July 5, 2026
Cosmic Queries Unleashed: Gravitons, Expanding Universes & the Weight of Space Travel
Universe, and WeightlessnessIn this Q&A edition of Space Nuts, Andrew Dunkley and Professor Fred Watson tackle an array of intriguing listener questions that delve into the complexities of the universe. From the implications of an expanding universe to the elusive graviton and the experience of transitioning from weightlessness back to Earth's gravity, this episode promises to enlighten and entertain.Main Topics:
- The potential for a future black void in our night sky as the universe continues to expand.
- Understanding the graviton: Why do some physicists believe in its existence despite its elusive nature?
- Exploring the properties of photons and their wave-particle duality.
- The impact of long-term weightlessness on astronauts and their return to normal gravity.
- Listener feedback and inspiring stories about engaging younger generations in astronomy.
- 00:00 - Introduction to today's Q&A session and listener engagement
- 02:30 - Clint's question about the future of the night sky and cosmic expansion
- 12:45 - Alan's deep dive into gravitons and their connection to gravity
- 28:00 - Misty's inquiry about the wave function of particles and photons
- 40:15 - Casey's question on the effects of returning to gravity after weightlessness
- 50:30 - Final thoughts and encouragement for listener questions
Join Andrew and Fred Watson for another fascinating exploration of the cosmos, and don't forget to send in your questions for future episodes. Keep your curiosity alive and continue to look up!
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Andrew Dunkley: Hello again. Thanks for joining us. This is a
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Q and A edition of Space Nuts. We talk
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astronomy, space science, and answer
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audience questions. Well, maybe we won't do
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one of those three things today. I don't
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know. We'll see how it goes. Uh, we've got a
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lot of questions to get through today. Um,
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Fred Watson reckons some of these are very,
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very tricky, so we'll see how it all pans
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out. Um, a question about the expanding
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universe. Never had one of those before. Uh,
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a question about gravitons. Never had one of
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those before. Yes, we have. Uh, photons
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and weight shift. That's all coming up on
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this edition of space nuts. 15
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seconds.
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Professor Fred Watson: Guidance is internal. 10,
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9. Ignition sequence start.
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Space nuts. 5, 4, 3. 2. 1, 2,
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3, 4, 5, 5, 4, 3, 2, 1.
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Andrew Dunkley: Space nuts. Astronauts report it feels
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good. And joining us once more to
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unravel all of that, or maybe ravel it
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up even more, is Professor Fred Watson
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Watson, astronomer at, uh, large. Hello,
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Fred Watson.
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Professor Fred Watson: Hello, Andrew. I do feel pretty ravelled at
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the moment.
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Andrew Dunkley: Yeah, look, we have got some tricky
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questions, but before we get to those, uh,
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we've received a note from Rennie in
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California.
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Uh, Rennie quite regularly sends questions
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into us, but he sent us a really lovely note
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which I want to share. Uh, he says no
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questions today, just to thank you. I try to
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absorb as much information as I can listening
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to your podcast. And when I'm engaged in a
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convers conversation with my two grandsons
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aged 15 and 12, I try to excite
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them and get them to think about our place in
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the universe and how it behaves. Now it's
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paying off with the announcement that my
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older grandson wants to carry on in college
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with some form of education in astronomy
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or particle physics. Thank you for paying
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it forward, Renny. Isn't that lovely?
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Professor Fred Watson: Yeah, that's great. Absolutely great.
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Andrew Dunkley: Uh, I love it when we get feedback from
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people that, that become inspired
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despite us.
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No, I mean, it's fantastic.
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Professor Fred Watson: It is.
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Andrew Dunkley: I'm really, really pleased. Really pleased.
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So, um, pass on our regards, Rennie, to your
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boys or, uh, your grandsons, um, and wish
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them well and. Yeah, look, just.
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I do the same thing with my grandson and
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three granddaughters. Um, I talk to them
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whenever there's something interesting to
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talk about, and there usually is, uh, in the
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astronomical world. And, um, I show
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them the images I take with the Telesco, and
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I've even had them outside looking up at the
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moon. And, um, yeah, it's captivating. Once,
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once they, you know, once you can convince
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them to actually get outside.
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Um, you know, the universe is their
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oyster. It's, uh, it's good
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stuff. So lovely to hear from you, Rennie.
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And that is really fabulous news.
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Are you ready for your first question,
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Fred Watson?
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Professor Fred Watson: Well, after a. Yes. After a build up like
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that, I guess we've got to tackle them,
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haven't we?
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Andrew Dunkley: Uh, we probably should.
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Professor Fred Watson: You're right, in a way. You know, the
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ultimate notes, I guess,
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is to provide that little bit of perhaps
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inspiration that might lead people to do
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things that might one day change the world.
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Who knows?
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Andrew Dunkley: Yep, you just don't know. You just don't
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know. Maybe that's our lot in life is to just
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try to inspire, uh, just a handful of people
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to pick up the baton, Fred Watson. Who knows?
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All right, question one. It's like a test,
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isn't it?
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Question one. Uh, if space is
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expanding faster than the speed of light,
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then in millions or billions of years from
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now, will our night sky be completely black
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or a completely black void? Um,
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uh, or completely black, devoid of
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all light except our local solar system. That
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comes from Clint. Uh, this is
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something that has come up occasionally and I
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think even in one of our most recent
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episodes, we were talking about the expansion
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of the universe and its significance. And,
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and I think in our Q and A episode, someone
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asked about the expansion of the universe.
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Um, so here it is again.
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Um, we are, ah,
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expanding, and it's
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expanding at an accelerating rate. Although
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it's debatable whether or not that
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acceleration is actually as m. Significant
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as it was. That is a
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separate debate. Um, but I think it's pretty
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clear that in the long distant future
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of this universe, it will become a black
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void, won't it?
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Professor Fred Watson: Uh, yes. So the answer to Clint's question
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is yes.
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Andrew Dunkley: Okay, question
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Professor Fred Watson: no. Exactly. As you said, um,
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if you've got, um. So
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when you say the universe is expanding more
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than the speed of light, you've got to be a
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bit specific because really what you're
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talking about is objects within
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the universe which are being carried along by
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the expansion of the universe. And so,
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uh, there will be, at a certain
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distance from us now,
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objects whose, what we call the recession
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velocity is faster than the speed of light,
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but they're actually, they're beyond
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the wall that we can't see beyond anyway,
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which is the cosmic microwave background
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radiation. But you can imagine as the
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expansion continues to accelerate, and you're
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right, it is still thought to be
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accelerating. We just don't quite know
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whether that acceleration is a constant.
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That's the thing you were alluding
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to because there's some evidence that
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maybe the acceleration is reducing,
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but nevertheless it's still accelerating. So
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it's still getting bigger, faster, uh, all
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the time. And so what that would do,
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um, you can, you can sort of
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imagine in your head what this situation
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would lead to. It means that the,
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the, the sort of black horizon, the horizon
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which is where light can never get to you
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because it's being carried away. The objects
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are being carried away faster than the speed
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of light. That black horizon will, will
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approach, um, it'll get nearer
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as the universe's expansion continues to
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accelerate. So eventually you can imagine
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that maybe you would see just
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the other galaxies in the Local Group, uh,
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which is Andromeda and the, uh, triangular
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whirlpool galaxy and things like that. But
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eventually, yeah, it might just be
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objects in our own solar system, uh,
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which makes astronomy a little bit of a.
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Boring. Yeah.
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Yeah.
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Andrew Dunkley: Well, let's go see what we can find. Oh,
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there's the moon.
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Professor Fred Watson: Yeah. Yeah. Oh, wait, it's gone.
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Andrew Dunkley: Well, it's moving away from us too.
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Professor Fred Watson: So it is rather slower than the speed of
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light. Yeah. Six centimetres a year.
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Andrew Dunkley: I can't imagine this is going to happen in an
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awful hurry, Fred Watson.
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Professor Fred Watson: No, it's not. It's very, very long way down
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the track. And of course, from our
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perspective here on, ah, Earth, long, uh,
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before anything like that takes place,
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um, we'll have been
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confronted by the expansion of the sun
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itself, um, as it turns into
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a red giant star.
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Andrew Dunkley: Yeah. Who knows where we'll be in the
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universe by then. We might have moved out
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into other parts of the galaxy by then if
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we've managed, um, to find some kind of
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propulsion system or learn how to fold
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space or whatever it is you need to do. Uh,
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maybe develop wormholes and be able
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to travel mega distances.
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Professor Fred Watson: Yeah. Fast. You're the person, you're the
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science fiction writer. You've got to tell us
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what it is we're going to do.
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Andrew Dunkley: Uh, I'm working, um, uh, on
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warp, uh, warp travel at the moment.
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Professor Fred Watson: Oh, good.
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Andrew Dunkley: In m. My. In my novels. So,
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yeah, I'm doing the final editing at this
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stage and it's, uh, it's the most horrible
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job.
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Professor Fred Watson: It is, isn't it? Yeah.
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Andrew Dunkley: Especially writing's fun.
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Professor Fred Watson: Yeah.
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Andrew Dunkley: But then you've got to fix all your blunders
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and you don't realise how really hopeless you
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are until you have
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Professor Fred Watson: to edit your own stuff.
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Andrew Dunkley: Yeah, yeah. I'd pay someone, but I can't
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afford it. It's not a, it's not a cheap
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thing to get Done book editing. Um,
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but anyway, uh, so the basic
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answer to Clint's question is yes, it's going
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to happen. Uh, there will be complete black
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nothingness, um,
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in a matter of about three weeks time, or
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could be three gazillion years time.
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Professor Fred Watson: I think the latter's more likely.
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Andrew Dunkley: More likely the latter. Thank you, Clint.
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Great to hear from you.
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Our next question comes from
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somebody whose name I forgot to write down.
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Uh, no, it didn't. It comes from, uh, Alan.
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Now, this is a pretty big question, so I'll
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just go straight through it and we can figure
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all out the rest out later. Uh, I know you
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want audio questions, but you know how they
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say you have a face made for radio? I've got
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one of those. Well, uh, I have a voice made
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for text. That's very
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good. I, um, hope it's not true. Uh, I
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discovered space nuts more than a year ago
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and have listened to your entire back
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catalogue.
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Professor Fred Watson: Wow.
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Andrew Dunkley: Wow. Get a job. No. Fantastic. Thank
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you. Uh, still listening and have not lost my
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mind yet.
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Professor Fred Watson: Wow.
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Andrew Dunkley: That's a record.
