WEBVTT 00:00:00.650 --> 00:00:03.140 We've already talked about the life cycle of stars 00:00:03.140 --> 00:00:06.070 roughly the same mass as our sun, give or take a little bit. 00:00:06.070 --> 00:00:07.710 What I want to do in this video is 00:00:07.710 --> 00:00:09.260 talk about more massive stars. 00:00:12.372 --> 00:00:14.080 And when I'm talking about massive stars, 00:00:14.080 --> 00:00:17.180 I'm talking about stars that have masses greater than 9 00:00:17.180 --> 00:00:20.960 times the sun. 00:00:20.960 --> 00:00:23.330 So the general idea is exactly the same. 00:00:23.330 --> 00:00:27.170 You're going to start off with this huge cloud of mainly 00:00:27.170 --> 00:00:27.910 hydrogen. 00:00:27.910 --> 00:00:29.410 And now, this cloud is going to have 00:00:29.410 --> 00:00:34.070 to be bigger than the clouds that condensed to form stars 00:00:34.070 --> 00:00:34.741 like our sun. 00:00:34.741 --> 00:00:36.240 But you're going to start with that, 00:00:36.240 --> 00:00:40.440 and eventually gravity's going to pull it together. 00:00:40.440 --> 00:00:43.330 And the core of it is going to get hot and dense enough 00:00:43.330 --> 00:00:47.090 for hydrogen to ignite, for hydrogen to start fusing. 00:00:47.090 --> 00:00:49.534 So this is hydrogen, and it is now fusing. 00:00:49.534 --> 00:00:50.200 Let me write it. 00:00:50.200 --> 00:00:51.630 It is now fusing. 00:00:51.630 --> 00:00:53.550 Hydrogen fusion. 00:00:53.550 --> 00:00:55.360 Let me write it like this. 00:00:55.360 --> 00:01:01.000 You now have hydrogen fusion in the middle. 00:01:01.000 --> 00:01:03.280 So it's ignited, and around it, you 00:01:03.280 --> 00:01:05.820 have just the other material of the cloud. 00:01:05.820 --> 00:01:06.990 So the rest of the hydrogen. 00:01:06.990 --> 00:01:09.640 And now, since it's so heated, it's really a plasma. 00:01:09.640 --> 00:01:12.280 It's really kind of a soup of electrons and nucleuses 00:01:12.280 --> 00:01:15.957 as opposed to well-formed atoms, especially close to the core. 00:01:15.957 --> 00:01:17.290 So now you have hydrogen fusion. 00:01:17.290 --> 00:01:19.820 We saw this happens at around 10 million Kelvin. 00:01:19.820 --> 00:01:21.276 And I want to make it very clear. 00:01:21.276 --> 00:01:23.150 Since we're talking about more massive stars, 00:01:23.150 --> 00:01:25.650 even at this stage, there's going 00:01:25.650 --> 00:01:31.710 to be more gravitational pressure, even at this stage, 00:01:31.710 --> 00:01:34.020 during the main sequence of the star, 00:01:34.020 --> 00:01:35.560 because it is more massive. 00:01:35.560 --> 00:01:38.460 And so this is going to burn faster and hotter. 00:01:38.460 --> 00:01:42.650 So this is going to be faster and hotter than something 00:01:42.650 --> 00:01:43.670 the mass of our sun. 00:01:46.350 --> 00:01:50.850 And so even this stage is going to happen over 00:01:50.850 --> 00:01:54.470 a much shorter period of time than for a star the mass 00:01:54.470 --> 00:01:55.100 of our sun. 00:01:55.100 --> 00:01:58.747 Our sun's life is going to be 10 or 11 billion total years. 00:01:58.747 --> 00:02:00.580 Here, we're going to be talking about things 00:02:00.580 --> 00:02:02.840 in maybe the tens of millions of years. 00:02:02.840 --> 00:02:05.579 So a factor of 1,000 shorter life span. 00:02:05.579 --> 00:02:07.370 But anyway, let's think about what happens. 00:02:07.370 --> 00:02:09.500 And so far, just the pattern of what happens, 00:02:09.500 --> 00:02:11.083 it's going to happen faster because we 00:02:11.083 --> 00:02:13.850 have more pressure, more gravity, more temperature. 