StarTalk Radio - Cosmic Queries – Black Hole Paradox with Matt O’Dowd

Episode Date: June 13, 2023

Can we use gravitational lensing to view distant planets? Neil deGrasse Tyson and comedian Chuck Nice explore black holes, quasars, entropy, and more with astrophysicist and host of PBS Space Time, Ma...tt O’Dowd.NOTE: StarTalk+ Patrons can listen to this entire episode commercial-free.Thanks to our Patrons Kelly Madison, Shaun Moats, Vascked, Irene Campbell, Joseph Brown, and Guillermo Leal for supporting us this week.Photo Credit: NOIRLab/NSF/AURA/J. da Silva, CC BY 4.0, via Wikimedia Commons Subscribe to SiriusXM Podcasts+ on Apple Podcasts to listen to new episodes ad-free and a whole week early.

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Starting point is 00:00:00 On the next episode of StarTalk, it's a Cosmic Queries with my friend and colleague, Matt O'Dowd, who's an expert in weird and wacky stuff in the universe, including black holes, quasars, gravitational lenses, and the like. So what is at the threshold of a quasar? Could the Big Rip rip into black holes? Could the Big Rip rip into black holes? And more, coming up on StarTalk Cosmic Queries. Welcome to StarTalk. Your place in the universe where science and pop culture collide.
Starting point is 00:00:43 StarTalk begins right now. This is StarTalk. Neil deGrasse Tyson here, your personal astrophysicist. I got with me Chuck Nice. Chuck, baby. Hey, hey, hey, Neil. What's happening? All right. We're doing cosmic queries today. Yes. Yeah. And today, we've got a friend and colleague,
Starting point is 00:01:04 a friend of StarTalk and a friend of mine, Matt Dowd. Matt, welcome back to StarTalk. Great to be here again, Neil. How are you doing? And Matt, is that a fake Zoom background behind you? Or like, what is that? Well, if the simulation hypothesis is correct, then yes. But I think I'm actually outside.
Starting point is 00:01:21 I'm on my day. Very nice. No, I think we hear birds and things. That's very beautiful. Your expertise is black holes, quasars, gravitational lensing, really juicy, tasty, cosmic things, all of which will kill you if you come in the vicinity of them. Immediately. The most hostile part of the cosmos.
Starting point is 00:01:42 Exactly. This is why we love them. You teach at Lehman College of the City University of New York. You're also an associate here at the Department of Astrophysics at the American Museum of Natural History. And you're a host and writer for the YouTube channel for PBS Space Time, which has nearly 3 million subscribers. Dude, you're rocking it.
Starting point is 00:02:05 Okay. Killing it. Totally killing it. So, Matt, I see you're like into a film called Inventing Reality. What's going on there? Yeah, this is a film that we recently got crowdfunded and we're in the process of writing. Love that.
Starting point is 00:02:20 Love that. Okay. And what's it about? It is about our quest for the fundamental. It's about humanity's search for the underlying clockwork of nature, both from the point of view of physics, but also from the point of view of neuroscience, brain science. So it's connecting how our brains construct our models of the world
Starting point is 00:02:41 and how that fact is connected to how science at a societal level constructs its models of the world. And you have a collaborator? Who's your collaborator? So, working with my partner, Bahar Golipur, who's a neuroscientist, we're writing it together and it's being produced with and directed by Andrew Kornhaber who's part of the Space Time team. Okay.
Starting point is 00:03:09 Very nice. Very nice. So everyone should have like a neuroscientist at arm's reach. 100%. Without a doubt. I'm not alone. I'm not alone in that.
Starting point is 00:03:18 Except I have to pay mine by the 45 minutes. But I do have one at arm's reach. So Chuck, we've got questions. We do. We're solicited from our Patreon members. Correct. The threshold of access to this feature is $5 a month.
Starting point is 00:03:34 That's it. That's all it is. All right. So, Matt, are you ready for us? Let's do it. Let's do it. All right. By the way, Matt and I have overlapping expertise in the Venn diagram.
Starting point is 00:03:44 So, what will happen is whatever is right in his bailiwork, he'll take it. But if there's some spillage, I'll jump in too. You okay with that, Matt? Let's do it together. Okay. All right. There you go. And if there's spillage from that, then Chuck can pick up the slack.
Starting point is 00:04:00 Right. At that point, we're not looking at spillage. We're looking more like at an environmental disaster okay you know i mean that's kind of ex-avon valdez territory if it's like and chuck what do you think about black holes we have reached a new low okay here we go uh this is bsm 1989, says, greetings, Dr. Tyson, Chuck, and Dr. Matt. My name is Blake, and I'm from Mobile, Alabama. Can you elaborate on energy density surrounding a black hole and how Hawking radiation might work? Is the material that falls into a black hole lost forever? And does it eventually somehow get out? Love it. That's all you, Matt.
Starting point is 00:04:51 Take it. Wow. All right. So this is, to answer this question, I need to summarize a large fraction of 20th century physics in a minute. Wait, wait, but we only have- I know. I'm going to try.
Starting point is 00:05:06 You're going to start your answer by saying, first let me summarize 20th century physics. No, I'm serious. So here we go, guys. The answer to your question is, I was born the son of a poor sharecropper. I mean, so much of the story of the development of 20th century physics is
Starting point is 00:05:23 around black holes, and this exact weird thing about black holes, that what goes in seems to not come out. And this is a paradox. Okay, so, all right. I mean, let me get these questions one piece at a time. So, the energy density around the black hole. I mean, so first of all, let's talk about a black hole. city around the black hole. I mean, so first of all, let's talk about a black hole. It is a place where gravity has had its ultimate victory. So it's usually the collapsed core of a star. So you have this hyper-dense region where it is, the gravity is so strong that light can't escape.