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Uh, here's something that's been bothering me
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for, uh, some months. Some physicists
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don't believe relativity, uh, when it says
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that gravity is not a force. Also, they
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believe that all forces are conveyed by
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particles. To unify gravity with other
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forces, they postulate the graviton to be
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that particle for gravity. It's said that
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nothing escapes a black hole, but actually
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gravity does. If gravitons exist
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and convey the force of gravity, then they
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escape black holes. So they are not affected
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by gravity. That means they do not affect
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each other. We know gravity does affect all
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massive particles and photons, massless
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particles that convey the electromagnetic
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force. I don't know if gravitons affect other
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massless particles. This is the interesting
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part. If f equals gm 1 m
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2 divided by d squared is
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the complete calculation for the force
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of gravity, no modifications introduced by
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relativity or quantum physics, then gravitons
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are not affected by anything. So gravitons
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affect every particle except gravitons and
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are not affected by anything. So is
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an asymmetry that breaks
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conservation, uh, of energy and momentum. My
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question is. Here it is. Why do some
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physicists still believe in
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gravitons? That comes from Alan in San
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Antonio, Texas. Boy, Alan, you've put a lot
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of thought into that. You really have.
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Professor Fred Watson: Yeah. And these are questions that are right
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on money as well. Yeah. Uh, especially the
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last one. Why do physicists believe in
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gravitons? I think most physicists probably
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do. Uh, Alan, because
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um, we know that gravity is a fundamental
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force and all the other fundamental forces
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have their subatomic particles,
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uh, which are basically
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um, um,
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particles that can. That sort of what we
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call, we call them bosons. They're what, they
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carry a field in a way. And the field is
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another way of looking at how a uh,
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force works. I didn't
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phrase that very well, but uh, that's why
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some physicists believe in gravitons. We've
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never found them. We don't have a particle
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physics theory of gravity. Uh, so we don't
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know that they exist. But I think most
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physicists would assume that they exist.
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And so uh, that
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first um, conundrum
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that you mentioned,
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if nothing escapes a black hole, well,
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gravity does. And so if
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gravitons exist and convey the force of
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gravity, then they escape black holes. So
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they're not affected by gravity. That means
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they do not affect each other. But in
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fact, um, uh,
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the bottom line with black holes it's
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quite complicated. Uh, but you
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don't have gravitons escaping
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from the black hole. Uh,
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the way people who know a lot more about
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these things than me, uh, the way they
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envisage this is that the gravitational
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field of the black hole is a kind
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of fossilised one that was
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established before the collapse
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into uh, a black hole.
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Or, and here's another way of looking at it.
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This really, you're gonna think, um, Alan,
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this is a cop out, but this is the way the
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physicists see it. Uh, the,
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the gravitational field of black hole
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basically uh, includes
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something called virtual gravitons.
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Uh, and so that sort of ties in with the fact
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that the, the gravitational field is a
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fossilised footprint, if I can put it that
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way. Um, the
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virtual gravitons, uh, are an
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embodiment of that, but they don't
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necessarily obey the
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normal laws of physics.
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So
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uh,
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basically what you've got here, and
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I think, um, the
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physicists who look at this problem probably
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just automatically drop into the two
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camps of relativist people who
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are ah, experts in general relativity. That's
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Einstein's theory of gravity that says, yes,
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um, gravity is not a force, it's just a
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distortion of space. Uh, and the quantum
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mechanics people who look at it from the
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perspective of gravitons.
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Um, and so yeah, the virtual particles,
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uh, the quantum mechanics
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person's answer to this,
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uh, they're basically
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just mathematical constructs, uh, in a
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quantum field. And so they don't have to
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obey speed limits or anything like that, or
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even don't have to worry about the event
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horizon so they can continually
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basically, uh, keep the gravitational force
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there without actually being
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trapped by it. I think that's the way
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physicists look at it.
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Andrew Dunkley: Uh, all that says to me is
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something. It's still a big mystery. There
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are so many different theories behind
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gravity, and we really don't know what it is.
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We know what it is, but we don't know why it
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is.
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Professor Fred Watson: Well, no. So all we know about
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gravity is the way it behaves. Um,
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we really don't know what it is. And in a
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way, Alan's question is well posed
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because it could end up that it's something
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different and there aren't gravitons.
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Um, and, uh, that's why we haven't found
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them, because they're not there. Um,
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it's fascinating. I mean, in a sense,
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uh, gravitons are along the same line as the
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hypothetical dark matter particles. We know,
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um, dark matter is real. We know it's
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there. Uh, we assume it's subatomic
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particles. We've seen some recent works. Uh,
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work. Sorry. We've seen some recent work that
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suggests perhaps they're not, um,
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perhaps it's not subatomic particles, but
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primordial black holes, which can be very
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small and very difficult to detect. Uh, which
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takes us back to the, um, macho
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theory. Massive compact halo objects, the
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macho theory of dark matter, as distinct from
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the WIMP theory, the weakly interacting
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massive particles. I
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think gravitons almost fall into the same
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boat as dark matter particles in the sense
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that we haven't detected them. We hypothesise
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that they're there. We've built constructs
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like virtual gravitons that allow us to do
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that without going completely mad. Um,
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but, uh, at the moment, still, I think,
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uh, the door is wide open for all kinds of
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new ideas that might change our view
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completely.
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Andrew Dunkley: Yeah, I guess the day we crack it will
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go, uh. Yeah, I should have thought of that.
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Professor Fred Watson: Exactly. Well, Alan's already thought of it.
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Andrew Dunkley: Yeah.
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Professor Fred Watson: Yeah. In terms of, you know, what, what the
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conundrums are and why it is. Why it's so
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difficult. Yeah, it's a great question.
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Andrew Dunkley: I guess the question that comes from that is,
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does it have to be a particle? And the answer
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is no. Um, it doesn't, uh, have to be
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just because everything else is made of
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particles. So.
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Professor Fred Watson: Yes, that's right. I mean, it's.
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So what's called the standard model of
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subatomic particles is this
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group of 17 particles which we don't
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think can be broken down into Anything
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smaller. That's why they're called
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fundamental, um, and
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they account. Among them are, uh,
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the force, um, particles,
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um, electromagnetic, strong
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and weak nuclear forces, um,
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uh, which we know about. Gravity is just
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assumed to be, uh, a fundamental force
417
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with its fundamental particle because it
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behaves in every other way. It behaves like
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the other ones do. Uh, but we just haven't
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managed to pinpoint the particle itself.
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There you go.
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Andrew Dunkley: Ah, Alan, you've kind of, um, put
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your thumb on one of the big mysteries of the
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universe and expected us to have an answer.
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Uh, no, it's just
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one of those great big, um, question marks in
427
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space. If you look up, you can see a giant
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question mark in space. That's gravity.
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Professor Fred Watson: That's right, yeah.
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Andrew Dunkley: Uh, whether or not there are gravitons, the
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debate remains. Thank, uh, you, Alan, for the
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question. This is Space Nuts Andrew Dunkley
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here with Professor Fred Watson Watson.
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Professor Fred Watson: I believe that this nation should commit
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Andrew Dunkley: itself to achieving the goal
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before this decade is out, of landing a
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man
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Professor Fred Watson: on the moon and returning him safely to the
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Earth.
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Andrew Dunkley: Beast nuts, Fred Watson.
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Our next question comes from, uh,
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somebody else who's thinking particles. I
443
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spend a lot of time thinking about
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photons and have, uh, so many questions about
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them. Uh, you know, I know
446
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this about Misty because, um, she's always
447
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walking around with a light bulb above her
448
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head. So that explains that,
449
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um, photons are really weird to understand.
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I'm curious to know if there are any
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fundamental particles that do not have a
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wave function. And then is it possible
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to detect a particle or photon that does not
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have any properties of a wave?
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And the last part of the question. Is it
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possible for a photon or particle to have
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such a long wavelength that we don't have a
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detector big enough to pick it up? That's,
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uh, from Misty in Pennsylvania, one of our
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administrators on the Facebook PODC Ask
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Group. So, um, uh, thank you, Misty,
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for sending in a question. Nice to hear from
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you and beautiful part of the world,
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Pennsylvania. Got to drive through that last
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year. And, uh, yeah, it is
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absolutely lovely in summer. Don't
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think I want to be there in winter.
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Nevertheless. Okay, so, um,
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photons. Yeah. What can we talk? What
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can you tell us about? Are there any
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particles that don't have wavelengths? That's
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an interest question.
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Professor Fred Watson: Yes. So that's M, more or less what
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it amounts to. So we see
475
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in quantum mechanics, uh,
476
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we see this fundamental thing that particles,
477
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m, uh, display the properties
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both of a particle and a wave. And so we
479
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call it a wave function. And as
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I understand it, and I Think, uh, quantum
481
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mechanics backs, uh, this up.
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Uh, there are no fundamental particles
483
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that don't have a wave function, so they
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all exhibit this wave particle
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duality.
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Andrew Dunkley: Um,
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Professor Fred Watson: It is, uh,
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I guess, you know, the way that,
489
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um, particle physicists think about
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these things are uh, a little bit different
491
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from the way we might interpret it. So when I
492
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think of the wave particle duality,
493
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my mind immediately goes to the photon,
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um, which, um, Misty's already mentioned.
495
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Uh, yes, we understand
496
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photons as particles because we see the
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photoelectric effect, which insists that
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they've got to be particles because you get
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basically quantized amounts of energy out of
500
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them. But then when I think about the waves,
501
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I think about things like polarisation,
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uh, where you've got waves that are
503
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oscillating in different directions. I think
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we talked about that a couple of episodes
505
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ago, we did, in the mapping of the magnetic
506
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fields of the galaxy of the universe. Um, and
507
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so I always think about waves vibrating
508
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through a median. But,
509
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um, the physicists
510
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kind of combine those two ideas
511
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and, uh, think in terms of, uh, something
512
00:21:45.990 --> 00:21:48.310
it's usually called quantized
513
00:21:48.470 --> 00:21:50.630
excitations of underlying
514
00:21:51.010 --> 00:21:53.090
fields. So
515
00:21:53.570 --> 00:21:56.510
that's to say that, um,
516
00:21:56.610 --> 00:21:59.490
it kind of mixes both relativity and
517
00:21:59.890 --> 00:22:02.610
quantum physics here because the
518
00:22:02.610 --> 00:22:04.850
underlying field is what?
519
00:22:05.530 --> 00:22:08.290
Um, it's the sort of,
520
00:22:08.370 --> 00:22:10.090
if I can put it that way, the background
521
00:22:10.090 --> 00:22:13.010
canvas on which the information
522
00:22:13.330 --> 00:22:16.050
is superimposed and the particle
523
00:22:16.450 --> 00:22:19.170
is a bit of that background canvas that is
524
00:22:19.250 --> 00:22:22.090
excited to vibrate and
525
00:22:22.170 --> 00:22:24.770
give you a wave, but it's
526
00:22:24.770 --> 00:22:27.370
excited in a way that is quantized. That
527
00:22:27.370 --> 00:22:30.210
means there isn't an
528
00:22:30.210 --> 00:22:33.210
infinite number of different excitations
529
00:22:33.290 --> 00:22:34.890
that can be set up.
