Nuclear Power in Space, SETI from the Moon & the Hubble Tension Unravelled
Space Nuts: Exploring the CosmosApril 30, 2026
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00:33:4931.01 MB

Nuclear Power in Space, SETI from the Moon & the Hubble Tension Unravelled

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Nuclear Space Policies, SETI from the Moon, and the Hubble Tension In this riveting episode of Space Nuts, hosts Andrew Dunkley and Professor Fred Watson delve into a range of fascinating topics that are shaping the future of space exploration. From the Pentagon's new nuclear energy policy for space missions to the exciting potential of searching for extraterrestrial intelligence from the far side of the Moon, this episode is packed with insights that will leave you pondering the cosmos.
Episode Highlights:
Nuclear Energy in Space: Andrew and Fred Watson discuss the recent directive from the Pentagon to NASA for the development of nuclear power stations in space, exploring the implications for lunar and orbital power supply systems. They examine the benefits and challenges of using nuclear energy in space, addressing public concerns and the potential for collaboration among government agencies.
SETI from the Far Side of the Moon: The hosts explore the advantages of conducting the Search for Extraterrestrial Intelligence (SETI) from the Moon's far side, where Earthly radio noise is absent. They discuss the capabilities of China's Chang'e 4 mission and its low-frequency radio spectrometer, which is attempting to detect technosignatures that could indicate the presence of alien life.
The Hubble Tension Debate: Andrew and Fred Watson unpack the ongoing debate surrounding the Hubble constant, highlighting the discrepancies between measurements obtained through different methods. They discuss new research that aims to refine our understanding of the universe's expansion rate and its implications for our grasp of dark matter and dark energy.

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Stay curious, keep looking up, and join us next time for more stellar insights and cosmic wonders. Until then, clear skies and happy stargazing.

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00:00:00 --> 00:00:02 Andrew Dunkley: Hello again. Thank you for joining us. This

00:00:02 --> 00:00:05 is Space Nuts. My name is Andrew

00:00:05 --> 00:00:07 Dunkley. If you've never heard of Space Nuts,

00:00:07 --> 00:00:08 where have you been for the last 10 years?

00:00:09 --> 00:00:11 Good, uh, to have you along if you're a first

00:00:11 --> 00:00:13 timer. And everybody else who's been with us

00:00:13 --> 00:00:16 for aeons. Uh, today

00:00:16 --> 00:00:18 on the show we will be talking about,

00:00:18 --> 00:00:21 uh, a. Ah, really interesting and some

00:00:21 --> 00:00:24 might think scary development, nuclear

00:00:24 --> 00:00:27 space policies. I don't think they're talking

00:00:27 --> 00:00:30 about, you know, weapons of mass destruction,

00:00:30 --> 00:00:32 but they are talking about power supply

00:00:32 --> 00:00:34 systems. We're, uh, also going to look at

00:00:34 --> 00:00:37 SETI from the far side of the moon because,

00:00:37 --> 00:00:40 uh, that's the best place to listen for alien

00:00:40 --> 00:00:43 civilizations because, well, Earth is very

00:00:43 --> 00:00:46 noisy. But the far side of the moon,

00:00:46 --> 00:00:48 you can't hear a thing. Except the aliens,

00:00:49 --> 00:00:52 apparently. And. Oh, uh, no. The

00:00:52 --> 00:00:54 Hubble tension debate is simmering

00:00:54 --> 00:00:56 again. We'll get into all of that on, on

00:00:56 --> 00:00:59 this, uh, this episode of space

00:00:59 --> 00:01:00 nuts.

00:01:00 --> 00:01:03 Generic: 15 seconds. Guidance is internal.

00:01:03 --> 00:01:06 10, 9. Ignition

00:01:06 --> 00:01:07 sequence start.

00:01:07 --> 00:01:07 Professor Fred Watson: Space nuts.

00:01:08 --> 00:01:10 Generic: 5, 4, 3, 2. 1. 2, 3, 4,

00:01:10 --> 00:01:12 5, 5, 4, 3, 2, 1.