Starting point is 00:05:58 Okay. We don't know what's really inside a black hole, but there's this region around, you know, really inside a black hole, but there's this region around, you know, whatever that collapsed object is where you have what we call the event horizon, and that's the distance from which light can't escape, and it's black, okay? And so these things are invisible, you know, unless they're eating a star or a galaxy or something, and then we see the mess they make. But back in the 1960s, Stephen Hawking realized that black holes shouldn't actually be completely black, they should radiate. And this was Hawking's most famous discovery, called Hawking radiation. And it's described in a couple of different ways. One way is that you have matter and antimatter particles spontaneously appearing near the event horizon.
Starting point is 00:06:47 Normally, they would vanish again, destroying each other. But if one gets sucked into the event horizon, the other can escape. That's sort of the POPs I level. Hawking's own description of it was talking about the positive and negative frequency modes of the quantum vacuum and how they get perturbed by the black hole, leaving the vacuum itself generates particles, which you see. Okay, so Hawking radiation causes black holes to leak away their mass. So there's the answer to the other part of the question. When something falls into a black hole, we think now, so originally we thought that nothing could escape a black hole because nothing can travel faster than light, right? But now, I think most
Starting point is 00:07:32 physicists believe that because you have this Hawking radiation, at least the energy that falls into a black hole can eventually leak away as that radiation. And the really important thing about that is that not only can the energy get out, but the information can get out. And this was the other perplexing thing about black holes. It shouldn't be possible to destroy what we call quantum information. But via Hawking radiation, many physicists now think that the details of what you threw into the black hole somehow get out by this Hawking radiation also. So they get remembered. They get remembered.
Starting point is 00:08:12 Exactly. So it's almost like whatever it is, although it's not a chair that went in, all of the things, the blueprint information on that tiny, tiny level, when it comes out, that is still available. Yeah. If you could go to the, you know, if you could collect all the Hawking radiation that evaporated out of a black hole over trillions of years, every little bit, and somehow piece it together, the worst jigsaw puzzle in the universe, you should be able to reconstruct the chair. And that's what you guys mean when you say information. You're talking about all the stuff that we actually are on that. The inventory, the particle inventory.
Starting point is 00:08:57 The inventory on the quantum, all the way down to the particles. Yeah, the information that you would need if you wanted to rewind the universe and find out what happened previously, if you had all the information, then in principle, you could run the clock backwards and figure out what fell into the black hole in the first place. And just to clarify a point you're making, you're saying it came out of the black hole, but in fact, it came out of the energy field in the vicinity of the black hole, which counts as coming out of the black hole. Is that right? So this is, thank you for getting to the biggest hole in my argument here. Hawking's arguments were based on sort of internal consistency arguments in that it had to exist for the universe to make sense,
Starting point is 00:09:42 but the actual mechanism of its creation isn't clear. We just know it has to sort of emerge from the vicinity of the black hole somehow. But that counts for having come out of the black hole because it's using the gravitational energy density created by the black hole, and it just happens to be outside of the event horizon. Yeah, so one description of how this happens
Starting point is 00:10:03 is that the thing that falls into the black hole, which is your antiparticle or your negative frequency mode or whatever, somehow gains negative mass or negative energy inside the black hole. Because the dimensions inside the black hole get all twisted around, and so it's possible to have this relative negative mass go inside, which causes the positive mass of the black hole to shrink a little bit. Wow. Okay. Now, Chuck, isn't that obvious? That's completely obvious. My God. That is insane.
Starting point is 00:10:37 I love it. Wow. All right. All right. Keep going. Here we go. Hello, Dr. Tyson, Dr. O'Dell. How do we know black holes follow the second law of thermodynamics? Can black holes, that's an observed phenomenon, right? There's no deep principle deeper than it. We just say, oh, looks like entropy increases everywhere. So let's make it a law.
Starting point is 00:11:13 And maybe the black hole violates this. This is such a good follow-on question. So the crazy thing about entropy is that it feels like it's something that just, you know, emerges from the way particles interact with each other, etc. But it also seems like one of the most fundamental things in physics because no matter where you look, entropy seems to increase. With a black hole, there is a way to think about its entropy. So we think of entropy as a measurement of the amount of disorder in a system, okay? So a system will always move towards states of more disorder,
Starting point is 00:11:54 okay? Think about, for example, the air in the room. If you took all of the air and compacted it down into, you know, a ball this size, it would, well, first of all, you'd die of asphyxiation immediately, but the air would immediately burst out to fill the room. Okay, this configuration where all the air particles are in this one spot, it would be considered a very special or very ordered configuration, and so it would be considered low entropy.
Starting point is 00:12:20 So the only thing it can do from there is expand into a more disordered arrangement. Fill the room, there will be high entropy. In the case of a black hole, we know a lot less about the location of the particles of the air molecules, okay. So we have very little information, there's a lot more hidden information in the air in the room when it's filling the whole
Starting point is 00:12:56 room, compared to if we have this ball of air in our hands, then we have a much better idea of at least the location of all of the particles, They're all in this ball of air, okay? So entropy can be considered as a measurement of the amount of hidden information in a system. And over time, we tend to lose more and
Starting point is 00:13:17 more of the information of a system. So for a black hole, as a black hole grows, it's swallowing things from the external universe. And because we can't get information about what fell into a black hole out very easily, as a black hole grows, its entropy increases. Okay, so the amount of hidden information increases. And so there's this very tight relationship between actually the surface area of a black hole
Starting point is 00:13:49 and the amount of stuff that it's eaten, which corresponds to the amount of information that that black hole is hiding. And so I won't get into the next point, but I got to mention, it was this simple observation that the entropy of a black hole is proportional to its surface area. And that's another story that led directly from this notion of black hole entropy.
