1 00:00:16,466 --> 00:00:17,634 Now okay. 2 00:00:17,634 --> 00:00:22,906 So now I'm going to get to the why this matters. 3 00:00:22,906 --> 00:00:26,810 So there's two different sources, two different targets. 4 00:00:26,810 --> 00:00:29,846 Remember, we can call them sources or targets. 5 00:00:29,846 --> 00:00:36,820 And notice they both have this continuous radiation. 6 00:00:36,820 --> 00:00:38,054 And I will talk about that. 7 00:00:38,054 --> 00:00:40,357 The [INAUDIBLE] will end with a discussion 8 00:00:40,357 --> 00:00:43,259 a little bit on what you can do with that. 9 00:00:43,259 --> 00:00:46,329 But for now, let's keep focused on these lines, 10 00:00:46,329 --> 00:00:48,031 these discrete characteristic lines. 11 00:00:48,031 --> 00:00:49,632 So there's the k alpha from molybdenum. 12 00:00:49,632 --> 00:00:51,501 There's the k alpha for copper. 13 00:00:51,501 --> 00:01:00,477 OK, now Moseley, Henry Moseley, was a brilliant scientist. 14 00:01:00,477 --> 00:01:04,781 And he was working with Rutherford and others. 15 00:01:04,781 --> 00:01:10,520 And he was really interested in looking at the trends. 16 00:01:10,520 --> 00:01:12,655 So he took all of these elements. 17 00:01:12,655 --> 00:01:15,358 So from calcium all the way to zinc. 18 00:01:15,358 --> 00:01:16,826 20 to 30. 19 00:01:16,826 --> 00:01:18,862 And he said I want to look at the k 20 00:01:18,862 --> 00:01:21,464 alpha lines of all of these. 21 00:01:21,464 --> 00:01:24,134 I want to look at the K alpha lines of all of these. 22 00:01:24,134 --> 00:01:28,271 And what he found was extraordinary. 23 00:01:28,271 --> 00:01:29,305 He did more. 24 00:01:29,305 --> 00:01:30,640 38 in total. 25 00:01:30,640 --> 00:01:33,410 But I'm just going to show you his data for these. 26 00:01:33,410 --> 00:01:34,144 OK? 27 00:01:34,144 --> 00:01:39,416 And what he did was absolutely profound because what 28 00:01:39,416 --> 00:01:40,350 he noticed-- 29 00:01:40,350 --> 00:01:41,217 there are the lines. 30 00:01:41,217 --> 00:01:42,685 These are actually his measurements. 31 00:01:42,685 --> 00:01:43,186 OK? 32 00:01:43,186 --> 00:01:46,156 These are his k alpha lines. 33 00:01:46,156 --> 00:01:50,026 And what he noticed in going from calcium down to-- 34 00:01:50,026 --> 00:01:51,795 ohh-- brass? 35 00:01:51,795 --> 00:01:54,097 OK, we'll talk about that in a minute. 36 00:01:54,097 --> 00:01:56,032 It's supposed to be zinc, isn't it? 37 00:01:56,032 --> 00:01:57,100 Why is it zinc? 38 00:01:57,100 --> 00:01:58,201 Well, why is it not zinc? 39 00:01:58,201 --> 00:02:00,336 Let's think about that later. 40 00:02:00,336 --> 00:02:05,375 For now he noticed that this has a square root relationship 41 00:02:05,375 --> 00:02:06,609 to the energy. 42 00:02:06,609 --> 00:02:09,512 So Moseley came up with-- 43 00:02:09,512 --> 00:02:12,382 he was working on this in 1912. 44 00:02:12,382 --> 00:02:14,217 OK? 45 00:02:14,217 --> 00:02:17,887 You got to remember 1913. 46 00:02:17,887 --> 00:02:23,159 1912 was when Rutherford did the gold foil experiments. 47 00:02:23,159 --> 00:02:26,663 It had been 44 years since Mendeleev 48 00:02:26,663 --> 00:02:30,100 put his periodic table to paper and published that. 49 00:02:30,100 --> 00:02:33,670 So for 44 years, we had a periodic table. 50 00:02:33,670 --> 00:02:36,305 But see, the thing is, there was a huge problem 51 00:02:36,305 --> 00:02:41,911 with the periodic table because Mendeleev 52 00:02:41,911 --> 00:02:46,950 had this, sort of, brilliant realization that periodicity-- 53 00:02:46,950 --> 00:02:53,456 periodicity-- was related to, both, the atomic mass-- 54 00:02:53,456 --> 00:02:55,391 and remember, we talked about this-- 55 00:02:55,391 --> 00:02:59,629 and the properties, the chemical properties. 56 00:02:59,629 --> 00:03:02,699 That chemical properties. 57 00:03:05,201 --> 00:03:10,440 That allowed him to create in ordering of the elements. 58 00:03:10,440 --> 00:03:12,108 In ordering of the elements. 59 00:03:12,108 --> 00:03:13,943 That is still the ordering, essentially, 60 00:03:13,943 --> 00:03:16,646 that we have today. 