00:02:13.850 --> 00:02:16.460 But it's going to happen in pretty much the same way 00:02:16.460 --> 00:02:20.000 as what we saw with a star the mass of the sun. 00:02:20.000 --> 00:02:23.060 Eventually that helium-- sorry, that hydrogen 00:02:23.060 --> 00:02:25.930 is going to fuse into a helium core that's 00:02:25.930 --> 00:02:28.164 going to have a hydrogen shell around it. 00:02:28.164 --> 00:02:30.080 It's going to have a hydrogen shell around it, 00:02:30.080 --> 00:02:31.520 hydrogen fusion shell around it. 00:02:31.520 --> 00:02:34.170 And then you have the rest of the star around that. 00:02:34.170 --> 00:02:35.870 So let me label it. 00:02:35.870 --> 00:02:41.740 This right here is our helium core. 00:02:41.740 --> 00:02:43.420 And more and more helium is going 00:02:43.420 --> 00:02:45.970 to be built up as this hydrogen in this shell fuses. 00:02:45.970 --> 00:02:49.930 And in a star the size of our sun or the mass of our sun, 00:02:49.930 --> 00:02:52.020 this is when it starts to become a red giant. 00:02:52.020 --> 00:02:56.020 Because this core is getting denser and denser and denser 00:02:56.020 --> 00:02:58.670 as more and more helium is produced. 00:02:58.670 --> 00:03:01.110 And as it gets denser and denser and denser, 00:03:01.110 --> 00:03:03.370 there's more and more gravitational pressure 00:03:03.370 --> 00:03:06.490 being put on the hydrogen, on this hydrogen shell 00:03:06.490 --> 00:03:09.600 out here, where we have fusion still happening. 00:03:09.600 --> 00:03:14.440 And so that's going to release more outward energy to push out 00:03:14.440 --> 00:03:17.836 the radius of the actual star. 00:03:17.836 --> 00:03:19.210 So the general process, and we're 00:03:19.210 --> 00:03:21.430 going to see this as the star gets more and more massive, 00:03:21.430 --> 00:03:23.888 is we're going to have heavier and heavier elements forming 00:03:23.888 --> 00:03:25.142 in the core. 00:03:25.142 --> 00:03:26.600 Those heavier and heavier elements, 00:03:26.600 --> 00:03:28.370 as the star gets denser and denser, 00:03:28.370 --> 00:03:31.170 will eventually ignite, kind of supporting the core. 00:03:31.170 --> 00:03:33.900 But because the core itself is getting denser and denser 00:03:33.900 --> 00:03:36.920 and denser, material is getting pushed further and further out 00:03:36.920 --> 00:03:38.010 with more and more energy. 00:03:38.010 --> 00:03:39.710 Although if the star is massive enough, 00:03:39.710 --> 00:03:41.460 it's not going to be able to be pushed out 00:03:41.460 --> 00:03:44.330 as far as you will have in kind of a red giant, 00:03:44.330 --> 00:03:45.824 with kind of a sun-like star. 00:03:45.824 --> 00:03:47.740 But let's just think about how this pattern is 00:03:47.740 --> 00:03:48.490 going to continue. 00:03:48.490 --> 00:03:52.280 So eventually, that helium, once it gets dense enough, 00:03:52.280 --> 00:03:55.340 it's going to ignite and it's going to fuse into carbon. 00:03:55.340 --> 00:03:57.760 And you're going to have a carbon core forming. 00:03:57.760 --> 00:03:59.350 So that is carbon core. 00:03:59.350 --> 00:04:00.840 That's a carbon core. 00:04:00.840 --> 00:04:02.810 Around that, you have a helium core. 00:04:05.650 --> 00:04:07.980 And near the center of the helium core, 00:04:07.980 --> 00:04:10.180 you have a shell of helium fusion-- 00:04:10.180 --> 00:04:13.150 that's helium, not hydrogen-- turning into carbon, making 00:04:13.150 --> 00:04:15.310 that carbon core denser and hotter. 00:04:15.310 --> 00:04:18.680 And then around that, you have hydrogen fusion. 00:04:18.680 --> 00:04:20.139 Have to be very careful. 00:04:20.139 --> 00:04:21.180 You have hydrogen fusion. 00:04:21.180 --> 00:04:23.925 And then around that, you have the rest of the star. 00:04:27.172 --> 00:04:29.380 And so this process is just going to keep continuing. 