Starting point is 00:14:38 Okay, so we're all two-dimensional holograms. That's the takeaway from this. That's it. There's a real answer. Chuck, I always knew you were just a two-dimensional person. No, I thought you meant my character. Okay. Not my physicality.
Starting point is 00:14:56 All right. Give me another one, Chuck. That was cool. By the way, I don't know if I said that that was Deepan Das. That was the person. Deepan Das? Deepan Das. Oh, Deep the way, I don't know if I said that that was Deependoss. That was the person who gave us that. Deependoss. Oh, Deependoss. Deependoss.
Starting point is 00:15:10 Okay. Okay. And this is Anthropocosmic Dylan. Anthropocosmic Dylan. Anthropocosmic. I like it. Yeah. Very cool.
Starting point is 00:15:23 Hello, Dr. Tyson, Dr. Dow, Dr. Comedy. In space documentaries like PBS Space Time, they talk about future cosmic events in distant galaxies on Earth timelines. Instead of saying the sun will blow up in 5 billion years from the perspective of a galaxy far away, how do you adjust for the time dilation so that the information you're talking about is correct in the instant?
Starting point is 00:15:48 In terms of relatively, it seems like galactic simulations sort of step through a wormhole to film exosolar systems. Mm. Or that should be exosolar. So in other words, what is the rate at which time ticks on things we're observing?
Starting point is 00:16:07 And if it's not ticking at the same rate that it was ticking here on Earth, who are we to put it on our timeline? On the Earth timeline. I like that. Which, by the way, thank you, Neil, for making me understand what the hell he was talking about. So why don't we pick that up when we return in segment two on StarTalk Cosmic Queries. Weird, wacky stuff that our guest, Matt O'Dowd, is an expert in when StarTalk returns. Hi, I'm Chris Cohen from Hallward, New Jersey, and I support
Starting point is 00:16:45 StarTalk on Patreon. Please enjoy this episode of StarTalk Radio with your and my favorite personal astrophysicist, Neil deGrasse Tyson. We're back. StarTalk Cosmic Aquarius. Got Chuck with me. Chuck, you still there?
Starting point is 00:17:05 Yeah. I'm still there, man. Hanging with us. There's some deep stuff coming down here. Matt O'Dowd, friend and colleague from Lehman College of the City University of New York. So, you're an expert in this session. We've got you in for, like, quasars and black holes and weird, wacky, fun things that will kill you post-haste
Starting point is 00:17:26 in the universe. So what else you got? So what we were talking about before the break was from Anthropocosmic Dylan, who is actually Dylan from San Diego. In the short, what he was talking about,
Starting point is 00:17:39 it seems like galactic simulations kind of stepped through a wormhole to film extrasolar systems, exosolar systems, because, you know, they're not really on our timeline, but we put them on our timeline. So what's the deal? What's up with that? I mean, yeah, how do we reckon the relativistic effects of time dilation in an expanding universe on a timeline that we're just trying to set up for the universe here on Earth. Shall I take a shot at this, Neil?
Starting point is 00:18:09 Yeah, please. I just asked you because I don't want to answer. All right. I'm leaving this for you. The stuff that I study is far enough away that this matters. Many of you have heard that the universe is expanding, which means that
Starting point is 00:18:23 distant galaxies appear to be moving away from us, and you look far enough away, they're moving away from us at a big fraction of the speed of light. Okay, and so Einstein showed us that the rate at which your clock ticks depends on your motion, and the rates that you see a clock ticking depends on the motion of that clock relative to you. Okay, so fast-moving objects you see that their clock appears to be ticking slower, right. And so I, for example, studied quasars in the very distant universe and we really have to take this into account. Okay, so we might see these quasars fluctuating.
Starting point is 00:19:07 Okay, these are supermassive black holes that are eating a bunch of gas from their galaxy and they're pretty chaotic. They splutter and they splurt over time. Super interesting to study that variability. But if you're looking at something that's half a universe away, then this thing called relativistic time dilation slows down their sputtering
Starting point is 00:19:32 and spurting dramatically. And so you have to remember that and put that fact into your calculation otherwise you get it all wrong. Oh, okay. So you do factor it in. You actually make the adjustment. Fortunately, it's simple algebra. Einstein made that one easy for us.
Starting point is 00:19:49 Right, right. Yeah, I have my one paper that is co-authored with a Nobel laureate. I'm the last author on that paper. I think it was the first measurement of time dilation in a supernova light curve. Because you have supernovae in the outer universe, we have predictions of how quickly they'll brighten and how slowly they will dim and so we know what they look like nearby and out in the universe it was taking longer for that to happen so we can say is this a different kind of supernova or you plug in the expansion rate of the universe for its
Starting point is 00:20:22 distance and bada bing it it comes out right as you expected. So, yeah, it wasn't actually happening slower. It was a time dilation effect. So, this was profound. Yeah. That is very cool. By the way, you don't have to qualify being the last author on a Nobel laureate paper. You could just be an author on the paper.
Starting point is 00:20:44 Okay. Okay, that's enough. The lead author was Brian Schmidt, who won the Nobel Prize for the discovery of dark energy, which was empowered by measurements such as these with supernovae. And he's in Australia now, I think.
Starting point is 00:21:03 Yeah, he's been in Aussie for a long time. I mean, he was born in the now, I think. Yeah, he's been in Aussie for a long time. I mean, he was born in the US, I believe. But he's been, yeah. He's down under. For the longest time. Yeah. Mm-hmm. All right, Chuck, give me more.