530
00:22:36.570 --> 00:22:39.450
They're specific numbers,
531
00:22:39.450 --> 00:22:41.770
which means you get specific wavelengths
532
00:22:42.090 --> 00:22:44.930
from the excitation. So it is all a
533
00:22:44.930 --> 00:22:46.660
mix of, of
534
00:22:47.460 --> 00:22:50.340
particles and waves, but it kind of brings
535
00:22:50.340 --> 00:22:52.940
it together and once you think of it in those
536
00:22:52.940 --> 00:22:54.820
terms, uh, then
537
00:22:56.100 --> 00:22:58.140
it becomes clear that you can't have a
538
00:22:58.140 --> 00:23:00.580
particle without its wave function.
539
00:23:00.980 --> 00:23:03.380
Andrew Dunkley: Which kind of writes off her second question.
540
00:23:03.380 --> 00:23:06.140
If there's, um, a long enough wavelength that
541
00:23:06.140 --> 00:23:07.940
we haven't got the equipment to detect it.
542
00:23:08.450 --> 00:23:10.260
Professor Fred Watson: Um, no, I don't think it does
543
00:23:11.380 --> 00:23:13.910
because I think, um,
544
00:23:14.970 --> 00:23:17.970
I mean we, you know, we. In, in
545
00:23:17.970 --> 00:23:20.410
a way the ultra low
546
00:23:20.410 --> 00:23:23.050
frequency radio waves are a bit like that,
547
00:23:23.730 --> 00:23:26.090
uh, because they are,
548
00:23:27.210 --> 00:23:29.009
uh. Some of them have got a wavelength bigger
549
00:23:29.009 --> 00:23:31.890
than the Earth. And
550
00:23:31.890 --> 00:23:34.050
so how do you detect that? Well, you've got
551
00:23:34.050 --> 00:23:36.090
to have a spacecraft that's got the other end
552
00:23:36.090 --> 00:23:38.850
of the aerial on it, you know, that sort of
553
00:23:38.850 --> 00:23:41.130
thing. Um, there's also,
554
00:23:42.530 --> 00:23:45.450
uh. What was I going to say,
555
00:23:45.630 --> 00:23:48.290
um, yeah, we know that there are
556
00:23:48.290 --> 00:23:50.970
gravitational waves that have got
557
00:23:51.290 --> 00:23:54.080
wavelengths measured in light years. Uh,
558
00:23:54.410 --> 00:23:56.650
I think the gravitational
559
00:23:57.690 --> 00:24:00.450
properties of the Big Bang. So the
560
00:24:00.450 --> 00:24:02.290
gravitational waves that were set up by the
561
00:24:02.290 --> 00:24:05.210
Big Bang are extremely long
562
00:24:05.290 --> 00:24:07.370
wavelength. I think I've got that the right
563
00:24:07.370 --> 00:24:10.000
way around. Um,
564
00:24:10.080 --> 00:24:12.840
it's so, uh. And we, you know, there are
565
00:24:12.840 --> 00:24:15.760
ones that we don't have normal,
566
00:24:16.160 --> 00:24:18.720
everyday ways of detecting them. There are
567
00:24:18.720 --> 00:24:20.520
subtleties because you expect some of these
568
00:24:20.520 --> 00:24:22.720
waves to be polarised. And that, I think,
569
00:24:22.720 --> 00:24:24.999
gives you an insight into it. But, yeah,
570
00:24:24.999 --> 00:24:27.920
it's, uh. Look, it is a good question.
571
00:24:28.600 --> 00:24:31.400
Uh, and I, uh, think, um, once again,
572
00:24:31.400 --> 00:24:34.360
mist is thinking outside the box. Uh,
573
00:24:34.360 --> 00:24:36.960
no particles without their wave
574
00:24:36.960 --> 00:24:39.480
function, because a particle is an
575
00:24:39.480 --> 00:24:42.260
excitation of the underlying field, a
576
00:24:42.260 --> 00:24:44.540
quantized excitation of the underlying field.
577
00:24:45.020 --> 00:24:47.740
Andrew Dunkley: So it is possible we cannot detect certain
578
00:24:47.740 --> 00:24:49.620
wavelengths because they're too big, but they
579
00:24:49.620 --> 00:24:50.300
still exist.
580
00:24:50.540 --> 00:24:51.780
Professor Fred Watson: I think that's right, yes.
581
00:24:51.780 --> 00:24:54.060
Andrew Dunkley: Yeah. All right. What about gravitons? Do you
582
00:24:54.060 --> 00:24:55.380
reckon they have a wavelength?
583
00:24:55.380 --> 00:24:57.700
Professor Fred Watson: Well, yes, they do. That's the thing. Um, if
584
00:24:57.700 --> 00:24:59.630
they exist, yes. Uh, because, um,
585
00:25:01.030 --> 00:25:03.980
uh, we've got gravitational waves. So the
586
00:25:03.980 --> 00:25:06.100
wave particle duality works both ways. If
587
00:25:06.100 --> 00:25:07.580
you've got a wave, you've got a particle.
588
00:25:07.900 --> 00:25:10.780
Andrew Dunkley: There you go. Uh, good one. Thanks,
589
00:25:10.780 --> 00:25:13.220
Misty. Hope all is well in Pennsylvania.
590
00:25:16.100 --> 00:25:18.420
Three, two, one.
591
00:25:18.980 --> 00:25:20.260
Professor Fred Watson: Space nuts.
592
00:25:20.500 --> 00:25:23.380
Andrew Dunkley: And our final question, uh, comes from
593
00:25:23.380 --> 00:25:25.380
another one of our regular contributors,
594
00:25:25.380 --> 00:25:28.140
Casey in Colorado. What does it feel
595
00:25:28.140 --> 00:25:30.740
like to go from weightlessness to normal
596
00:25:30.740 --> 00:25:33.060
gravity for astronauts when returning to
597
00:25:33.060 --> 00:25:36.030
Earth? I think it would depend
598
00:25:36.030 --> 00:25:38.940
on how long you've been up there and, uh,
599
00:25:38.940 --> 00:25:40.470
whether or not you've actually bothered to
600
00:25:40.470 --> 00:25:41.470
use the treadmill.
601
00:25:43.230 --> 00:25:45.030
Professor Fred Watson: Well, that's right. The treadmill is all
602
00:25:45.030 --> 00:25:46.750
about keeping up your muscle strength.
603
00:25:46.910 --> 00:25:49.070
Andrew Dunkley: Exactly. Um, because once you're out there,
604
00:25:49.310 --> 00:25:51.900
your muscles immediately start to wither. Uh,
605
00:25:52.390 --> 00:25:52.910
they do.
606
00:25:52.910 --> 00:25:55.390
Professor Fred Watson: And you don't really have anything against
607
00:25:55.390 --> 00:25:58.230
which to push to keep them,
608
00:25:58.230 --> 00:26:00.060
you know, keep them going, other than the.
609
00:26:00.530 --> 00:26:02.450
The, um, torture equipment that
610
00:26:03.490 --> 00:26:06.010
NASA and Roscosmos provide on their space
611
00:26:06.010 --> 00:26:06.530
station.
612
00:26:06.530 --> 00:26:08.890
Andrew Dunkley: I think on Space Lab, they didn't have a
613
00:26:08.890 --> 00:26:10.850
treadmill. They had a running track that ran
614
00:26:10.850 --> 00:26:13.810
around the inside of
615
00:26:14.850 --> 00:26:17.850
wall of, uh, Skylab, I think. And
616
00:26:17.850 --> 00:26:20.690
so I've seen footage of astronauts actually
617
00:26:20.690 --> 00:26:23.090
running in a circle around the
618
00:26:23.410 --> 00:26:25.250
interior of Skylab.
619
00:26:25.570 --> 00:26:28.250
Professor Fred Watson: So they're keeping themselves, um, running
620
00:26:28.250 --> 00:26:30.290
just by the centrifugal force that they're
621
00:26:30.370 --> 00:26:32.990
setting up. Yeah, yeah, yeah. That's
622
00:26:32.990 --> 00:26:34.570
interesting. I didn't know that. That's, uh.
623
00:26:34.630 --> 00:26:37.270
Andrew Dunkley: Yeah, I'm sure that if you had online, you'd
624
00:26:37.270 --> 00:26:40.030
find Footage of it. I. I strongly remember
625
00:26:40.030 --> 00:26:42.430
that M. I saw it on the news one day and
626
00:26:42.430 --> 00:26:44.510
thought, wow, how did they do that? Well,
627
00:26:44.510 --> 00:26:45.620
there's no gravity, duh. Uh,
628
00:26:47.470 --> 00:26:49.230
Professor Fred Watson: yeah. Um,
629
00:26:50.350 --> 00:26:53.350
wasn't there something like that in 2001 A
630
00:26:53.350 --> 00:26:55.070
Space Odyssey? I think there was. Could have
631
00:26:55.070 --> 00:26:55.270
been.
632
00:26:55.270 --> 00:26:58.030
Andrew Dunkley: I think I watched that very recently.
633
00:26:58.110 --> 00:27:00.150
I just thought I really wanted to watch it
634
00:27:00.150 --> 00:27:02.500
again. But, um, I fell asleep. But
635
00:27:02.980 --> 00:27:04.860
it's very late. Judy had gone to bed, and I
636
00:27:04.860 --> 00:27:07.730
thought, oh, I might just start this. Uh,
637
00:27:07.730 --> 00:27:08.900
yeah, I was gone.
638
00:27:11.420 --> 00:27:13.860
Um, what was the question? Oh, uh, what's the
639
00:27:13.940 --> 00:27:16.620
feel like? I also remember seeing
640
00:27:16.620 --> 00:27:19.460
footage of cosmonauts, uh, coming back
641
00:27:19.460 --> 00:27:22.180
from very long haul time in space.
642
00:27:23.220 --> 00:27:25.580
And they'd get them out of the capsule once
643
00:27:25.580 --> 00:27:27.420
they came back to Earth and they couldn't
644
00:27:27.420 --> 00:27:27.820
stand up.
