. 246 00:11:52,470 --> 00:11:59,470 You know that 1, 2, 3 half-lives have gone by. 247 00:11:59,470 --> 00:12:01,000 And you could also think about it this way. 248 00:12:01,000 --> 00:12:04,760 1/2 to the 3rd power, because every time you have 1/2 of the 249 00:12:04,760 --> 00:12:08,100 original sample-- that's the number of half-lives-- after 250 00:12:08,100 --> 00:12:11,340 three half-lives you'll have 1/8 of your original sample. 251 00:12:11,340 --> 00:12:12,450 And that's what we have here. 252 00:12:12,450 --> 00:12:16,230 We have 1/8 of 80 grams. And this is just when you're doing 253 00:12:16,230 --> 00:12:18,140 it with a discreet you know, when you're right at the 254 00:12:18,140 --> 00:12:19,270 half-life point. 255 00:12:19,270 --> 00:12:21,200 In the next video we're going to explore what if I asked you 256 00:12:21,200 --> 00:12:24,000 a question, how many of the particles, or how many grams 257 00:12:24,000 --> 00:12:26,300 will you have in exactly 10 days? 258 00:12:26,300 --> 00:12:28,420 Or at two and a half years? 259 00:12:28,420 --> 00:00:00,000 And we'll do that in the next video.