Starting point is 00:21:15 Moving on to Brendan Gabassi. And Brendan says, hey, this is Brendan from Lansing, Michigan. And is it possible for a black hole of any size to be a quasar, given it has enough matter around it to heat up? And how close would a quasar have to be to the Milky Way in order for us to just see it in the evening sky? And if it's not too much to ask, can you elaborate on the news that is quickly spreading about the hole that's 20 times the size of Earth in the sun?
Starting point is 00:21:51 I mean, I don't think that's related to a black hole because our sun could never be one. But he's got anxiety. Be nice to the people with anxiety, Chuck. Tell me about the—hey, man, stop worrying about the hole in the sun. There's a black hole sun. Please. It's a black hole sun. Please. It's a question about holes. That's all it is.
Starting point is 00:22:09 It is. Question about holes. Nice job. Why don't you take the sun one first? Oh, the sun one. No, I am tempted to shift screen and Google that right now, but that would be cheating. Is it a sunspot maybe? Galileo. Yeah, I mean sun sunspots are, you know,
Starting point is 00:22:26 ordinary sunspots are about the size of the Earth, but the sun can have storms and explosions that are way bigger than Earth. Yeah, we are approaching a solar maximum in terms of magnetic storms. Right, that's in 2025. It's on the upswing. You know, I saw the Northern Lights
Starting point is 00:22:41 from right here on this deck a few weeks ago for the first time in my life. Wow. And this is New York State. Wait, you saw it aurora? I saw it aurora. You know, it was faint and it was, you know, but it filled the horizon. And, you know, you could see the curtains shifting very slowly.
Starting point is 00:22:58 Nice. Nice. Did you see colors? Or just the colors? Once my, yeah, once our eyes had really adapted, we could see a little bit. And what's your location now on Earth? We're upstate New York.
Starting point is 00:23:12 Upstate New York. Far away from city lights. Yeah, exactly. So that wasn't just the Empire State Building. Exactly. Oh, damn. Because the Yankees won or something. Okay.
Starting point is 00:23:24 Just checking. So anyway, and it's 20 times they they say, the size of the Earth. But then when you think about it, how many Earths can you fit inside the sun? A million. 110 in diameter. What, a million in volume? But yeah. Yeah, yeah, yeah.
Starting point is 00:23:37 A hundred across times a cube is a million, right? So you could put a million suns inside the entire ball. No, a million Earths. A million Earths. I'm sorry. A million Earths inside the ball that is the sun. But you would see,
Starting point is 00:23:52 what'd you say, a hundred Earths going straight across. Yeah. Yeah, about that. But I'm saying, if the sun can hold a million Earths, what are you worried about for a whole 20 times?
Starting point is 00:24:03 Exactly. For 20 times the size. Good deal. That's 20% of the diameter. That's not a small hole, but it seems to be shining still. I think we have another part of this question that I actually have some expertise in. Yeah, let's do it.
Starting point is 00:24:19 Yeah, so the rest of it. All right. So can you have quasars that are small? Like, you know, you can have relatively small black holes. Can they become quasars in the right circumstances? Well, sort of. So any size, any decent size black hole can form what we call an accretion disk around it.
Starting point is 00:24:40 So if you get gas close enough, the gas will form this whirlpool of material that's swirling into the black hole. The whirlpool will heat up. And it's from that heat glow that you get the super bright quasar. Now, a quasar and the related what we call active galactic nuclei are when you have a black hole in the center of a galaxy and they're big. But there are smaller black holes, what we call stellar mass black holes, that are left over after a massive star dies. And these might be, you know, 10 times the mass
Starting point is 00:25:11 of the sun, you know, up to, you know, several tens times the mass of the sun. And these things can form what look like mini quasars, but it's in a very special circumstance. And that's when that black hole happens to fall into a binary orbit or to have formed in the binary orbit with another star. Okay, now if those stars get too close, then the envelope of the living star can spill over into the influence of the black hole
Starting point is 00:25:40 and it starts getting siphoned off. So is the black hole eating that star? Is it slowly siphoning off and eating that star? It's flaying the star. Exactly. Flaying. Flaying. It's cannibalizing, vampirizing something.
Starting point is 00:25:53 It's eating the star. Well, I love that. Vampirizing. I love that. That's definitely what it's doing. It's sucking its life out. And then, so you get an accretion disk that's relatively small compared to, you know, a quasar, but it's still, you know, solar system size, it's still big.
Starting point is 00:26:07 And these are called X-ray binaries because we first saw them from the bright X-ray light that they emit. And these we see through the universe, even in the Milky Way. The nearest one is the Cygnus X-1 black hole, which is about 1,000 light years away. So we do get mini quasars. So these are basically nearby baby quasars. Well, baby, except they're not going to grow up to be adult quasars.
Starting point is 00:26:34 Oh, yeah. Okay. What would you say is the threshold between just an active galactic nucleus and what we officially would label as a quasar. Yeah, it's a, you know, the definitions are muddy because these things are very far away. And they all, all these active galactic nuclei look a bit different depending on, you know,
Starting point is 00:26:56 how much gas is going in, how big the black hole is, even what is the orientation of the accretion disk. At some angles, we don't even see it because there's a bunch of gunk surrounding it that blocks it. So there could be galaxies that are quasars for some parts of the universe and not for others. Yeah, absolutely.
Starting point is 00:27:15 Yeah, okay. That's interesting. So it's an orientation thing. Exactly. But the threshold for a quasar, it's essentially a very luminous active galactic nucleus in which we can see the accretion disk. So you have these two parameters,
Starting point is 00:27:30 the luminosity, which is partially driven by the black hole mass. A bigger black hole mass can support a bigger disk. It's complicated. Now, Matt, what I heard is it's still true, because it's been a while since I've looked at this, that the reason why quasars are all far away is because nearby galaxies that may have once been quasars ate all of their gas.