645
00:27:27.820 --> 00:27:29.740
Professor Fred Watson: Couldn't stand up. Yeah. I've seen similar
646
00:27:29.740 --> 00:27:32.740
things and. Well, you know, even with the
647
00:27:32.740 --> 00:27:34.960
exercise that the Artemis II crew
648
00:27:35.520 --> 00:27:38.240
were doing, they were a little bit wobbly
649
00:27:38.320 --> 00:27:40.920
when they got out of the spacecraft. And we
650
00:27:40.920 --> 00:27:43.920
all saw them going across the deck of the,
651
00:27:44.280 --> 00:27:46.820
uh, recovery ship. Uh,
652
00:27:47.280 --> 00:27:49.239
so I think how wobbly you are probably
653
00:27:49.239 --> 00:27:51.120
depends on just how much effort you've put
654
00:27:51.120 --> 00:27:53.720
into keeping up your muscle strength. So I
655
00:27:53.720 --> 00:27:56.480
think that's the key thing that Casey
656
00:27:57.360 --> 00:28:00.280
might be thinking of. Um, exactly. As
657
00:28:00.280 --> 00:28:02.600
you've said, your muscles go to waste very
658
00:28:02.600 --> 00:28:05.100
quickly. Uh, and if you. You don't
659
00:28:05.100 --> 00:28:06.740
exercise, then you're going to be in big
660
00:28:06.740 --> 00:28:08.780
trouble. You simply would not be able to
661
00:28:08.780 --> 00:28:11.700
walk. Um, so quite a
662
00:28:11.700 --> 00:28:14.140
significant, uh, thing. Ah. Which would also,
663
00:28:14.140 --> 00:28:16.180
of course, depend on how long you've been in
664
00:28:16.180 --> 00:28:17.580
space, how long you've been weightless.
665
00:28:17.820 --> 00:28:20.259
Andrew Dunkley: And the other thing they might suffer from is
666
00:28:20.259 --> 00:28:23.100
fatigue because they have
667
00:28:23.100 --> 00:28:26.060
to work so much harder to achieve the same
668
00:28:26.940 --> 00:28:29.180
mobility as they were used to. When they had
669
00:28:29.180 --> 00:28:32.120
full muscle strength, they'd get
670
00:28:32.120 --> 00:28:34.600
very tired very fast. I think,
671
00:28:35.560 --> 00:28:37.560
all jokes aside, I think the,
672
00:28:38.130 --> 00:28:39.880
um, everyday person,
673
00:28:41.300 --> 00:28:43.340
uh, who's been through, um,
674
00:28:43.480 --> 00:28:46.200
immunotherapy or some
675
00:28:46.200 --> 00:28:49.120
form of, um, um, um,
676
00:28:49.400 --> 00:28:51.620
inhibitor for, um,
677
00:28:53.080 --> 00:28:56.080
testosterone, for example, for cancer
678
00:28:56.080 --> 00:28:58.990
treatment or something like that, that
679
00:28:58.990 --> 00:29:01.110
has the same effect on your muscles. Muscle
680
00:29:01.110 --> 00:29:03.550
wastage. When you stop producing testosterone
681
00:29:04.510 --> 00:29:06.590
as a male, your muscles
682
00:29:07.550 --> 00:29:09.350
actually do fade away. And you've got to do
683
00:29:09.350 --> 00:29:12.270
exercise to keep. Like astronauts, you've got
684
00:29:12.270 --> 00:29:14.190
to keep your exercise up to keep your muscles
685
00:29:14.190 --> 00:29:17.070
in trim, but it
686
00:29:17.070 --> 00:29:20.030
does slow you down. Um, and case in
687
00:29:20.030 --> 00:29:22.230
point, I did have that sort of treatment for
688
00:29:22.230 --> 00:29:24.590
my prostate cancer. And for six months
689
00:29:25.660 --> 00:29:28.180
I went into basically the
690
00:29:28.180 --> 00:29:30.460
equivalent to menopause. I had muscle
691
00:29:30.460 --> 00:29:32.980
wastage. Um, I kept up my
692
00:29:32.980 --> 00:29:35.740
exercise, but it wasn't enough. And I
693
00:29:35.980 --> 00:29:38.060
had a situation where I'd go out and play
694
00:29:38.060 --> 00:29:40.899
golf. I lost 40 yards on
695
00:29:40.899 --> 00:29:43.460
shots simply because my muscles had wasted
696
00:29:43.460 --> 00:29:46.180
away. And it's probably taken a year to get
697
00:29:46.180 --> 00:29:46.780
it all back.
698
00:29:47.100 --> 00:29:47.740
Professor Fred Watson: Yeah, interesting.
699
00:29:48.620 --> 00:29:51.580
Andrew Dunkley: Yeah. Um, it would be the same effect for an
700
00:29:51.580 --> 00:29:53.780
astronaut on it. Exactly the same. Different,
701
00:29:53.860 --> 00:29:56.100
different, you know, different mechanism.
702
00:29:56.180 --> 00:29:58.100
Mechanism, but same effect.
703
00:29:59.010 --> 00:30:01.900
Um, and. And yet the
704
00:30:01.900 --> 00:30:03.500
other thing that they'd probably have to deal
705
00:30:03.500 --> 00:30:05.140
with is some, some of them have very
706
00:30:05.700 --> 00:30:08.660
significant health effects from, from
707
00:30:08.660 --> 00:30:10.700
being in zero G and you come back to Earth.
708
00:30:10.700 --> 00:30:13.620
Like we had a, um, didn't. Wasn't there an
709
00:30:13.620 --> 00:30:15.700
astronaut recently who was temporarily
710
00:30:15.700 --> 00:30:18.500
blinded from,
711
00:30:18.500 --> 00:30:21.260
from zero G? And there's all sorts of
712
00:30:21.260 --> 00:30:24.260
things that um, they can suffer from. And
713
00:30:24.660 --> 00:30:26.140
a lot of the time when they come back to
714
00:30:26.140 --> 00:30:28.540
Earth, it does fix itself because you're back
715
00:30:28.540 --> 00:30:31.340
in your normal environment. But when you're
716
00:30:31.340 --> 00:30:33.420
out there orbiting or going to the moon and
717
00:30:33.420 --> 00:30:36.100
back, it is not a human environment.
718
00:30:36.980 --> 00:30:39.500
Professor Fred Watson: That's not normal. Yeah, so it was an
719
00:30:39.500 --> 00:30:42.100
evacuation the uh, beginning of the year, I
720
00:30:42.100 --> 00:30:44.060
think it was, that we only really found out a
721
00:30:44.060 --> 00:30:46.900
few snippets about not very long ago.
722
00:30:47.780 --> 00:30:49.700
And I can't remember what the details were
723
00:30:50.260 --> 00:30:52.480
because my brain's atrophy because of
724
00:30:54.720 --> 00:30:55.440
old age.
725
00:30:56.320 --> 00:30:59.320
Andrew Dunkley: Yes, indeed. But, uh, there
726
00:30:59.320 --> 00:31:02.030
would be various levels of, um,
727
00:31:02.030 --> 00:31:04.320
dysfunction as a consequence of spending time
728
00:31:04.320 --> 00:31:07.280
in space. It would be a
729
00:31:07.840 --> 00:31:10.480
person to person variable.
730
00:31:10.790 --> 00:31:13.480
Um, it's not a one size
731
00:31:13.480 --> 00:31:15.800
fits all situation. Some people who'd come
732
00:31:15.800 --> 00:31:18.600
back probably not feel anything. But if, um,
733
00:31:18.800 --> 00:31:20.840
if you're up there long enough. Yeah, it's
734
00:31:20.840 --> 00:31:22.400
going to have a big impact on you.
735
00:31:22.400 --> 00:31:23.440
Professor Fred Watson: Yes, indeed.
736
00:31:24.240 --> 00:31:26.400
Andrew Dunkley: Thank you so much for the question, Kasey. I
737
00:31:26.400 --> 00:31:29.120
hope we covered it
738
00:31:29.360 --> 00:31:32.240
reasonably well. Um, anyway,
739
00:31:32.290 --> 00:31:34.960
uh, in the not too distant future, I'm pretty
740
00:31:34.960 --> 00:31:36.600
sure there'll be so many people going in and
741
00:31:36.600 --> 00:31:38.600
out of space, they'll come up with ways of
742
00:31:38.600 --> 00:31:41.520
dealing with it. Who knows? And
743
00:31:41.520 --> 00:31:42.960
I think that brings us to the end.
744
00:31:42.960 --> 00:31:44.720
Don't forget, if you've got, uh, questions
745
00:31:44.720 --> 00:31:47.360
for us or observations or comments or
746
00:31:47.360 --> 00:31:49.200
whatever you like, you can go to our website,
747
00:31:49.820 --> 00:31:51.940
send it to us in a text or audio
748
00:31:51.940 --> 00:31:53.344
format@spacenuts
749
00:31:53.656 --> 00:31:55.300
IO or
750
00:31:55.300 --> 00:31:58.060
spacenutspodcast.com
751
00:31:58.460 --> 00:32:01.220
and just click on the little ama button at
752
00:32:01.220 --> 00:32:04.060
the top that stands for Ask me Anything. And
753
00:32:04.930 --> 00:32:07.420
um, you can send it through. Don't forget to
754
00:32:07.500 --> 00:32:09.980
tell us who you are or where you're from.
755
00:32:11.420 --> 00:32:13.140
And Fred Watson, that's it. Thanks so much
756
00:32:13.140 --> 00:32:15.500
for answering those. That was a tough batch
757
00:32:15.500 --> 00:32:15.820
today.
758
00:32:17.500 --> 00:32:19.380
Professor Fred Watson: Great questions though. Well done. To all our
759
00:32:19.380 --> 00:32:22.200
listeners for what they do in terms
760
00:32:22.200 --> 00:32:24.520
of, uh, thinking through a lot of these
761
00:32:24.520 --> 00:32:25.480
issues. It's great.
762
00:32:25.960 --> 00:32:27.520
Andrew Dunkley: Very good. All right, we'll catch you real
763
00:32:27.520 --> 00:32:28.640
soon. Fred Watson, thanks so much.
764
00:32:28.640 --> 00:32:30.040
Professor Fred Watson: Looking forward to it. Thanks, Andrew.
765
00:32:30.200 --> 00:32:32.000
Andrew Dunkley: Professor Fred Watson Watson, astronomer at
766
00:32:32.000 --> 00:32:34.240
large. And thanks to Huw in the studio, who
767
00:32:34.240 --> 00:32:35.980
couldn't be with us today because, um,
768
00:32:36.920 --> 00:32:39.560
there was, um, so much going on with
769
00:32:39.560 --> 00:32:41.960
gravitons and weightlessness, he just
770
00:32:42.360 --> 00:32:45.120
decided to float away. And from me,
771
00:32:45.120 --> 00:32:46.440
Andrew Dunkley. Thanks for your company.
