1 00:00:00,000 --> 00:00:05,111 So we've had our a discussion of what happens to the sun in the future and that 2 00:00:05,111 --> 00:00:10,031 was pretty interesting and we talked about all kinds of options about a what 3 00:00:10,031 --> 00:00:14,979 can happen to the reminisce. I said that I would come back and say 4 00:00:14,979 --> 00:00:19,558 what happens with more massive stars and the time to do that is now. 5 00:00:19,558 --> 00:00:24,542 So we start with a star who's mass is bigger than eight solar masses, that 6 00:00:24,542 --> 00:00:29,727 turns out to be a good place to make the cutoff, between solar mass and eight 7 00:00:29,727 --> 00:00:34,711 solar masses there are some changes but these two extremes will give us a 8 00:00:34,711 --> 00:00:37,540 representation of what happens, start with. 9 00:00:37,540 --> 00:00:42,996 Massive star can finish its main sequence life in as little as ten million years. 10 00:00:42,996 --> 00:00:47,914 So these stars are ephemeral compared to the sun; a thousand times faster. 11 00:00:47,914 --> 00:00:52,697 And, as usual, main sequence was when it was fusing hydrogen in the core. 12 00:00:52,697 --> 00:00:58,020 When the core runs out of hydrogen the core contracts, the envelope expands and 13 00:00:58,020 --> 00:01:03,207 pools and you get a red giant except because it started out as a big star we 14 00:01:03,207 --> 00:01:06,980 might get something you would call a red super giant so. 15 00:01:06,980 --> 00:01:11,338 This happens within a million years of the core collapse. 16 00:01:11,338 --> 00:01:14,534 It's finished its red giant expansion stage. 17 00:01:14,534 --> 00:01:19,837 Its size can be five astronomical units. We have a hydrogen burning shell 18 00:01:19,837 --> 00:01:23,470 surrounding an inert helium core and a huge. 19 00:01:23,470 --> 00:01:27,934 extended envelope. There will be mass loss in this period. 20 00:01:27,934 --> 00:01:32,845 The only difference is that here the inert helium core is too big. 21 00:01:32,845 --> 00:01:37,532 It never actually becomes inert. It's a smaller fraction of the actual 22 00:01:37,532 --> 00:01:41,863 mass of the whole star. So it does not collapse because of 23 00:01:41,863 --> 00:01:48,074 degeneracy but the core becomes massive. Eventually, it's not its own gravity but 24 00:01:48,074 --> 00:01:53,603 it is compressed by the external layers the internal temperatures were already 25 00:01:53,603 --> 00:01:57,828 high enough and so this is the red supergiant phase. 26 00:01:57,828 --> 00:02:02,015 Notice that there's not a huge increase in luminosity. 27 00:02:02,015 --> 00:02:07,830 At this point the star is, the, outer layers are cooling rapidly as the star 28 00:02:07,830 --> 00:02:12,715 expands so that luminosity rises somewhat but not very much. 29 00:02:12,715 --> 00:02:17,212 this was already 100,000 solar luminosity object. 30 00:02:17,212 --> 00:02:22,640 It doesn't get that much more luminous as a red giant and as usual 31 00:02:22,640 --> 00:02:25,344 helium core ignites. It's not as flashy. 32 00:02:25,344 --> 00:02:29,367 But since we don't see the flash, that makes no difference. 33 00:02:29,367 --> 00:02:34,777 we now have the structure or we have helium fusion in the core, hydrogen 34 00:02:34,777 --> 00:02:39,701 fusion in a shell, the envelope, the the hydrogen fusing shell having 35 00:02:39,701 --> 00:02:43,793 expanded, reduces its rate. The envelope contracts and heats. 36 00:02:43,793 --> 00:02:49,129 We have the horizontal branch for this giant star it makes a blue super 37 00:02:49,129 --> 00:02:55,138 giant its moving over to the left of the diagram is becoming blue. 38 00:02:55,138 --> 00:02:58,045 It's lives on the horizontal branch. 39 00:02:58,045 --> 00:03:03,619 Number not 700,000,000 years but only 1,000,000 years and again the helium 40 00:03:03,619 --> 00:03:09,193 fusion in the core is rapidly depositing a carbon oxygen core surrounded by a 41 00:03:09,193 --> 00:03:15,268 shell of inert helia fusing helium surrounded by inert helium, surrounded by 42 00:03:15,268 --> 00:03:20,342 hydrogen that is fusing surrounded by the inert hydrogen atmosphere. 43 00:03:20,342 --> 00:03:23,487 And here is where things become interesting. 44 00:03:23,487 --> 00:03:26,560 When the carbon oxygen core collapses here. 45 00:03:26,560 --> 00:03:33,916 It does reach a temperature, 600 million K, at which carbon nuclei can fuse and 46 00:03:33,916 --> 00:03:41,438 the carbon fusion process produces things like manganese and neon, magnesium and 47 00:03:41,438 --> 00:03:48,929 neon and oxygen and so we now have a collection of an inert a oxygen neon core 48 00:03:48,929 --> 00:03:53,281 surrounded by a carbon burning shell, surrounded by inert carbon. 49 00:03:53,281 --> 00:03:57,632 Surrounded by a helium burning shell, surrounded by inert helium. 