Starting point is 00:27:52 Right. They completely consumed their accretion disk. So there's nothing left to regulate. Get in my belly. They've eaten it. Is this a fair... Because the quasars at the edge of the universe, that's long ago.
Starting point is 00:28:04 And far away. In a galaxy far, far away. The nearby galaxies have done lived their early lives, done eaten their, and so we don't have a prevalence of quasars nearby. Is that understanding still accurate? The short answer is you're totally right. The longer answer is you're partially right. And there's another effect so it's true that that the universe went through something that we call the quasar epoch which was yeah like you know ended a few billion years ago uh and and the quasars so there's this kind of middle period of
Starting point is 00:28:39 of the universe's life where the quasars flared up in the biggest galaxies that exist in the universe. And that basically corresponded to when those galaxies were being built. Okay, so as the Big Bang happened, galaxies started being built. So there was a supply of food. A supply of food for the biggest galaxies, which had the biggest black holes. Nowadays, those galaxies are basically done being built and more of the
Starting point is 00:29:05 galaxy building action is for the lower mass galaxies, like some spiral galaxies, a bit more like the Milky Way. And these things don't tend to create big quasars. But the other effect is that full-blown quasars aren't that common in the universe. And so we don't even have a galaxy that would have been one very close to us. Right. So now you say they're not that prevalent or common in the universe. Could there still be a lot more that we haven't seen?
Starting point is 00:29:44 Just because how much of the night sky have we actually seen? You know what I mean? Or does it work out that what we have seen, you can extrapolate and say that we're going to see that exact amount if we were to see everything? Yeah, I mean, I think you answered the question, Chuck, so thanks. But we've seen a lot of the universe. Our surveys
Starting point is 00:30:07 have scanned a huge volume of the universe. It's hard to look directly through the disk of the Milky Way because there's too much stuff in the way, but above and below we've seen a lot, and we've found many hundreds of thousands of quasars there. So I say they're not common, but the
Starting point is 00:30:23 universe is big. But we see them. Yes, big. A big universe, rare things are common. Corbundant or something, yeah. It makes perfect sense. Makes perfect sense, right? It just makes perfect sense.
Starting point is 00:30:43 It can't get any simpler than that. All right. Well, just to be clear, if one in a million people is seven feet tall, then in a country of 300 million people, they're 307 foot taller. So... You still might not get on the basketball team. You're right.
Starting point is 00:30:54 Yeah, the big numbers bail you out of that. Right, exactly. And of course, what's the adjective we have for big numbers? They would be astronomical. Yes. We kind of corner the big numbers, don't we, Neil? Yeah, we totally own the big numbers.
Starting point is 00:31:13 We got all the big numbers. That's for sure. Biggest numbers. All right, give me another one. This is Cameron Bellamy. He says, greetings from Baltimore, Maryland. On this show, Neil has talked about the consequences of our expanding universe and its eventual big rip. I'm curious how this phenomenon will affect black holes.
Starting point is 00:31:33 From my understanding, black holes are super dense matter. And space-time expands. Will the super dense black holes become less dense until eventually representing matter density similar to what the rest of the universe has and thereby being able to be ripped? Will the opportunity for life arise from what was once a black hole as the universe expands in the far distant future? Damn, my boy's thinking about this stuff. Let me tell you, this question he should have followed up with, and it only took me one year
Starting point is 00:32:13 to think of this question. Alright, we're going to pick up the answer to that at the beginning of segment three, right after this break. We're back. Cosmic Queries. Based on the expertise of my friend and colleague,
Starting point is 00:32:40 Matt O'Dowd, who teaches at Lehman College of the City University of New York. And Matt, how do we find you on social media? Beyond your YouTube channel, which has 3 million followers. Yeah, so you could go to PBS Space Time and just watch me talk about space and quantum mechanics
Starting point is 00:32:58 and everything physics. I've seen episodes. You're great. You're totally there, friendly and informative and I always want more when I see it. So congratulations on what you've created there. Appreciate that. And it's a part of the PBS universe. Yeah, it's a PBS show.
Starting point is 00:33:13 PBS Digital Studios, to be precise. Otherwise, I am Matt of Earth Underscores on Twitter and on Instagram. Matt of? Matt of Earth. Of Earth. Earth. This is Earth's Matt. This is Earth's Matt. Mars has its own Matt. Just in case
Starting point is 00:33:35 people are wondering. Alright, we're picking up where we left off. We had Cameron Bellamy who basically was saying when you look at the Big Rip and you consider black holes. Will it affect black holes? Yeah. Will it affect black holes?
Starting point is 00:33:48 And does it affect them differently because they're so dense? Yeah. What do you know about that? Yeah. So this is pretty speculative, but I'm going to take my best guess. So the big rip is
Starting point is 00:33:57 probably not going to happen. It only happens if dark energy is something more exotic than most physicists think it is. If the happens if dark energy is something more exotic than most physicists think it is. If the strength of dark energy increases over time, then eventually the accelerating expansion of the universe can affect smaller and
Starting point is 00:34:16 smaller regions, eventually subatomic scales tearing everything apart, blah, blah. Okay, so if that's the case, then it would affect black holes, I think, because black holes contain space, and if that space contains an increasing amount of dark energy, that dark energy has an anti-gravitational effect. I think what it would do would be to cause black
Starting point is 00:34:41 holes to evaporate more quickly. That would be my guess. So black holes are evaporate more quickly. That would be my guess. So black holes are evaporating, as we learned, by Hawking radiation, my guess. So the event horizon is shrinking. So my guess is that a Big Rip-style dark energy would cause that evaporation to happen more quickly. So my guess, I'd like to hear what you said there.