61 00:03:16,646 --> 00:03:21,484 But the problem is why did they have that ordering? 62 00:03:21,484 --> 00:03:25,288 I didn't really tell you why, sometimes, he was like, well, 63 00:03:25,288 --> 00:03:27,257 the properties win. 64 00:03:27,257 --> 00:03:28,791 OK, maybe the mass-- no, no. 65 00:03:28,791 --> 00:03:29,526 Properties win. 66 00:03:29,526 --> 00:03:31,794 Properties need to be aligned in this column, 67 00:03:31,794 --> 00:03:33,296 so I'm I'm going to move those over. 68 00:03:33,296 --> 00:03:35,865 Like, that's what he did. 69 00:03:35,865 --> 00:03:39,802 But he didn't know why, except that it made sense to him. 70 00:03:39,802 --> 00:03:42,238 Moseley's experiments told us. 71 00:03:42,238 --> 00:03:43,473 They gave us the why. 72 00:03:43,473 --> 00:03:45,508 Aw, it was so important. 73 00:03:45,508 --> 00:03:48,144 And Moseley's law-- 74 00:03:48,144 --> 00:03:52,281 Moseley's law-- was, essentially, 75 00:03:52,281 --> 00:03:54,784 him thinking about the Bohr model 76 00:03:54,784 --> 00:03:57,120 for these characteristic x-rays. 77 00:03:57,120 --> 00:04:01,024 So he said that h nu-- 78 00:04:01,024 --> 00:04:05,094 so that's the frequency for some k alpha line-- 79 00:04:05,094 --> 00:04:08,164 is equal to 13.6 ev. 80 00:04:08,164 --> 00:04:09,599 All that looks familiar. 81 00:04:09,599 --> 00:04:13,203 Times z minus 1 squared. 82 00:04:13,203 --> 00:04:16,873 And then, he did the difference in energy, 83 00:04:16,873 --> 00:04:21,010 just like we've done now a number of times in this class. 84 00:04:21,010 --> 00:04:22,278 That's what he did. 85 00:04:22,278 --> 00:04:24,781 And this is 3/4. 86 00:04:24,781 --> 00:04:25,548 Why this? 87 00:04:25,548 --> 00:04:27,417 Well, let's talk about that in a second. 88 00:04:27,417 --> 00:04:39,862 So 13.6 ev times 3/4 times z minus 1 squared. 89 00:04:39,862 --> 00:04:41,464 Two things about this, right? 90 00:04:41,464 --> 00:04:48,104 One is why is it 1 over 1 squared minus 1 over 2 squared? 91 00:04:48,104 --> 00:04:51,741 Well that's because they knew, or at least they 92 00:04:51,741 --> 00:04:54,978 were pretty confident, that you had this positive charge 93 00:04:54,978 --> 00:04:56,145 in the middle here. 94 00:04:56,145 --> 00:04:58,548 That's the protons and the nucleus. 95 00:04:58,548 --> 00:04:59,949 And then, you had these electrons. 96 00:04:59,949 --> 00:05:00,450 Right? 97 00:05:00,450 --> 00:05:03,286 So you had, like, the 1s electrons. 98 00:05:03,286 --> 00:05:06,422 And then, you had another shell out here. 99 00:05:06,422 --> 00:05:08,725 And so they knew, OK, 2s. 100 00:05:08,725 --> 00:05:13,196 Maybe that's combined with 2p, so it goes on. 101 00:05:13,196 --> 00:05:16,332 So what happens in the x-ray experiment? 102 00:05:16,332 --> 00:05:18,901 Well what happens is you shoot an electron in. 103 00:05:18,901 --> 00:05:21,871 Rank and just crank the voltage up 104 00:05:21,871 --> 00:05:25,775 so high that an electron could come and knock that out. 105 00:05:25,775 --> 00:05:26,276 Right? 106 00:05:26,276 --> 00:05:28,978 And so that's what did it. 107 00:05:28,978 --> 00:05:32,982 And so now one of these can cascade down there 108 00:05:32,982 --> 00:05:38,021 and give off a k alpha photon. 109 00:05:38,021 --> 00:05:38,554 Right? 110 00:05:38,554 --> 00:05:40,123 This is nothing new. 111 00:05:40,123 --> 00:05:41,858 We've talked about this. 112 00:05:41,858 --> 00:05:44,694 But you see it here in the equation. 113 00:05:44,694 --> 00:05:46,095 You see it in two ways. 114 00:05:46,095 --> 00:05:50,066 First, we're going from 2 to 1. 115 00:05:50,066 --> 00:05:52,034 1 squared minus 1/2 squared. 116 00:05:52,034 --> 00:05:53,469 3/4. 117 00:05:53,469 --> 00:05:54,237 Right? 118 00:05:54,237 --> 00:05:57,774 But second-- and this was critical-- 119 00:05:57,774 --> 00:05:59,142 the z minus. 120 00:05:59,142 --> 00:06:06,683 The z minus told us that all these positive charges 121 00:06:06,683 --> 00:06:09,085 in here, all these positive charges, 122 00:06:09,085 --> 00:06:12,388 are screened perfectly by one electron, this one that 123 00:06:12,388 --> 00:06:13,856 was left. 124 00:06:13,856 --> 00:06:15,692 And it works. 