00:01:13 --> 00:01:14 Andrew Dunkley: Space nuts.

00:01:14 --> 00:01:16 Generic: Astronauts report it feels good.

00:01:17 --> 00:01:19 Andrew Dunkley: And joining us to nuke a few storeys is

00:01:19 --> 00:01:21 Professor Fred Watson Watson, uh, astronomer

00:01:21 --> 00:01:22 at large. Hello, Fred Watson.

00:01:23 --> 00:01:26 Professor Fred Watson: Hello, Andrew. Lovely to hear, uh, your

00:01:26 --> 00:01:28 voice and see your face.

00:01:28 --> 00:01:30 Andrew Dunkley: Yes, my voice is still a little bit down

00:01:31 --> 00:01:33 like that. Could do an Elvis song as a

00:01:33 --> 00:01:34 backing.

00:01:34 --> 00:01:36 Professor Fred Watson: Oh, you could, yeah, yeah, Way on, just down.

00:01:37 --> 00:01:39 Well, we. So at the end of the show, you

00:01:39 --> 00:01:42 definitely need to say thank you very much.

00:01:42 --> 00:01:44 Andrew Dunkley: Thank you very much. Uh, yes,

00:01:44 --> 00:01:46 that's what happens when I get a cold. My

00:01:46 --> 00:01:49 voice just goes down deep. When I first

00:01:49 --> 00:01:51 started in radio, I did midnight to dawns. In

00:01:51 --> 00:01:53 the days where they didn't automate it,

00:01:53 --> 00:01:55 everything, everything was live.

00:01:56 --> 00:01:58 And around four in the morning when I used to

00:01:58 --> 00:02:01 get really, really tired, my voice would just

00:02:01 --> 00:02:04 naturally go down there and.

00:02:05 --> 00:02:07 And it was really weird because, um,

00:02:07 --> 00:02:10 it wasn't my natural voice. But,

00:02:10 --> 00:02:12 um, at the moment it's. It's enjoying that

00:02:12 --> 00:02:14 part of the spectrum.

00:02:14 --> 00:02:16 Professor Fred Watson: So, m. Yes.

00:02:16 --> 00:02:18 Andrew Dunkley: Hopefully it'll get better soon. I don't like

00:02:18 --> 00:02:19 the feeling, I must say.

00:02:19 --> 00:02:20 Professor Fred Watson: No, you wouldn't.

00:02:20 --> 00:02:22 Andrew Dunkley: Anyway, we battle on, don't we?

00:02:22 --> 00:02:25 Professor Fred Watson: No point getting all that's. You know,

00:02:25 --> 00:02:28 we do in Space Nuts. We come rain or shine

00:02:28 --> 00:02:31 or absence or whatever, we keep going. We do.

00:02:31 --> 00:02:34 Andrew Dunkley: Speaking of battling on nuclear energy,

00:02:36 --> 00:02:39 uh, this. This is a policy that's just been

00:02:39 --> 00:02:42 announced by the Pentagon and the Department

00:02:42 --> 00:02:44 of Energy and they've kind of dragged NASA

00:02:44 --> 00:02:47 into it. They said, hey, NASA,

00:02:47 --> 00:02:49 we want you to build us a couple of power

00:02:49 --> 00:02:50 stations and they've got to be nuclear and

00:02:50 --> 00:02:53 they've got to be ready by 2028. How about

00:02:53 --> 00:02:53 it?

00:02:54 --> 00:02:56 Professor Fred Watson: Yeah, that's more or less it.

00:02:57 --> 00:03:00 It's a six page policy document.

00:03:00 --> 00:03:03 Uh, its title is NSTM

00:03:03 --> 00:03:06 M3. Uh, which is

00:03:06 --> 00:03:09 to direct a parallel and mutually

00:03:09 --> 00:03:11 reinforcing design, uh, set of design

00:03:11 --> 00:03:14 competitions by NASA and the Defence

00:03:14 --> 00:03:16 Department to enable, and I'm quoting here,

00:03:16 --> 00:03:18 to enable near term demonstration and use of

00:03:19 --> 00:03:22 mid power space reactors in orbit and on the

00:03:22 --> 00:03:24 lunar surface and prepare to deploy

00:03:25 --> 00:03:27 high power reactors in the 2000 and 30s.