Starting point is 00:35:01 My guess is that the opposite will happen, is that they'll evaporate less quickly because the expansion dilutes the energy density in their environment. Around the black hole? Around them, and which will make it less likely to produce the particles.
Starting point is 00:35:17 However, what you said seems to be all in, where the black hole volume is made of space-time, like anything outside the volume. is made of space-time, like anything outside the volume. And it's space-time that's getting stretched. So I can imagine the Big Rip simply unzipping black holes. Right. Right?
Starting point is 00:35:37 And because it's stretching them out so that they no longer have their black hole event horizon density. Yeah. I bet someone has calculated this. I need to find out. Yeah. So I haven't calculated it, but some combination of our two answers
Starting point is 00:35:54 sound like it could be it. Now, let's get back real quick because I know we don't have a lot of time left in the show because we've got to get to more questions. Do it. Please go back to why the big rip is not going to happen because you're the first person. No, no, no. It will happen if the strength of this dark energy
Starting point is 00:36:10 grows relative to gravity as the universe expands. It will happen. What Matt was saying is, we're not entirely sure that dark energy will grow in strength as the universe expands relative. Did I characterize it correctly? Yeah, the default model for dark energy is that it maintains a constant energy density. Maintains a constant.
Starting point is 00:36:31 Okay, I got you. Now, I'm totally straight now. Okay, great. Okay. That's awesome. All right, let's go to our friend, Alejandro Reynoso. I have to assume he's not offended by this, Chuck, because otherwise we would have gotten mail from him by now.
Starting point is 00:36:52 We have not. We have not received any cease and desist orders from Alejandro Renoso. So Alejandro Renoso says. So the authorities haven't shown up at your door. They haven't. So, Alejandro Reynoso says... So, yeah. So, the authorities haven't shown up at your door. They haven't... Okay. And where's he from, Chuck? This is Alejandro Reynoso from Monjere, Mexico.
Starting point is 00:37:17 And he says, hello. Okay. Or should I say, hola. Now, then he says, my question is, how do you use gravitational lensing in your observations? Does it actually let you see distant objects clearly? Or do you need to make many adjustments to come up with your image? So how are you utilizing gravitational lensing?
Starting point is 00:37:42 Yeah, Matt, what does your object look like after it's been gravitationally lensed? Great. I love this question because I know about it. For one, so... The Einstein guy, again, predicted that gravitational fields bend the path of light, bend the fabric of space-time. And so you look out there in the universe and you see that distant
Starting point is 00:38:07 objects aren't necessarily where they appear to be. Particularly if there's something big like a whole galaxy between you and that object. And the things that I'm interested in are gravitationally lensed quasars. There we go, quasars again, where you have a distant quasar, an intervening galaxy, and you just happen to be perfectly lined
Starting point is 00:38:28 up so that the light from that distant quasar is deflected by the gravitational field and comes back towards us. And so we actually see the same quasar through multiple paths through space. We get light from multiple different paths through space. So it actually looks like you see two images or four images, but really there's always an odd number of images. And that's because in between the two images or the four images, there's a tiny little image of the original object.
Starting point is 00:38:57 Normally you can't see that because you've got this great big galaxy or whatever is doing the lensing in the way. But yeah, fun fact, you always get an odd number of is doing the lensing in the way. But yeah, fun fact, you always get an odd number of images with gravitational lensing. So my interest is in trying to use gravitational lensing to probe the inner structure of those quasars. So you
Starting point is 00:39:19 have this giant accretion disk around the black hole, but really these things are so far away that there's no telescope that we can even imagine building that'll be able to take a real picture of a quasar and see that in a structure. But in the case of gravitational lensing, you can basically reconstruct what the quasar looks like because you have one more effect at play. So the lens, if it's a galaxy, is a pretty crappy lens. It's made of stars.
Starting point is 00:39:47 And because everything in the universe is moving relative to each other, you see occasionally you'll get this extra special alignment of a star inside the lensing galaxy with one of these pathways. So one of these pathways might pass in the gravitational field of an individual star with such an alignment that
Starting point is 00:40:07 that one image grows in brightness and then shrinks again. And so over time you see these, let's say there are four images, you see them flicker on different time scales. And from that flickering you can actually reconstruct the inner structure of the quasar because the rate of the flickering depends on how big the quasar is. And so you can sort of map it out in this way. And I remember I was active in graduate school when this first measurement was made
Starting point is 00:40:37 where someone looked at one of the lensed quasars and it flared in some way. And then they waited for the other image to flare. And it flared in exactly the same way. That's crazy.
Starting point is 00:40:51 And that time delay was the path length difference between one direction around the object and the other. I mean, it was a brilliant thing.
Starting point is 00:41:00 Everyone was sitting around waiting for it and bada bing! There it is. That is really cool. And you know what? That's how you knew it was the same object. It had to be the same.
Starting point is 00:41:08 It was just on a delay. It was on a time delay. Because it did the exact same thing. Wow. Exactly the same thing. Wow. I know, I know. I thought the same way.
Starting point is 00:41:15 That is so cool. Because initially, you don't know what it is. It's just an object in the image. Right. And so, I was in graduate school when that happened. That's how old I am, Matt. I'm like decades older than you. So I remember when this stuff was... Well, you know, that exact thing, like measuring the different path lengths is going to be one of the ways that we actually
Starting point is 00:41:36 figure out what dark energy is. Because if you can measure those different path lengths, you can get the distances to the lens, to the quasar. And so you can actually map the expansion history of the universe by getting those distances. And that's one of the ways we might be able to figure out the rate at which the universe is accelerating. Right. Because, oh my God, that's it. Because the universe is actually not just expanding at a constant rate.