50 00:03:57,632 --> 00:04:03,071 Surrounded by a hydrogen burning shell, surrounded by a red super giant envelope 51 00:04:03,071 --> 00:04:07,695 that is even bigger than before. And the carbon fusion phase is very 52 00:04:07,695 --> 00:04:11,978 inefficient energetically. Much of the energy is carried off by 53 00:04:11,978 --> 00:04:15,446 neutrinos. We have huge mass loss and stellar super 54 00:04:15,446 --> 00:04:21,060 winds and the whole core is. The converted from carbon to oxygen neon 55 00:04:21,060 --> 00:04:25,076 within 1,000 years. And then well, if the star is 56 00:04:25,076 --> 00:04:29,431 sufficiently massive, then we get neon, or oxygen fusing. 57 00:04:29,431 --> 00:04:34,420 And the process continues. We get neon fusion at one and a half 58 00:04:34,420 --> 00:04:39,961 billion degrees kelvin, one and a half. If the star is massive enough, the 59 00:04:39,961 --> 00:04:43,982 process continues. At 1.5 billion Kelvin, neon fuses to 60 00:04:43,982 --> 00:04:49,492 produce oxygen and magnesium. here the neutrino flux, remember the 61 00:04:49,492 --> 00:04:55,002 neutrinos just penetrate the star and leave, are carrying off a full solar 62 00:04:55,002 --> 00:05:00,139 luminocity just in neutrini. you get rid of the neon in just a few 63 00:05:00,139 --> 00:05:03,457 years. that slightly higher temperature, about 64 00:05:03,457 --> 00:05:08,482 two billion kelvin, oxygen fusion ignites, producing silicon and sulfur and 65 00:05:08,482 --> 00:05:12,080 phosphorus. Here neutrinos are carrying off a 100,000 66 00:05:12,080 --> 00:05:15,951 solar luminosities. You get through with oxygen in a year. 67 00:05:15,951 --> 00:05:20,975 The next state is silicon fusion at 3.5 billion kelvin and silicon fusion 68 00:05:20,975 --> 00:05:25,524 produces nickel which decays to iron, and that's an important point. 69 00:05:25,524 --> 00:05:29,734 And here neutrinos are carrying off amazing amounts of energy. 70 00:05:29,734 --> 00:05:33,740 And the silicon fusions process is complete in about a day. 71 00:05:33,740 --> 00:05:40,063 The result of all of this story is that you have been building up an inert core 72 00:05:40,063 --> 00:05:43,240 of iron. The changes are going on very, very 73 00:05:43,240 --> 00:05:44,790 rapidly. The exterior 74 00:05:44,790 --> 00:05:50,406 atmosphere has far to much inertia to really respond to all these rapid changes 75 00:05:50,406 --> 00:05:55,820 and in the process the neutron capture slow nucleosynthesis process is producing 76 00:05:55,820 --> 00:06:01,301 nucleotides heavier than iron so this is where mut a lot of heavier elements get 77 00:06:01,301 --> 00:06:06,105 synthesized and at the end of the silicone day the day it took to fuse 78 00:06:06,105 --> 00:06:10,414 silicon you have a core. Radius of about the Earth maybe a mass of 79 00:06:10,414 --> 00:06:15,272 a few solar masses which contains the following onion structure, it's got an 80 00:06:15,272 --> 00:06:20,386 inert nickel iron core surrounded by a silicon fusing shell surrounded by inert 81 00:06:20,386 --> 00:06:24,988 silicon surrounded by an oxygen fusing shell surrounded by inert oxygen 82 00:06:24,988 --> 00:06:30,038 surrounded by a neon and you so on you get the idea and all of this surrounded 83 00:06:30,038 --> 00:06:33,950 by a five AU or larger hydrogen helium envelope. 84 00:06:33,950 --> 00:06:38,446 the temperatures are now. On the order of three, 5 billion K 85 00:06:38,446 --> 00:06:42,500 densities in the center are as high as ten to the eleven. 86 00:06:42,500 --> 00:06:46,848 Kilos per meter cubed. At these high temperatures the photons 87 00:06:46,848 --> 00:06:51,809 that are being emitted are gamma rays and they cause photodisintegration. 88 00:06:51,809 --> 00:06:56,362 So, in fact at this last stage, the star starts very rapidly undoing. 89 00:06:56,362 --> 00:06:59,420 Whereas it's been doing all these millennium. 90 00:06:59,420 --> 00:07:03,021 working to construct heavier and heavier elements. 91 00:07:03,021 --> 00:07:08,458 All these nuclei are broken apart. iron breaks down under bombardment to a 92 00:07:08,458 --> 00:07:11,380 collection of alpha particles and, and junk. 93 00:07:11,380 --> 00:07:16,420 And so on and even alpha particles decompose back into protons. 94 00:07:16,420 --> 00:07:21,749 And now, what happens when the combined mass of the star collapses this iron 95 00:07:21,749 --> 00:07:24,414 core? Well, you can't ignite new fusion. 96 00:07:24,414 --> 00:07:30,094 I mean, you might get iron nuclei to fuse if you try hard enough, but that doesn't 97 00:07:30,094 --> 00:07:33,531 produce energy that won't stabilize the collapse. 98 00:07:33,531 --> 00:07:39,421 Once this iron core decides to collapse, it's not really obvious what is going to 99 00:07:39,421 --> 00:07:42,858 stop it. we'll see what it is that stops it, in 100 00:07:42,858 --> 00:07:43,840 the next clip.