00:03:28 --> 00:03:31 Uh, I'm quoting here from uh,

00:03:31 --> 00:03:33 people who are closely involved with this.

00:03:33 --> 00:03:36 For this to work it has to be a collaboration

00:03:36 --> 00:03:38 between multiple government agencies. Well

00:03:39 --> 00:03:41 that's a novel idea, isn't it? Yeah,

00:03:41 --> 00:03:43 um, that's the way that work.

00:03:44 --> 00:03:47 Yeah, that's the way that we do the right R

00:03:47 --> 00:03:49 D and get the right tools in place for these

00:03:49 --> 00:03:51 events to unfold over the next few years.

00:03:51 --> 00:03:54 Yeah. Yes. So um, that's right. So the

00:03:54 --> 00:03:57 bottom line is NASA is

00:03:57 --> 00:03:59 directed to start work within

00:03:59 --> 00:04:02 30 days on a mid power space

00:04:02 --> 00:04:05 reactor generating at least 20 kilowatts of

00:04:05 --> 00:04:07 power with a variant that can operate on the

00:04:07 --> 00:04:09 lunar surface. He calls for the

00:04:09 --> 00:04:11 agency to work with multiple companies on

00:04:11 --> 00:04:13 reactor designs including for a low power

00:04:13 --> 00:04:16 system that produces as little as 1 kilowatt

00:04:16 --> 00:04:19 if doing so offers lower cost and schedule

00:04:19 --> 00:04:21 risk. And this is um, it's a White House

00:04:22 --> 00:04:24 release, uh, that I'm quot from here. So

00:04:24 --> 00:04:26 it's, it's definitely the official thing.

00:04:26 --> 00:04:27 Yeah. Wow.

00:04:27 --> 00:04:29 Andrew Dunkley: Should we be surprised by this though?

00:04:29 --> 00:04:32 Professor Fred Watson: Uh no, no we shouldn't. I mean actually

00:04:32 --> 00:04:35 we did get um. Was it Jared Isaacman, the

00:04:35 --> 00:04:38 uh, the new, relatively new head of

00:04:38 --> 00:04:41 NASA, who I think we covered this uh,

00:04:41 --> 00:04:44 quite a few months ago, talked about the idea

00:04:44 --> 00:04:46 of uh, using a uh, 100 kilowatt

00:04:47 --> 00:04:49 nuclear reactor on the lunar surface. Because

00:04:49 --> 00:04:51 that raises a few eyebrows. Uh, but it looks

00:04:51 --> 00:04:54 as though this is the first step in, in

00:04:55 --> 00:04:58 expediting that uh, to start small,

00:04:58 --> 00:05:01 maybe even the smallest 1kW it'll run an

00:05:01 --> 00:05:03 electric fire and uh,

00:05:04 --> 00:05:07 keep um, going upwards. Uh, there's an

00:05:07 --> 00:05:09 interesting uh, disparity in

00:05:10 --> 00:05:12 the sort of urgency of this though because

00:05:12 --> 00:05:15 um, the next paragraph of the White House

00:05:15 --> 00:05:17 release says the policy calls on the Defence

00:05:17 --> 00:05:20 Department to provide a briefing to the

00:05:20 --> 00:05:23 White House in 90 days on um, potential

00:05:23 --> 00:05:26 uses and payloads for space nuclear systems

00:05:26 --> 00:05:28 of varying power levels. The Pentagon will in

00:05:28 --> 00:05:30 the first year of the policy use its space

00:05:30 --> 00:05:33 nuclear funding to support NASA's efforts,

00:05:33 --> 00:05:35 then conduct its own competition for space

00:05:35 --> 00:05:38 nuclear power systems. I get the feeling here

00:05:38 --> 00:05:40 that there's going to be too many fingers in

00:05:40 --> 00:05:43 the pie and too many people deciding which

00:05:43 --> 00:05:45 companies are going to get the, you know,

00:05:45 --> 00:05:47 going to get the contracts to do this.