Starting point is 00:42:03 It's speeding up. So when you're able to get those distances and see the differences on the delay, you can actually kind of calculate the dark energy because that's what's behind it, right? Yeah. Damn! Oh, God!
Starting point is 00:42:17 Science is amazing! Science. Wow! Okay. Okay, that's amazing. No, but we still, there's still people who walk among us and say, Okay, that's amazing. No, but we still, there's still people who walk among us
Starting point is 00:42:28 and say, Adam, that's science. That makes sense. Science is in. What is wrong with people? What is wrong with people? This stuff is so... We're figuring out
Starting point is 00:42:38 the time delay through different path lengths around a lens galaxy across 80% of the universe. And you're saying, Adam, that's science. If that're saying, I need night science. If that doesn't get you, nothing will. That is some amazing stuff right there.
Starting point is 00:42:49 All right, here we go. This is Renee Scroop. Renee Scroop says, Hey, guys, I just heard about the red star Arcturus and that I could have a planet or substellar object orbiting it 12 times larger than Jupiter. About a month ago, you had a guest on that said Jupiter was the largest planet ever discovered. So what do you think could be orbiting?
Starting point is 00:43:14 Can't wait to hear the answer. Thanks from Orange County, California. Rene. Okay, I don't know that we had a guest that said Jupiter was the largest planet ever, because it's definitely not. All right. that we had a guest that said Jupiter was the largest planet ever, because it's definitely not. All right? Plenty of
Starting point is 00:43:25 other planets in the exoplanet catalog are bigger than Jupiter. The difference is, if you start getting much bigger than Jupiter, we don't really call them planets anymore. Right? I mean, they're like brown dwarfs. We have other vocabulary for them. So that's really what's going on here.
Starting point is 00:43:41 They're failed stars. Failed star. Matt, do you have any insight into that question? Yeah, I mean, I'm not aware of this result, but 10 times larger, 12 times larger than Jupiter is really getting on the verge of the smallest star level. Well, 100. So it's a brown ball. So the question is, is it a planet or is it a failed star?
Starting point is 00:44:00 And I think the answer is it depends on how it formed. You know, if the two form together by collapsing from the same giant cloud of gas and finding each other, then it's a binary star system. One of them is just a failed star. But if the big star formed first and then this giant Jupiter formed in the disk of leftovers around that star, then you might call it a giant planet. But...
Starting point is 00:44:26 Yeah, so the origin story matters. The origin story matters, it sounds like. That makes sense. So one's cleaning up stuff. Yeah, exactly. And the other... The other one is out of the same birth sack. Out of the same...
Starting point is 00:44:37 Right. Wow. Okay, cool, man. Yo, that was a cool question, Rene. Thanks. I kind of dig it. Here we go. Trisha Lynch says, Hello and greetings from a cool question, Rene. Thanks. I kind of dig it. Here we go. Trisha Lynch says,
Starting point is 00:44:46 Hello and greetings from Beaverton, Oregon. My question is, what would happen if galaxies stopped rotating? What? What would happen? It wouldn't be good. Let me tell you that. Next question.
Starting point is 00:45:01 There you go. Thank you, folks, and good night. There you go, Trisha. Hope you can sleep. No, no, and good night. There you go, Tricia. Hope you can sleep. No, no, no. I got one. I'm going to tee up Matt on this one. You ready?
Starting point is 00:45:10 So if the Milky Way stopped rotating today, then every single star would fall to the center. Yeah, immediately. Because it's its orbital speed that's maintaining our distance. Without that orbital speed, they will fall to the center. Immediately. Because it's its orbital speed that's maintaining our distance. Without that orbital speed, they will fall to the center. And Matt, what do you have waiting for everybody at the center?
Starting point is 00:45:31 Behind door number one, Matt. My favorite cosmic friend, the supermassive black hole. There you go. Sagittarius A star. Four million suns worth of black hole. And, I mean,
Starting point is 00:45:44 if they really stopped perfectly, then technically everything would, well, yeah. It would be a mess. It would go straight to that black hole. It wouldn't be four million, it would be billions of times the mass of the sun. Is the black hole exactly in the center of mass of the Milky Way? I'm not sure.
Starting point is 00:46:00 I'm not sure. So they might do close, you know, everything would end up in these giant... I don't know if it's exactly in the center. Good question. ...things, but there'd be collisions and... Yeah, it would be bad. All around.
Starting point is 00:46:13 And the whole galaxy could just be eaten by the black hole at that point. That would be interesting. Wow. All right. Yeah, that's... That'd be something Thanos would do. That would be.
Starting point is 00:46:24 Just, yeah. You don't like me when I'm angry. Except he doesn't snap a finger. That would be. Just, yeah. You don't like me when I'm angry. Except he doesn't snap a finger. He actually claps. Like the clapper that turns the lights off. Turn the galaxy off. And then everything just falls to the supermassive black hole in the center of the galaxy.
Starting point is 00:46:37 Or the choreographer on Broadway. Step up to the thing. Yeah, that would be, that's how to destroy a galaxy on the spot and make a super massive, super duper massive black hole. Look at that. All right, here we go.
Starting point is 00:46:52 Ignacio Carasconi says, or Caracasoni says, hey, greetings from Brooklyn, New York. My kid and I are fans of the show. That's right. And we have been to. He and who are fans? My kid and I are fans of the show. That's right. And we have been to... He and who are fans? My kid and I are fans of the show.