772
00:32:46.440 --> 00:32:47.840
We'll catch you on the next episode of
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SpaceNuts real soon.
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Professor Fred Watson: Soon.
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Andrew Dunkley: Bye. Bye. You've been listening
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to the Space Nuts podcast,
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available at Apple Podcasts, Spotify,
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00:32:58.220 --> 00:33:00.980
iHeartRadio or your favourite podcast
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player. You can also stream on
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00:33:02.700 --> 00:33:04.380
demand@bytes.com.
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00:33:04.700 --> 00:33:06.780
Professor Fred Watson: this has been another quality podcast
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production from bytes.com.
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Andrew Dunkley: Hello again. Thanks for joining us. This is a
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Q and A edition of Space Nuts. We talk
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astronomy, space science, and answer
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audience questions. Well, maybe we won't do
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one of those three things today. I don't
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know. We'll see how it goes. Uh, we've got a
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lot of questions to get through today. Um,
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Fred Watson reckons some of these are very,
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very tricky, so we'll see how it all pans
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out. Um, a question about the expanding
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universe. Never had one of those before. Uh,
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a question about gravitons. Never had one of
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those before. Yes, we have. Uh, photons
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and weight shift. That's all coming up on
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this edition of space nuts. 15
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seconds.
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Professor Fred Watson: Guidance is internal. 10,
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9. Ignition sequence start.
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Space nuts. 5, 4, 3. 2. 1, 2,
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3, 4, 5, 5, 4, 3, 2, 1.
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Andrew Dunkley: Space nuts. Astronauts report it feels
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good. And joining us once more to
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unravel all of that, or maybe ravel it
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up even more, is Professor Fred Watson
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Watson, astronomer at, uh, large. Hello,
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Fred Watson.
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Professor Fred Watson: Hello, Andrew. I do feel pretty ravelled at
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the moment.
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Andrew Dunkley: Yeah, look, we have got some tricky
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questions, but before we get to those, uh,
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we've received a note from Rennie in
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California.
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Uh, Rennie quite regularly sends questions
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into us, but he sent us a really lovely note
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which I want to share. Uh, he says no
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questions today, just to thank you. I try to
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absorb as much information as I can listening
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to your podcast. And when I'm engaged in a
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convers conversation with my two grandsons
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aged 15 and 12, I try to excite
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them and get them to think about our place in
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the universe and how it behaves. Now it's
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paying off with the announcement that my
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older grandson wants to carry on in college
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with some form of education in astronomy
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or particle physics. Thank you for paying
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it forward, Renny. Isn't that lovely?
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Professor Fred Watson: Yeah, that's great. Absolutely great.
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Andrew Dunkley: Uh, I love it when we get feedback from
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people that, that become inspired
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despite us.
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No, I mean, it's fantastic.
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Professor Fred Watson: It is.
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Andrew Dunkley: I'm really, really pleased. Really pleased.
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So, um, pass on our regards, Rennie, to your
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boys or, uh, your grandsons, um, and wish
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them well and. Yeah, look, just.
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I do the same thing with my grandson and
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three granddaughters. Um, I talk to them
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whenever there's something interesting to
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talk about, and there usually is, uh, in the
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astronomical world. And, um, I show
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them the images I take with the Telesco, and
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I've even had them outside looking up at the
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moon. And, um, yeah, it's captivating. Once,
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once they, you know, once you can convince
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them to actually get outside.
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Um, you know, the universe is their
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oyster. It's, uh, it's good
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stuff. So lovely to hear from you, Rennie.
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And that is really fabulous news.
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Are you ready for your first question,
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Fred Watson?
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Professor Fred Watson: Well, after a. Yes. After a build up like
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that, I guess we've got to tackle them,
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haven't we?
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Andrew Dunkley: Uh, we probably should.
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Professor Fred Watson: You're right, in a way. You know, the
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ultimate notes, I guess,
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is to provide that little bit of perhaps
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inspiration that might lead people to do
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things that might one day change the world.
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Who knows?
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Andrew Dunkley: Yep, you just don't know. You just don't
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know. Maybe that's our lot in life is to just
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try to inspire, uh, just a handful of people
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to pick up the baton, Fred Watson. Who knows?
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All right, question one. It's like a test,
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isn't it?
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Question one. Uh, if space is
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expanding faster than the speed of light,
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then in millions or billions of years from
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now, will our night sky be completely black
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or a completely black void? Um,
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uh, or completely black, devoid of
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all light except our local solar system. That
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comes from Clint. Uh, this is
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something that has come up occasionally and I
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think even in one of our most recent
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episodes, we were talking about the expansion
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of the universe and its significance. And,
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and I think in our Q and A episode, someone
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asked about the expansion of the universe.
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Um, so here it is again.
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Um, we are, ah,
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expanding, and it's
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expanding at an accelerating rate. Although
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it's debatable whether or not that
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acceleration is actually as m. Significant
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as it was. That is a
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separate debate. Um, but I think it's pretty
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clear that in the long distant future
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of this universe, it will become a black
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void, won't it?
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Professor Fred Watson: Uh, yes. So the answer to Clint's question
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is yes.
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Andrew Dunkley: Okay, question
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Professor Fred Watson: no. Exactly. As you said, um,
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if you've got, um. So
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when you say the universe is expanding more
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than the speed of light, you've got to be a
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bit specific because really what you're
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talking about is objects within
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the universe which are being carried along by
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the expansion of the universe. And so,
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uh, there will be, at a certain
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distance from us now,
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objects whose, what we call the recession
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velocity is faster than the speed of light,
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but they're actually, they're beyond
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the wall that we can't see beyond anyway,
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which is the cosmic microwave background
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radiation. But you can imagine as the
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expansion continues to accelerate, and you're
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right, it is still thought to be
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accelerating. We just don't quite know
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whether that acceleration is a constant.
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That's the thing you were alluding
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to because there's some evidence that
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maybe the acceleration is reducing,
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but nevertheless it's still accelerating. So
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it's still getting bigger, faster, uh, all
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the time. And so what that would do,
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um, you can, you can sort of
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imagine in your head what this situation
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would lead to. It means that the,
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the, the sort of black horizon, the horizon
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which is where light can never get to you
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because it's being carried away. The objects
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are being carried away faster than the speed
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of light. That black horizon will, will
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approach, um, it'll get nearer
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as the universe's expansion continues to
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accelerate. So eventually you can imagine
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that maybe you would see just
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the other galaxies in the Local Group, uh,
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which is Andromeda and the, uh, triangular
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whirlpool galaxy and things like that. But
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eventually, yeah, it might just be
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objects in our own solar system, uh,
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which makes astronomy a little bit of a.
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Boring. Yeah.
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Yeah.
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Andrew Dunkley: Well, let's go see what we can find. Oh,
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there's the moon.
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Professor Fred Watson: Yeah. Yeah. Oh, wait, it's gone.
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Andrew Dunkley: Well, it's moving away from us too.
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Professor Fred Watson: So it is rather slower than the speed of
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light. Yeah. Six centimetres a year.
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Andrew Dunkley: I can't imagine this is going to happen in an
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awful hurry, Fred Watson.
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Professor Fred Watson: No, it's not. It's very, very long way down
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the track. And of course, from our
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perspective here on, ah, Earth, long, uh,
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before anything like that takes place,
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um, we'll have been
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confronted by the expansion of the sun
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itself, um, as it turns into
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a red giant star.
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Andrew Dunkley: Yeah. Who knows where we'll be in the
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universe by then. We might have moved out
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into other parts of the galaxy by then if
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we've managed, um, to find some kind of
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propulsion system or learn how to fold
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space or whatever it is you need to do. Uh,
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maybe develop wormholes and be able
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to travel mega distances.
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Professor Fred Watson: Yeah. Fast. You're the person, you're the
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science fiction writer. You've got to tell us
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what it is we're going to do.
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Andrew Dunkley: Uh, I'm working, um, uh, on
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warp, uh, warp travel at the moment.
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Professor Fred Watson: Oh, good.
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Andrew Dunkley: In m. My. In my novels. So,
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yeah, I'm doing the final editing at this
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stage and it's, uh, it's the most horrible
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job.
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Professor Fred Watson: It is, isn't it? Yeah.
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Andrew Dunkley: Especially writing's fun.
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Professor Fred Watson: Yeah.
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Andrew Dunkley: But then you've got to fix all your blunders
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and you don't realise how really hopeless you
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are until you have
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Professor Fred Watson: to edit your own stuff.
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Andrew Dunkley: Yeah, yeah. I'd pay someone, but I can't
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afford it. It's not a, it's not a cheap
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thing to get Done book editing. Um,
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but anyway, uh, so the basic
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answer to Clint's question is yes, it's going
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to happen. Uh, there will be complete black
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nothingness, um,
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in a matter of about three weeks time, or
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could be three gazillion years time.
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Professor Fred Watson: I think the latter's more likely.
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Andrew Dunkley: More likely the latter. Thank you, Clint.
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Great to hear from you.
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Our next question comes from
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somebody whose name I forgot to write down.
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Uh, no, it didn't. It comes from, uh, Alan.
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Now, this is a pretty big question, so I'll
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just go straight through it and we can figure
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all out the rest out later. Uh, I know you
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want audio questions, but you know how they
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say you have a face made for radio? I've got
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one of those. Well, uh, I have a voice made
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for text. That's very
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good. I, um, hope it's not true. Uh, I
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discovered space nuts more than a year ago
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and have listened to your entire back
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catalogue.
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Professor Fred Watson: Wow.
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Andrew Dunkley: Wow. Get a job. No. Fantastic. Thank
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you. Uh, still listening and have not lost my
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mind yet.
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Professor Fred Watson: Wow.
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Andrew Dunkley: That's a record.
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Uh, here's something that's been bothering me
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for, uh, some months. Some physicists
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don't believe relativity, uh, when it says
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that gravity is not a force. Also, they
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believe that all forces are conveyed by
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particles. To unify gravity with other
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forces, they postulate the graviton to be
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that particle for gravity. It's said that
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nothing escapes a black hole, but actually
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gravity does. If gravitons exist
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and convey the force of gravity, then they
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escape black holes. So they are not affected
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by gravity. That means they do not affect
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each other. We know gravity does affect all
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massive particles and photons, massless
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particles that convey the electromagnetic
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force. I don't know if gravitons affect other
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massless particles. This is the interesting
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part. If f equals gm 1 m
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2 divided by d squared is
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the complete calculation for the force
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of gravity, no modifications introduced by
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relativity or quantum physics, then gravitons
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are not affected by anything. So gravitons
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affect every particle except gravitons and
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are not affected by anything. So is
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an asymmetry that breaks
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conservation, uh, of energy and momentum. My
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question is. Here it is. Why do some
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physicists still believe in
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gravitons? That comes from Alan in San
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Antonio, Texas. Boy, Alan, you've put a lot
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of thought into that. You really have.