00:05:48 --> 00:05:51 Andrew Dunkley: The options for nuclear power these days

00:05:51 --> 00:05:53 are so much more,

00:05:54 --> 00:05:56 uh, available and simple. Like

00:05:56 --> 00:05:59 you can make very small nuclear power

00:05:59 --> 00:06:02 stations now. You can, you can build one

00:06:03 --> 00:06:05 that's, that's small enough just to service a

00:06:05 --> 00:06:08 town these days. You don't need these big

00:06:08 --> 00:06:11 complex setups anymore.

00:06:11 --> 00:06:14 So it probably is the logical way to go.

00:06:14 --> 00:06:16 Even though when you say the word nuclear,

00:06:16 --> 00:06:18 everybody sort of runs for the hills. Not

00:06:18 --> 00:06:21 that that would save them, but um,

00:06:21 --> 00:06:24 it's not, ah, as big and scary as people

00:06:25 --> 00:06:28 envisage. But um, it's, it's got bad

00:06:28 --> 00:06:30 press for a long, long time. So whenever you

00:06:30 --> 00:06:32 talk about nuclear power station or look what

00:06:32 --> 00:06:35 happened in Australia, um, we're so

00:06:35 --> 00:06:36 scared of it. We've never done it.

00:06:38 --> 00:06:40 Professor Fred Watson: And people think of Three Mile, Three Mile

00:06:40 --> 00:06:42 island in Chernobyl.

00:06:43 --> 00:06:46 Uh, and uh, yes. And the bottom line

00:06:46 --> 00:06:48 is that if things go wrong, you have a very

00:06:48 --> 00:06:51 big environmental problem. And uh, that would

00:06:51 --> 00:06:52 be the case.

00:06:52 --> 00:06:53 Andrew Dunkley: It's fukush.

00:06:53 --> 00:06:53 Professor Fred Watson: Yeah.

00:06:53 --> 00:06:56 Andrew Dunkley: With the earthquake and the tide and the

00:06:56 --> 00:06:59 tsunami. Yeah, that's so mess.

00:06:59 --> 00:07:02 Professor Fred Watson: Yes. So, uh, it is scary, I

00:07:02 --> 00:07:05 think. Um, but, but

00:07:05 --> 00:07:08 well, so I grew up in a country that, uh,

00:07:08 --> 00:07:10 pioneered nuclear power with the US

00:07:11 --> 00:07:13 and there are several nuclear power stations.

00:07:14 --> 00:07:15 Uh, I used to live not very far from one

00:07:15 --> 00:07:18 actually at uh, Torness in Scotland.

00:07:20 --> 00:07:22 Yes, I think it's Taunus. Uh, and

00:07:23 --> 00:07:26 look, everybody just regarded it as

00:07:26 --> 00:07:29 a normal power station. It was very much a

00:07:29 --> 00:07:31 low key thing. Uh, and you

00:07:32 --> 00:07:35 see statistics like there's more

00:07:35 --> 00:07:38 radiation comes from the natural emissions

00:07:38 --> 00:07:40 from rocks in the uk. If you go down to

00:07:40 --> 00:07:43 Cornwall, the rocks are basically radioactive

00:07:43 --> 00:07:43 there.

00:07:43 --> 00:07:44 Andrew Dunkley: Oh wow.

00:07:44 --> 00:07:47 Professor Fred Watson: There's radon in the atmosphere. Um, but it's

00:07:47 --> 00:07:49 at a level that humans can tolerate. Humans

00:07:49 --> 00:07:52 have been tolerating it for hundreds of

00:07:52 --> 00:07:54 thousands of years. And uh, that's.

00:07:54 --> 00:07:57 Andrew Dunkley: Yeah, you're exposed to radiation every time

00:07:57 --> 00:07:58 you walk outside.

00:07:58 --> 00:08:01 Professor Fred Watson: Well, that's right, you are. Yes. So, um, so

00:08:01 --> 00:08:04 it, it's got to be treated with respect.