Starting point is 00:47:10 And we have been to the Hayden Planetarium at least a dozen times. Nice. So my question for Matthew, Neil, and hello, Chuck. Yeah, he ain't asking me anything. Just saying hi. Okay. He says, why is solar gravitational lens mission hasn't happened yet and when is it likely one of the most powerful tools to study exoplanets and find life besides our local sample when will that happen happen? You know, I think...
Starting point is 00:47:46 Matt, do you think he's talking about the lensing that Bodan Pachinsky was doing, the microlensing? Do you think that's what he's talking about there? This is a plan to send out a little telescope to a point in the outer solstice. So there's a point in the outer solstice. So there's a point in way out beyond Neptune. I was going to say Pluto, then I realized you were here,
Starting point is 00:48:13 Neil. Way beyond Neptune. And so there's this point where, and so you've got the sun. The sun is a big gravitational object. It bends the path of light. And there's this region. I can't remember how far away it object. It bends the path of light. And there's this region. I can't remember how far away it is. It's like a week light travel time away or something like that where light from a distant object will come to a focus due to the Sun's gravitational field.
Starting point is 00:48:39 And if you could put a telescope in this, basically this focal range. I remember this telescope. Yeah, yeah, yeah. This sort of you know, and it extends over a certain range because it depends on how far away the object is. But if you put a telescope
Starting point is 00:48:55 there, then the sun would become an extra lens on that telescope and it would produce such powerful magnification that you could see, so the calculations go, a single planet orbiting around a distant star, which is something that is extremely difficult for us to do. I remember this, but then I stopped reading about it.
Starting point is 00:49:18 So has this idea gone away? No, it hasn't gone away. You know, people have been thinking about it for a long time and are still, like I hear people talking about it and that we should do it. But wait, but Matt, isn't the sun in the way? How are you going to see a lensed planet when the sun is brighter than everything?
Starting point is 00:49:38 It's like trying to find a firefly in a Hollywood searchlight. How does this actually work? I agree and I see where you get the magnification effect. That would be amazing. I get that. But there's still the matter of this. I guess you have to have some kind of like a some kind of disc that blocks the sunlight
Starting point is 00:49:56 in the telescope. You'd have to have something like that. I love it when you ask me a question and then answer it perfectly. So, I mean, you know, I'm just thinking it up on the fly. I'm sure you know about coronagraphs, we call them, which are... Yeah, yeah, yeah. And there are ideas about how you would build
Starting point is 00:50:13 these giant coronagraphs, basically a big circle, but there are also various interesting complex things that would unfurl in front of this distant telescope that would block the sun's light. And so you could see this, you know, basically this ring. So what it would look like would be the sun blotted out, but then surrounding the sun, this perfect ring, what we call an Einstein ring.
Starting point is 00:50:41 And that perfect ring would be the exoplanet. Okay, so if it were another civilization doing this for the Earth, they would use their star to look at the Earth. If they just happened to be in the right position to do that, then Earth's structure would be smeared around. But to the level that if you reconstruct
Starting point is 00:51:01 it, and you could reconstruct it just by using good old Einstein general relativity to figure out what the image looked like, you know, and... So anybody could do it. Yeah, anybody could do it. Literally, literally anybody. You could see, you know,
Starting point is 00:51:19 continental coastlines down to, I can't remember the exact scale, but, you know, kilometers or something like that. So you could literally map the surface of that distant planet. But you'd have to reconstruct the sphere from the smeared surface. Exactly, yeah.
Starting point is 00:51:33 The visual image from that, right. So that'd be what a task that would be. I forgot all about that telescope. Matt, thanks for reminding me of that. I gotta tell you the truth. It sounds like the worst camera ever. I'm sorry. It really does.
Starting point is 00:51:45 I don't want to be a hater, but I'm just saying. Chuck, hating on the most advanced system. No, I'm joking. So, Matt, we've got to call it quits there. Man, that went fast. Sounds good. Geez. I'm sad, Doc.
Starting point is 00:51:58 All right. Well, you know what? Let me give you one quick one because this guy is personal and professional, this question. It's a personal professional question. This is David Lees or Lees. And he says, Hello, Dr. O'Dell. Have there been any surprise findings in your research
Starting point is 00:52:12 that have shaken up your understanding of astrophysics? In my personal research? In your personal research. I wish. In my personal research, have I shaken up the understanding of my, oh man, now I'm going to get sad because I don't think I have personally revolutionized my own understanding.
Starting point is 00:52:35 You know, there have been things that have surprised me. There's been objects that I've studied that have surprised the hell out of me. Gravitational lenses that have done things that I really didn't expect them to. I have managed to find ways to look at the interiors of quasars that are relatively new and found things like... Yeah, that's good. So it's not a new object, it's a new tactic.
Starting point is 00:53:01 Yeah, yeah, yeah. New tactics, but... You're a little hard on yourself there, man. I know, right? You're a little hard on yourself. He's a weird stuff out there. And for everybody listening,
Starting point is 00:53:11 you just found out the heart of every scientist right there in that question and answer. Because scientists, what they don't want to do is succeed. What they want to do
Starting point is 00:53:21 is look down and go, what the F is that? What? What the F is that? What? What the F is that? Oh, my God. Come over here. What is that? That's what gets scientists all freaked out.
Starting point is 00:53:33 That's how it works. Yeah. It's not the discovery of what you know. Right. It's finding something you have no idea what the hell you're looking at. Right. Right. So, all right.
Starting point is 00:53:42 All right, dudes. We got to call it quits there. So, thank you for yet another episode of StarTalk Cosmic Queries. Neil deGrasse Tyson here, as always, bidding you to keep looking up.

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