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Professor Fred Watson: Yeah. And these are questions that are right
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on money as well. Yeah. Uh, especially the
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last one. Why do physicists believe in
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gravitons? I think most physicists probably
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do. Uh, Alan, because
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um, we know that gravity is a fundamental
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force and all the other fundamental forces
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have their subatomic particles,
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uh, which are basically
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um, um,
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particles that can. That sort of what we
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call, we call them bosons. They're what, they
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carry a field in a way. And the field is
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another way of looking at how a uh,
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force works. I didn't
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phrase that very well, but uh, that's why
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some physicists believe in gravitons. We've
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never found them. We don't have a particle
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physics theory of gravity. Uh, so we don't
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know that they exist. But I think most
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physicists would assume that they exist.
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And so uh, that
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first um, conundrum
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that you mentioned,
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if nothing escapes a black hole, well,
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gravity does. And so if
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gravitons exist and convey the force of
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gravity, then they escape black holes. So
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they're not affected by gravity. That means
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they do not affect each other. But in
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fact, um, uh,
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the bottom line with black holes it's
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quite complicated. Uh, but you
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don't have gravitons escaping
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from the black hole. Uh,
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the way people who know a lot more about
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these things than me, uh, the way they
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envisage this is that the gravitational
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field of the black hole is a kind
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of fossilised one that was
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established before the collapse
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into uh, a black hole.
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Or, and here's another way of looking at it.
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This really, you're gonna think, um, Alan,
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this is a cop out, but this is the way the
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physicists see it. Uh, the,
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the gravitational field of black hole
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basically uh, includes
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something called virtual gravitons.
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Uh, and so that sort of ties in with the fact
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that the, the gravitational field is a
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fossilised footprint, if I can put it that
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way. Um, the
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virtual gravitons, uh, are an
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embodiment of that, but they don't
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necessarily obey the
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normal laws of physics.
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So
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uh,
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basically what you've got here, and
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I think, um, the
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physicists who look at this problem probably
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just automatically drop into the two
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camps of relativist people who
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are ah, experts in general relativity. That's
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Einstein's theory of gravity that says, yes,
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um, gravity is not a force, it's just a
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distortion of space. Uh, and the quantum
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mechanics people who look at it from the
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perspective of gravitons.
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Um, and so yeah, the virtual particles,
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uh, the quantum mechanics
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person's answer to this,
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uh, they're basically
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just mathematical constructs, uh, in a
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quantum field. And so they don't have to
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obey speed limits or anything like that, or
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even don't have to worry about the event
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horizon so they can continually
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basically, uh, keep the gravitational force
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there without actually being
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trapped by it. I think that's the way
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physicists look at it.
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Andrew Dunkley: Uh, all that says to me is
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something. It's still a big mystery. There
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are so many different theories behind
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gravity, and we really don't know what it is.
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We know what it is, but we don't know why it
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is.
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Professor Fred Watson: Well, no. So all we know about
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gravity is the way it behaves. Um,
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we really don't know what it is. And in a
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way, Alan's question is well posed
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because it could end up that it's something
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different and there aren't gravitons.
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Um, and, uh, that's why we haven't found
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them, because they're not there. Um,
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it's fascinating. I mean, in a sense,
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uh, gravitons are along the same line as the
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hypothetical dark matter particles. We know,
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um, dark matter is real. We know it's
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there. Uh, we assume it's subatomic
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particles. We've seen some recent works. Uh,
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work. Sorry. We've seen some recent work that
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suggests perhaps they're not, um,
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perhaps it's not subatomic particles, but
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primordial black holes, which can be very
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small and very difficult to detect. Uh, which
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takes us back to the, um, macho
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theory. Massive compact halo objects, the
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macho theory of dark matter, as distinct from
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the WIMP theory, the weakly interacting
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massive particles. I
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think gravitons almost fall into the same
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boat as dark matter particles in the sense
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that we haven't detected them. We hypothesise
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that they're there. We've built constructs
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like virtual gravitons that allow us to do
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that without going completely mad. Um,
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but, uh, at the moment, still, I think,
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uh, the door is wide open for all kinds of
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new ideas that might change our view
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completely.
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Andrew Dunkley: Yeah, I guess the day we crack it will
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go, uh. Yeah, I should have thought of that.
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Professor Fred Watson: Exactly. Well, Alan's already thought of it.
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Andrew Dunkley: Yeah.
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Professor Fred Watson: Yeah. In terms of, you know, what, what the
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conundrums are and why it is. Why it's so
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difficult. Yeah, it's a great question.
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Andrew Dunkley: I guess the question that comes from that is,
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does it have to be a particle? And the answer
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is no. Um, it doesn't, uh, have to be
402
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just because everything else is made of
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particles. So.
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Professor Fred Watson: Yes, that's right. I mean, it's.
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So what's called the standard model of
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subatomic particles is this
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group of 17 particles which we don't
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think can be broken down into Anything
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smaller. That's why they're called
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fundamental, um, and
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they account. Among them are, uh,
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the force, um, particles,
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um, electromagnetic, strong
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and weak nuclear forces, um,
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uh, which we know about. Gravity is just
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assumed to be, uh, a fundamental force
417
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with its fundamental particle because it
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behaves in every other way. It behaves like
419
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the other ones do. Uh, but we just haven't
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managed to pinpoint the particle itself.
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There you go.
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Andrew Dunkley: Ah, Alan, you've kind of, um, put
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your thumb on one of the big mysteries of the
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universe and expected us to have an answer.
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Uh, no, it's just
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one of those great big, um, question marks in
427
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space. If you look up, you can see a giant
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question mark in space. That's gravity.
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Professor Fred Watson: That's right, yeah.
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Andrew Dunkley: Uh, whether or not there are gravitons, the
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debate remains. Thank, uh, you, Alan, for the
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question. This is Space Nuts Andrew Dunkley
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00:18:14.210 --> 00:18:16.290
here with Professor Fred Watson Watson.
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Professor Fred Watson: I believe that this nation should commit
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Andrew Dunkley: itself to achieving the goal
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before this decade is out, of landing a
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man
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Professor Fred Watson: on the moon and returning him safely to the
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Earth.
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Andrew Dunkley: Beast nuts, Fred Watson.
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Our next question comes from, uh,
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somebody else who's thinking particles. I
443
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spend a lot of time thinking about
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photons and have, uh, so many questions about
445
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them. Uh, you know, I know
446
00:18:44.370 --> 00:18:46.770
this about Misty because, um, she's always
447
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walking around with a light bulb above her
448
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head. So that explains that,
449
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um, photons are really weird to understand.
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I'm curious to know if there are any
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fundamental particles that do not have a
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wave function. And then is it possible
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to detect a particle or photon that does not
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have any properties of a wave?
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And the last part of the question. Is it
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possible for a photon or particle to have
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such a long wavelength that we don't have a
458
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detector big enough to pick it up? That's,
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uh, from Misty in Pennsylvania, one of our
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administrators on the Facebook PODC Ask
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Group. So, um, uh, thank you, Misty,
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for sending in a question. Nice to hear from
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you and beautiful part of the world,
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Pennsylvania. Got to drive through that last
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year. And, uh, yeah, it is
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absolutely lovely in summer. Don't
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think I want to be there in winter.
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Nevertheless. Okay, so, um,
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photons. Yeah. What can we talk? What
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can you tell us about? Are there any
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particles that don't have wavelengths? That's
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an interest question.
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Professor Fred Watson: Yes. So that's M, more or less what
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it amounts to. So we see
475
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in quantum mechanics, uh,
476
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we see this fundamental thing that particles,
477
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m, uh, display the properties
478
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both of a particle and a wave. And so we
479
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call it a wave function. And as
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I understand it, and I Think, uh, quantum
481
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mechanics backs, uh, this up.
482
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Uh, there are no fundamental particles
483
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that don't have a wave function, so they
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all exhibit this wave particle
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duality.
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Andrew Dunkley: Um,
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Professor Fred Watson: It is, uh,
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I guess, you know, the way that,
489
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um, particle physicists think about
490
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these things are uh, a little bit different
491
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from the way we might interpret it. So when I
492
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think of the wave particle duality,
493
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my mind immediately goes to the photon,
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um, which, um, Misty's already mentioned.
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Uh, yes, we understand
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photons as particles because we see the
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photoelectric effect, which insists that
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they've got to be particles because you get
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basically quantized amounts of energy out of
500
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them. But then when I think about the waves,
501
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I think about things like polarisation,
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uh, where you've got waves that are
503
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oscillating in different directions. I think
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we talked about that a couple of episodes
505
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ago, we did, in the mapping of the magnetic
506
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fields of the galaxy of the universe. Um, and
507
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so I always think about waves vibrating
508
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through a median. But,
509
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um, the physicists
510
00:21:38.710 --> 00:21:41.350
kind of combine those two ideas
511
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and, uh, think in terms of, uh, something
512
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it's usually called quantized
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00:21:48.470 --> 00:21:50.630
excitations of underlying
514
00:21:51.010 --> 00:21:53.090
fields. So
515
00:21:53.570 --> 00:21:56.510
that's to say that, um,
516
00:21:56.610 --> 00:21:59.490
it kind of mixes both relativity and
517
00:21:59.890 --> 00:22:02.610
quantum physics here because the
518
00:22:02.610 --> 00:22:04.850
underlying field is what?
519
00:22:05.530 --> 00:22:08.290
Um, it's the sort of,
520
00:22:08.370 --> 00:22:10.090
if I can put it that way, the background
521
00:22:10.090 --> 00:22:13.010
canvas on which the information
522
00:22:13.330 --> 00:22:16.050
is superimposed and the particle
523
00:22:16.450 --> 00:22:19.170
is a bit of that background canvas that is
524
00:22:19.250 --> 00:22:22.090
excited to vibrate and
525
00:22:22.170 --> 00:22:24.770
give you a wave, but it's
526
00:22:24.770 --> 00:22:27.370
excited in a way that is quantized. That
527
00:22:27.370 --> 00:22:30.210
means there isn't an
528
00:22:30.210 --> 00:22:33.210
infinite number of different excitations
529
00:22:33.290 --> 00:22:34.890
that can be set up.