00:08:04 --> 00:08:07 Um, I, I think what freaks people out

00:08:07 --> 00:08:10 though as well is the idea of sticking a

00:08:10 --> 00:08:13 nuclear reactor on top of a rocket and then

00:08:13 --> 00:08:15 sending it into space. And there was an

00:08:15 --> 00:08:18 accident, uh, with a. So just

00:08:18 --> 00:08:21 stepping back, uh, NAS, their

00:08:21 --> 00:08:24 RTGs, radioisotope

00:08:24 --> 00:08:27 thermal generator, thermoelectric generators,

00:08:27 --> 00:08:29 I think that's what it stands for. Uh, on

00:08:29 --> 00:08:31 several spacecraft, including the two

00:08:31 --> 00:08:34 Voyagers, I think the pioneers have got it as

00:08:34 --> 00:08:36 well. Um, the Curiosity, um,

00:08:38 --> 00:08:40 and um, Perseverance.

00:08:40 --> 00:08:43 Both have RTG power supplies. Uh,

00:08:43 --> 00:08:46 so that's uh, uh,

00:08:46 --> 00:08:49 a well trodden path. But there was an

00:08:49 --> 00:08:50 accident, I think it might have been in the

00:08:50 --> 00:08:52 80s with a spacecraft that was launched with

00:08:53 --> 00:08:55 something like an RTG on board and it did,

00:08:56 --> 00:08:59 uh, it went wrong. I can't remember

00:08:59 --> 00:09:01 the details but I think it was Canada that

00:09:01 --> 00:09:03 took the punch. And there was a lot of

00:09:04 --> 00:09:06 radioactive debris that got spread over

00:09:07 --> 00:09:09 very, very sparsely, uh,

00:09:10 --> 00:09:12 populated regions. Uh,

00:09:12 --> 00:09:15 literal fallout. Yes, that's right. Yes,

00:09:15 --> 00:09:18 exactly. Flaws out the sky. If I remember

00:09:18 --> 00:09:20 rightly. I'm digging up things from the past

00:09:20 --> 00:09:22 year, but I think that's the case and that

00:09:22 --> 00:09:24 clearly freaks people out. If you've got a

00:09:24 --> 00:09:27 launch that doesn't work, uh, what's going to

00:09:27 --> 00:09:27 happen?

00:09:28 --> 00:09:31 Andrew Dunkley: I imagine so. But uh, it certainly does ramp

00:09:31 --> 00:09:33 up the space race between the US and China.

00:09:33 --> 00:09:35 And you know, China's probably going to fall

00:09:35 --> 00:09:37 a bit behind here because I think they were

00:09:37 --> 00:09:39 trying to set up a coal fired power station

00:09:39 --> 00:09:40 on the moon. You know, it

00:09:40 --> 00:09:43 um, might m, might

00:09:43 --> 00:09:44 slow them down a bit.

00:09:44 --> 00:09:46 Professor Fred Watson: Yeah, China's doing pretty well. They are

00:09:46 --> 00:09:49 doing sustainability. Yeah, yeah, they are.

00:09:49 --> 00:09:51 Ah, but yeah, they do use a lot of coal

00:09:51 --> 00:09:51 still.

00:09:51 --> 00:09:54 Andrew Dunkley: Yeah, they do, they do. So this is probably

00:09:54 --> 00:09:57 going to happen and what other

00:09:57 --> 00:09:59 option would there be? That's the thing. I

00:09:59 --> 00:10:01 mean some people will say no, put up solar

00:10:01 --> 00:10:04 energy systems, but um,

00:10:04 --> 00:10:06 nuclear is probably a much more

00:10:06 --> 00:10:08 efficient way of doing it.

00:10:08 --> 00:10:10 Professor Fred Watson: Yeah, well for a start, you've got the

00:10:10 --> 00:10:12 baseline load. You're not worried about where

00:10:12 --> 00:10:15 the sun is in the sky. The idea

00:10:15 --> 00:10:18 of being at the south pole of the moon,

00:10:19 --> 00:10:21 which is where the focus is in terms

00:10:21 --> 00:10:24 of our uh, exploration of the moon.