125 00:06:15,692 --> 00:06:18,394 He assumed perfect [INAUDIBLE]. 126 00:06:18,394 --> 00:06:20,296 So what do all these see? 127 00:06:20,296 --> 00:06:22,231 They see z minus 1. 128 00:06:22,231 --> 00:06:28,204 They see z minus 1 if z is related to the atomic number. 129 00:06:28,204 --> 00:06:31,174 Now here's where this was so powerful 130 00:06:31,174 --> 00:06:33,443 because when you-- and if you can't read this, 131 00:06:33,443 --> 00:06:34,409 don't worry about that. 132 00:06:34,409 --> 00:06:37,947 I just want to show you that it is a perfectly straight line. 133 00:06:37,947 --> 00:06:41,150 When you plot the K alpha transitions, 134 00:06:41,150 --> 00:06:43,386 these are different elements. 135 00:06:43,386 --> 00:06:45,588 These are his different elements. 136 00:06:45,588 --> 00:06:51,159 And if you plot the square root of the frequency 137 00:06:51,159 --> 00:06:56,999 versus element, it is a perfect line that holds. 138 00:06:56,999 --> 00:06:58,901 And so what Moseley wrote in the paper 139 00:06:58,901 --> 00:07:03,005 is we have your proof in 1930 that there is, in the atom, 140 00:07:03,005 --> 00:07:04,307 a fundamental quantity. 141 00:07:04,307 --> 00:07:07,977 A fundamental quantity, which increases by regular steps 142 00:07:07,977 --> 00:07:10,480 as one passes from one element to the next. 143 00:07:10,480 --> 00:07:12,915 This quantity can only be-- only be-- 144 00:07:12,915 --> 00:07:15,752 the charge on the central positive nucleus, 145 00:07:15,752 --> 00:07:18,121 of the existence of which we already have definite proof. 146 00:07:18,121 --> 00:07:19,155 Now we know about that. 147 00:07:19,155 --> 00:07:22,792 We know from experiments that Rutherford 148 00:07:22,792 --> 00:07:25,895 did that that nucleus had the positive charge. 149 00:07:25,895 --> 00:07:28,431 But they didn't know that it was connected 150 00:07:28,431 --> 00:07:30,400 to the position in the periodic table. 151 00:07:33,169 --> 00:07:37,573 In fact, years later, people talking about those 152 00:07:37,573 --> 00:07:38,107 experiences-- 153 00:07:38,107 --> 00:07:41,344 I mean, people didn't even take Rutherford's experiments 154 00:07:41,344 --> 00:07:46,682 as seriously until Moseley's work came along. 155 00:07:46,682 --> 00:07:51,220 44 years had come since Mendeleev. 156 00:07:51,220 --> 00:07:55,091 But Moseley gave it the foundation that it needed. 157 00:07:55,091 --> 00:08:00,196 Periodicity is because of atomic number. 158 00:08:00,196 --> 00:08:02,698 Periodicity is atomic number. 159 00:08:02,698 --> 00:08:05,802 That was not known. 160 00:08:05,802 --> 00:08:08,771 That z gives you the periodicity. 161 00:08:08,771 --> 00:08:09,272 Right? 162 00:08:09,272 --> 00:08:11,974 And that gives you, also, the number of protons. 163 00:08:14,177 --> 00:08:16,512 This was a time when they didn't know what was going on. 164 00:08:16,512 --> 00:08:20,049 Why did the mass change so much the neutron wasn't discovered 165 00:08:20,049 --> 00:08:23,753 till 1932, 20 years later? 166 00:08:23,753 --> 00:08:25,822 But this gave the grounding that was 167 00:08:25,822 --> 00:08:28,357 needed to the chemistry of the periodic table. 168 00:08:28,357 --> 00:08:30,660 It was a very important discovery. 169 00:08:30,660 --> 00:08:31,994 Very, very important discovery. 170 00:08:31,994 --> 00:08:33,462 So that's my why this matters. 171 00:08:33,462 --> 00:08:40,970 And it's really tragic because he died, tragically, 172 00:08:40,970 --> 00:08:43,806 in World War I at age 27. 173 00:08:43,806 --> 00:08:47,910 And the Nobel Prize was not given in 1916 174 00:08:47,910 --> 00:08:49,312 for either physics or chemistry. 175 00:08:49,312 --> 00:08:50,780 He died in 1915. 176 00:08:50,780 --> 00:08:52,949 And most people, at the time, believe that he 177 00:08:52,949 --> 00:08:55,585 would have won it at age 28. 178 00:08:55,585 --> 00:08:58,855 That's how important that discovery was.