530
00:22:36.570 --> 00:22:39.450
They're specific numbers,
531
00:22:39.450 --> 00:22:41.770
which means you get specific wavelengths
532
00:22:42.090 --> 00:22:44.930
from the excitation. So it is all a
533
00:22:44.930 --> 00:22:46.660
mix of, of
534
00:22:47.460 --> 00:22:50.340
particles and waves, but it kind of brings
535
00:22:50.340 --> 00:22:52.940
it together and once you think of it in those
536
00:22:52.940 --> 00:22:54.820
terms, uh, then
537
00:22:56.100 --> 00:22:58.140
it becomes clear that you can't have a
538
00:22:58.140 --> 00:23:00.580
particle without its wave function.
539
00:23:00.980 --> 00:23:03.380
Andrew Dunkley: Which kind of writes off her second question.
540
00:23:03.380 --> 00:23:06.140
If there's, um, a long enough wavelength that
541
00:23:06.140 --> 00:23:07.940
we haven't got the equipment to detect it.
542
00:23:08.450 --> 00:23:10.260
Professor Fred Watson: Um, no, I don't think it does
543
00:23:11.380 --> 00:23:13.910
because I think, um,
544
00:23:14.970 --> 00:23:17.970
I mean we, you know, we. In, in
545
00:23:17.970 --> 00:23:20.410
a way the ultra low
546
00:23:20.410 --> 00:23:23.050
frequency radio waves are a bit like that,
547
00:23:23.730 --> 00:23:26.090
uh, because they are,
548
00:23:27.210 --> 00:23:29.009
uh. Some of them have got a wavelength bigger
549
00:23:29.009 --> 00:23:31.890
than the Earth. And
550
00:23:31.890 --> 00:23:34.050
so how do you detect that? Well, you've got
551
00:23:34.050 --> 00:23:36.090
to have a spacecraft that's got the other end
552
00:23:36.090 --> 00:23:38.850
of the aerial on it, you know, that sort of
553
00:23:38.850 --> 00:23:41.130
thing. Um, there's also,
554
00:23:42.530 --> 00:23:45.450
uh. What was I going to say,
555
00:23:45.630 --> 00:23:48.290
um, yeah, we know that there are
556
00:23:48.290 --> 00:23:50.970
gravitational waves that have got
557
00:23:51.290 --> 00:23:54.080
wavelengths measured in light years. Uh,
558
00:23:54.410 --> 00:23:56.650
I think the gravitational
559
00:23:57.690 --> 00:24:00.450
properties of the Big Bang. So the
560
00:24:00.450 --> 00:24:02.290
gravitational waves that were set up by the
561
00:24:02.290 --> 00:24:05.210
Big Bang are extremely long
562
00:24:05.290 --> 00:24:07.370
wavelength. I think I've got that the right
563
00:24:07.370 --> 00:24:10.000
way around. Um,
564
00:24:10.080 --> 00:24:12.840
it's so, uh. And we, you know, there are
565
00:24:12.840 --> 00:24:15.760
ones that we don't have normal,
566
00:24:16.160 --> 00:24:18.720
everyday ways of detecting them. There are
567
00:24:18.720 --> 00:24:20.520
subtleties because you expect some of these
568
00:24:20.520 --> 00:24:22.720
waves to be polarised. And that, I think,
569
00:24:22.720 --> 00:24:24.999
gives you an insight into it. But, yeah,
570
00:24:24.999 --> 00:24:27.920
it's, uh. Look, it is a good question.
571
00:24:28.600 --> 00:24:31.400
Uh, and I, uh, think, um, once again,
572
00:24:31.400 --> 00:24:34.360
mist is thinking outside the box. Uh,
573
00:24:34.360 --> 00:24:36.960
no particles without their wave
574
00:24:36.960 --> 00:24:39.480
function, because a particle is an
575
00:24:39.480 --> 00:24:42.260
excitation of the underlying field, a
576
00:24:42.260 --> 00:24:44.540
quantized excitation of the underlying field.
577
00:24:45.020 --> 00:24:47.740
Andrew Dunkley: So it is possible we cannot detect certain
578
00:24:47.740 --> 00:24:49.620
wavelengths because they're too big, but they
579
00:24:49.620 --> 00:24:50.300
still exist.
580
00:24:50.540 --> 00:24:51.780
Professor Fred Watson: I think that's right, yes.
581
00:24:51.780 --> 00:24:54.060
Andrew Dunkley: Yeah. All right. What about gravitons? Do you
582
00:24:54.060 --> 00:24:55.380
reckon they have a wavelength?
583
00:24:55.380 --> 00:24:57.700
Professor Fred Watson: Well, yes, they do. That's the thing. Um, if
584
00:24:57.700 --> 00:24:59.630
they exist, yes. Uh, because, um,
585
00:25:01.030 --> 00:25:03.980
uh, we've got gravitational waves. So the
586
00:25:03.980 --> 00:25:06.100
wave particle duality works both ways. If
587
00:25:06.100 --> 00:25:07.580
you've got a wave, you've got a particle.
588
00:25:07.900 --> 00:25:10.780
Andrew Dunkley: There you go. Uh, good one. Thanks,
589
00:25:10.780 --> 00:25:13.220
Misty. Hope all is well in Pennsylvania.
590
00:25:16.100 --> 00:25:18.420
Three, two, one.
591
00:25:18.980 --> 00:25:20.260
Professor Fred Watson: Space nuts.
592
00:25:20.500 --> 00:25:23.380
Andrew Dunkley: And our final question, uh, comes from
593
00:25:23.380 --> 00:25:25.380
another one of our regular contributors,
594
00:25:25.380 --> 00:25:28.140
Casey in Colorado. What does it feel
595
00:25:28.140 --> 00:25:30.740
like to go from weightlessness to normal
596
00:25:30.740 --> 00:25:33.060
gravity for astronauts when returning to
597
00:25:33.060 --> 00:25:36.030
Earth? I think it would depend
598
00:25:36.030 --> 00:25:38.940
on how long you've been up there and, uh,
599
00:25:38.940 --> 00:25:40.470
whether or not you've actually bothered to
600
00:25:40.470 --> 00:25:41.470
use the treadmill.
601
00:25:43.230 --> 00:25:45.030
Professor Fred Watson: Well, that's right. The treadmill is all
602
00:25:45.030 --> 00:25:46.750
about keeping up your muscle strength.
603
00:25:46.910 --> 00:25:49.070
Andrew Dunkley: Exactly. Um, because once you're out there,
604
00:25:49.310 --> 00:25:51.900
your muscles immediately start to wither. Uh,
605
00:25:52.390 --> 00:25:52.910
they do.
606
00:25:52.910 --> 00:25:55.390
Professor Fred Watson: And you don't really have anything against
607
00:25:55.390 --> 00:25:58.230
which to push to keep them,
608
00:25:58.230 --> 00:26:00.060
you know, keep them going, other than the.
609
00:26:00.530 --> 00:26:02.450
The, um, torture equipment that
610
00:26:03.490 --> 00:26:06.010
NASA and Roscosmos provide on their space
611
00:26:06.010 --> 00:26:06.530
station.
612
00:26:06.530 --> 00:26:08.890
Andrew Dunkley: I think on Space Lab, they didn't have a
613
00:26:08.890 --> 00:26:10.850
treadmill. They had a running track that ran
614
00:26:10.850 --> 00:26:13.810
around the inside of
615
00:26:14.850 --> 00:26:17.850
wall of, uh, Skylab, I think. And
616
00:26:17.850 --> 00:26:20.690
so I've seen footage of astronauts actually
617
00:26:20.690 --> 00:26:23.090
running in a circle around the
618
00:26:23.410 --> 00:26:25.250
interior of Skylab.
619
00:26:25.570 --> 00:26:28.250
Professor Fred Watson: So they're keeping themselves, um, running
620
00:26:28.250 --> 00:26:30.290
just by the centrifugal force that they're
621
00:26:30.370 --> 00:26:32.990
setting up. Yeah, yeah, yeah. That's
622
00:26:32.990 --> 00:26:34.570
interesting. I didn't know that. That's, uh.
623
00:26:34.630 --> 00:26:37.270
Andrew Dunkley: Yeah, I'm sure that if you had online, you'd
624
00:26:37.270 --> 00:26:40.030
find Footage of it. I. I strongly remember
625
00:26:40.030 --> 00:26:42.430
that M. I saw it on the news one day and
626
00:26:42.430 --> 00:26:44.510
thought, wow, how did they do that? Well,
627
00:26:44.510 --> 00:26:45.620
there's no gravity, duh. Uh,
628
00:26:47.470 --> 00:26:49.230
Professor Fred Watson: yeah. Um,
629
00:26:50.350 --> 00:26:53.350
wasn't there something like that in 2001 A
630
00:26:53.350 --> 00:26:55.070
Space Odyssey? I think there was. Could have
631
00:26:55.070 --> 00:26:55.270
been.
632
00:26:55.270 --> 00:26:58.030
Andrew Dunkley: I think I watched that very recently.
633
00:26:58.110 --> 00:27:00.150
I just thought I really wanted to watch it
634
00:27:00.150 --> 00:27:02.500
again. But, um, I fell asleep. But
635
00:27:02.980 --> 00:27:04.860
it's very late. Judy had gone to bed, and I
636
00:27:04.860 --> 00:27:07.730
thought, oh, I might just start this. Uh,
637
00:27:07.730 --> 00:27:08.900
yeah, I was gone.
638
00:27:11.420 --> 00:27:13.860
Um, what was the question? Oh, uh, what's the
639
00:27:13.940 --> 00:27:16.620
feel like? I also remember seeing
640
00:27:16.620 --> 00:27:19.460
footage of cosmonauts, uh, coming back
641
00:27:19.460 --> 00:27:22.180
from very long haul time in space.
642
00:27:23.220 --> 00:27:25.580
And they'd get them out of the capsule once
643
00:27:25.580 --> 00:27:27.420
they came back to Earth and they couldn't
644
00:27:27.420 --> 00:27:27.820
stand up.