00:04:29.380 --> 00:04:31.700 Eventually that carbon is going to start fusing. 00:04:31.700 --> 00:04:33.090 And you're going to have heavier and heavier 00:04:33.090 --> 00:04:34.048 elements form the core. 00:04:34.048 --> 00:04:36.130 And so this is a depiction off of Wikipedia 00:04:36.130 --> 00:04:39.440 of a fairly mature massive star. 00:04:39.440 --> 00:04:41.760 And you keep forming these shells 00:04:41.760 --> 00:04:43.760 of heavier and heavier elements, and cores 00:04:43.760 --> 00:04:46.380 of heavier and heavier elements until eventually, you 00:04:46.380 --> 00:04:47.310 get to iron. 00:04:47.310 --> 00:04:52.650 And in particular, we're talking about iron 56. 00:04:52.650 --> 00:04:54.920 Iron with an atomic mass of 56. 00:04:54.920 --> 00:04:57.980 Here on this periodic table that 26 is its atomic number. 00:04:57.980 --> 00:04:59.680 It's how many protons it has. 00:04:59.680 --> 00:05:03.010 56, you kind of view it as a count of the protons 00:05:03.010 --> 00:05:05.940 and neutrons, although it's not exact. 00:05:05.940 --> 00:05:08.720 But at this point, the reason why you stop here is that you 00:05:08.720 --> 00:05:12.290 cannot get energy by fusing iron. 00:05:12.290 --> 00:05:15.210 Fusing iron into heavier elements beyond iron 00:05:15.210 --> 00:05:16.720 actually requires energy. 00:05:16.720 --> 00:05:19.070 So it would actually be an endothermic process. 00:05:19.070 --> 00:05:23.200 So to fuse iron actually won't help support the core. 00:05:23.200 --> 00:05:25.980 So what I want to do in this-- So just to be very clear, 00:05:25.980 --> 00:05:28.630 this is how the heavy elements actually formed. 00:05:28.630 --> 00:05:31.500 We started with hydrogen, hydrogen fusing 00:05:31.500 --> 00:05:34.090 into helium, helium fusing into carbon, 00:05:34.090 --> 00:05:36.979 and then all of these things in various combinations-- 00:05:36.979 --> 00:05:38.520 and I won't go into all the details-- 00:05:38.520 --> 00:05:40.380 are fusing heavier and heavier elements. 00:05:40.380 --> 00:05:42.650 Neon, oxygen, and you see it right over here. 00:05:42.650 --> 00:05:43.700 Silicon. 00:05:43.700 --> 00:05:45.300 And these aren't the only elements that are forming, 00:05:45.300 --> 00:05:47.820 but these are kind of the main core elements that are forming. 00:05:47.820 --> 00:05:50.236 But along the way, you have all this other stuff, lithium, 00:05:50.236 --> 00:05:51.070 beryllium, boron. 00:05:51.070 --> 00:05:53.520 All of this other stuff is also forming. 00:05:53.520 --> 00:05:57.330 So this is how you form elements up to iron 56. 00:05:57.330 --> 00:06:00.980 And also, this is actually how you can form up to nickel 56, 00:06:00.980 --> 00:06:03.600 just to be exact. 00:06:03.600 --> 00:06:05.470 There will also be some nickel 56, 00:06:05.470 --> 00:06:07.770 which has the same mass as iron 56, 00:06:07.770 --> 00:06:11.400 just has two fewer neutrons and two more protons. 00:06:11.400 --> 00:06:15.590 So nickel 56 will also form, can also 00:06:15.590 --> 00:06:17.420 be, it'll be like a nickel-iron core. 00:06:17.420 --> 00:06:19.250 But that's about how far a star can 00:06:19.250 --> 00:06:23.940 get, regardless of how massive it is, at least by going 00:06:23.940 --> 00:06:26.150 through traditional fusion, through 00:06:26.150 --> 00:06:28.280 the traditional ignition mechanism. 00:06:28.280 --> 00:06:30.310 What I want to do is leave you there 00:06:30.310 --> 00:06:33.180 just so you can think about what might happen next, 00:06:33.180 --> 00:06:36.400 now that we can't fuse this star anymore. 00:06:36.400 --> 00:06:39.890 And what we're actually going to see is that it will supernova.