645
00:27:27.820 --> 00:27:29.740
Professor Fred Watson: Couldn't stand up. Yeah. I've seen similar
646
00:27:29.740 --> 00:27:32.740
things and. Well, you know, even with the
647
00:27:32.740 --> 00:27:34.960
exercise that the Artemis II crew
648
00:27:35.520 --> 00:27:38.240
were doing, they were a little bit wobbly
649
00:27:38.320 --> 00:27:40.920
when they got out of the spacecraft. And we
650
00:27:40.920 --> 00:27:43.920
all saw them going across the deck of the,
651
00:27:44.280 --> 00:27:46.820
uh, recovery ship. Uh,
652
00:27:47.280 --> 00:27:49.239
so I think how wobbly you are probably
653
00:27:49.239 --> 00:27:51.120
depends on just how much effort you've put
654
00:27:51.120 --> 00:27:53.720
into keeping up your muscle strength. So I
655
00:27:53.720 --> 00:27:56.480
think that's the key thing that Casey
656
00:27:57.360 --> 00:28:00.280
might be thinking of. Um, exactly. As
657
00:28:00.280 --> 00:28:02.600
you've said, your muscles go to waste very
658
00:28:02.600 --> 00:28:05.100
quickly. Uh, and if you. You don't
659
00:28:05.100 --> 00:28:06.740
exercise, then you're going to be in big
660
00:28:06.740 --> 00:28:08.780
trouble. You simply would not be able to
661
00:28:08.780 --> 00:28:11.700
walk. Um, so quite a
662
00:28:11.700 --> 00:28:14.140
significant, uh, thing. Ah. Which would also,
663
00:28:14.140 --> 00:28:16.180
of course, depend on how long you've been in
664
00:28:16.180 --> 00:28:17.580
space, how long you've been weightless.
665
00:28:17.820 --> 00:28:20.259
Andrew Dunkley: And the other thing they might suffer from is
666
00:28:20.259 --> 00:28:23.100
fatigue because they have
667
00:28:23.100 --> 00:28:26.060
to work so much harder to achieve the same
668
00:28:26.940 --> 00:28:29.180
mobility as they were used to. When they had
669
00:28:29.180 --> 00:28:32.120
full muscle strength, they'd get
670
00:28:32.120 --> 00:28:34.600
very tired very fast. I think,
671
00:28:35.560 --> 00:28:37.560
all jokes aside, I think the,
672
00:28:38.130 --> 00:28:39.880
um, everyday person,
673
00:28:41.300 --> 00:28:43.340
uh, who's been through, um,
674
00:28:43.480 --> 00:28:46.200
immunotherapy or some
675
00:28:46.200 --> 00:28:49.120
form of, um, um, um,
676
00:28:49.400 --> 00:28:51.620
inhibitor for, um,
677
00:28:53.080 --> 00:28:56.080
testosterone, for example, for cancer
678
00:28:56.080 --> 00:28:58.990
treatment or something like that, that
679
00:28:58.990 --> 00:29:01.110
has the same effect on your muscles. Muscle
680
00:29:01.110 --> 00:29:03.550
wastage. When you stop producing testosterone
681
00:29:04.510 --> 00:29:06.590
as a male, your muscles
682
00:29:07.550 --> 00:29:09.350
actually do fade away. And you've got to do
683
00:29:09.350 --> 00:29:12.270
exercise to keep. Like astronauts, you've got
684
00:29:12.270 --> 00:29:14.190
to keep your exercise up to keep your muscles
685
00:29:14.190 --> 00:29:17.070
in trim, but it
686
00:29:17.070 --> 00:29:20.030
does slow you down. Um, and case in
687
00:29:20.030 --> 00:29:22.230
point, I did have that sort of treatment for
688
00:29:22.230 --> 00:29:24.590
my prostate cancer. And for six months
689
00:29:25.660 --> 00:29:28.180
I went into basically the
690
00:29:28.180 --> 00:29:30.460
equivalent to menopause. I had muscle
691
00:29:30.460 --> 00:29:32.980
wastage. Um, I kept up my
692
00:29:32.980 --> 00:29:35.740
exercise, but it wasn't enough. And I
693
00:29:35.980 --> 00:29:38.060
had a situation where I'd go out and play
694
00:29:38.060 --> 00:29:40.899
golf. I lost 40 yards on
695
00:29:40.899 --> 00:29:43.460
shots simply because my muscles had wasted
696
00:29:43.460 --> 00:29:46.180
away. And it's probably taken a year to get
697
00:29:46.180 --> 00:29:46.780
it all back.
698
00:29:47.100 --> 00:29:47.740
Professor Fred Watson: Yeah, interesting.
699
00:29:48.620 --> 00:29:51.580
Andrew Dunkley: Yeah. Um, it would be the same effect for an
700
00:29:51.580 --> 00:29:53.780
astronaut on it. Exactly the same. Different,
701
00:29:53.860 --> 00:29:56.100
different, you know, different mechanism.
702
00:29:56.180 --> 00:29:58.100
Mechanism, but same effect.
703
00:29:59.010 --> 00:30:01.900
Um, and. And yet the
704
00:30:01.900 --> 00:30:03.500
other thing that they'd probably have to deal
705
00:30:03.500 --> 00:30:05.140
with is some, some of them have very
706
00:30:05.700 --> 00:30:08.660
significant health effects from, from
707
00:30:08.660 --> 00:30:10.700
being in zero G and you come back to Earth.
708
00:30:10.700 --> 00:30:13.620
Like we had a, um, didn't. Wasn't there an
709
00:30:13.620 --> 00:30:15.700
astronaut recently who was temporarily
710
00:30:15.700 --> 00:30:18.500
blinded from,
711
00:30:18.500 --> 00:30:21.260
from zero G? And there's all sorts of
712
00:30:21.260 --> 00:30:24.260
things that um, they can suffer from. And
713
00:30:24.660 --> 00:30:26.140
a lot of the time when they come back to
714
00:30:26.140 --> 00:30:28.540
Earth, it does fix itself because you're back
715
00:30:28.540 --> 00:30:31.340
in your normal environment. But when you're
716
00:30:31.340 --> 00:30:33.420
out there orbiting or going to the moon and
717
00:30:33.420 --> 00:30:36.100
back, it is not a human environment.
718
00:30:36.980 --> 00:30:39.500
Professor Fred Watson: That's not normal. Yeah, so it was an
719
00:30:39.500 --> 00:30:42.100
evacuation the uh, beginning of the year, I
720
00:30:42.100 --> 00:30:44.060
think it was, that we only really found out a
721
00:30:44.060 --> 00:30:46.900
few snippets about not very long ago.
722
00:30:47.780 --> 00:30:49.700
And I can't remember what the details were
723
00:30:50.260 --> 00:30:52.480
because my brain's atrophy because of
724
00:30:54.720 --> 00:30:55.440
old age.
725
00:30:56.320 --> 00:30:59.320
Andrew Dunkley: Yes, indeed. But, uh, there
726
00:30:59.320 --> 00:31:02.030
would be various levels of, um,
727
00:31:02.030 --> 00:31:04.320
dysfunction as a consequence of spending time
728
00:31:04.320 --> 00:31:07.280
in space. It would be a
729
00:31:07.840 --> 00:31:10.480
person to person variable.
730
00:31:10.790 --> 00:31:13.480
Um, it's not a one size
731
00:31:13.480 --> 00:31:15.800
fits all situation. Some people who'd come
732
00:31:15.800 --> 00:31:18.600
back probably not feel anything. But if, um,
733
00:31:18.800 --> 00:31:20.840
if you're up there long enough. Yeah, it's
734
00:31:20.840 --> 00:31:22.400
going to have a big impact on you.
735
00:31:22.400 --> 00:31:23.440
Professor Fred Watson: Yes, indeed.
736
00:31:24.240 --> 00:31:26.400
Andrew Dunkley: Thank you so much for the question, Kasey. I
737
00:31:26.400 --> 00:31:29.120
hope we covered it
738
00:31:29.360 --> 00:31:32.240
reasonably well. Um, anyway,
739
00:31:32.290 --> 00:31:34.960
uh, in the not too distant future, I'm pretty
740
00:31:34.960 --> 00:31:36.600
sure there'll be so many people going in and
741
00:31:36.600 --> 00:31:38.600
out of space, they'll come up with ways of
742
00:31:38.600 --> 00:31:41.520
dealing with it. Who knows? And
743
00:31:41.520 --> 00:31:42.960
I think that brings us to the end.
744
00:31:42.960 --> 00:31:44.720
Don't forget, if you've got, uh, questions
745
00:31:44.720 --> 00:31:47.360
for us or observations or comments or
746
00:31:47.360 --> 00:31:49.200
whatever you like, you can go to our website,
747
00:31:49.820 --> 00:31:51.940
send it to us in a text or audio
748
00:31:51.940 --> 00:31:53.344
format@spacenuts
749
00:31:53.656 --> 00:31:55.300
IO or
750
00:31:55.300 --> 00:31:58.060
spacenutspodcast.com
751
00:31:58.460 --> 00:32:01.220
and just click on the little ama button at
752
00:32:01.220 --> 00:32:04.060
the top that stands for Ask me Anything. And
753
00:32:04.930 --> 00:32:07.420
um, you can send it through. Don't forget to
754
00:32:07.500 --> 00:32:09.980
tell us who you are or where you're from.
755
00:32:11.420 --> 00:32:13.140
And Fred Watson, that's it. Thanks so much
756
00:32:13.140 --> 00:32:15.500
for answering those. That was a tough batch
757
00:32:15.500 --> 00:32:15.820
today.
758
00:32:17.500 --> 00:32:19.380
Professor Fred Watson: Great questions though. Well done. To all our
759
00:32:19.380 --> 00:32:22.200
listeners for what they do in terms
760
00:32:22.200 --> 00:32:24.520
of, uh, thinking through a lot of these
761
00:32:24.520 --> 00:32:25.480
issues. It's great.
762
00:32:25.960 --> 00:32:27.520
Andrew Dunkley: Very good. All right, we'll catch you real
763
00:32:27.520 --> 00:32:28.640
soon. Fred Watson, thanks so much.
764
00:32:28.640 --> 00:32:30.040
Professor Fred Watson: Looking forward to it. Thanks, Andrew.
765
00:32:30.200 --> 00:32:32.000
Andrew Dunkley: Professor Fred Watson Watson, astronomer at
766
00:32:32.000 --> 00:32:34.240
large. And thanks to Huw in the studio, who
767
00:32:34.240 --> 00:32:35.980
couldn't be with us today because, um,
768
00:32:36.920 --> 00:32:39.560
there was, um, so much going on with
769
00:32:39.560 --> 00:32:41.960
gravitons and weightlessness, he just
770
00:32:42.360 --> 00:32:45.120
decided to float away. And from me,
771
00:32:45.120 --> 00:32:46.440
Andrew Dunkley. Thanks for your company.
772
00:32:46.440 --> 00:32:47.840
We'll catch you on the next episode of
773
00:32:47.840 --> 00:32:48.710
SpaceNuts real soon.
774
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Professor Fred Watson: Soon.
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Andrew Dunkley: Bye. Bye. You've been listening
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to the Space Nuts podcast,
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available at Apple Podcasts, Spotify,
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iHeartRadio or your favourite podcast
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player. You can also stream on
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demand@bytes.com.
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Professor Fred Watson: this has been another quality podcast
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production from bytes.com.
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