00:10:24 --> 00:10:27 Uh, it puts a different slant

00:10:27 --> 00:10:30 on it because it means that you are looking

00:10:30 --> 00:10:33 at a very low sun altitude in the

00:10:33 --> 00:10:35 sky. Uh, the sun's coming in nearly

00:10:35 --> 00:10:37 horizontally. The sunlight, now that's not

00:10:38 --> 00:10:41 uh, as bad a thing on the moon as it would be

00:10:41 --> 00:10:43 on the Earth. The Earth, as the sun gets

00:10:43 --> 00:10:44 lower, it's going through a thicker and

00:10:44 --> 00:10:47 thicker layer of atmosphere. So its uh, power

00:10:47 --> 00:10:50 is attenuated. On the moon that doesn't

00:10:50 --> 00:10:52 happen because there ain't no atmosphere. But

00:10:52 --> 00:10:55 it does bring challenges for your solar

00:10:55 --> 00:10:56 panels. You know, you've got to build arrays

00:10:56 --> 00:10:58 that are almost vertical and if you're

00:10:58 --> 00:11:01 looking for a big structure, uh, then

00:11:01 --> 00:11:04 uh, it becomes different slightly different

00:11:04 --> 00:11:07 engineering, um, issue. Plus you've got to

00:11:07 --> 00:11:09 take all that stuff up there as well. You

00:11:09 --> 00:11:12 know, going up to the moon with arrays of

00:11:12 --> 00:11:14 solar panels in the spacecraft might not

00:11:14 --> 00:11:16 leave room for much else. Whereas a nuclear

00:11:16 --> 00:11:18 reactor of the kind that people are talking

00:11:18 --> 00:11:20 about would be relatively compact. I m mean,

00:11:20 --> 00:11:23 the RTG devices are, I think

00:11:23 --> 00:11:26 it's, is it 13 kilogrammes of, uh,

00:11:26 --> 00:11:29 plutonium that they have in them.

00:11:29 --> 00:11:32 They're about the size of a, you know,

00:11:32 --> 00:11:35 a tea urn or something like that. Or a drink

00:11:35 --> 00:11:37 serum. Yeah, yeah.

00:11:37 --> 00:11:40 Andrew Dunkley: It's much simpler than it was 20, 30,

00:11:40 --> 00:11:43 40, 50 years ago. And of course they're

00:11:43 --> 00:11:45 talking not only about the moon, but people,

00:11:45 --> 00:11:48 uh, on Mars, uh, they'll need power as well.

00:11:48 --> 00:11:50 Um, I know in the movie the Martian they used

00:11:50 --> 00:11:52 solar panels, but that Mars is a bit further

00:11:52 --> 00:11:54 away, so the solar panels probably wouldn't

00:11:54 --> 00:11:55 be as efficient.

00:11:55 --> 00:11:56 Professor Fred Watson: Exactly.

00:11:57 --> 00:11:59 Andrew Dunkley: Nuclear, um, power makes, Makes perfect

00:11:59 --> 00:12:02 sense. Uh, although, you know, solar energy

00:12:02 --> 00:12:05 is quite, um, well used

00:12:05 --> 00:12:08 in space. Artemis 2 used it.

00:12:09 --> 00:12:11 Professor Fred Watson: Um, that's correct, yes. Uh, and

00:12:11 --> 00:12:13 um, you know, thinking of the different

00:12:13 --> 00:12:15 spacecraft, the one that's got perhaps the

00:12:15 --> 00:12:17 most spectacular solar panels is Lucy, uh,

00:12:18 --> 00:12:20 spacecraft which is on its way to the Trojan

00:12:20 --> 00:12:23 asteroids. Uh, and that's got

00:12:23 --> 00:12:26 solar panels which are huge. And that's

00:12:26 --> 00:12:28 because you're going out to the asteroid belt

00:12:28 --> 00:12:30 and beyond. Actually you go into the orbit of

00:12:30 --> 00:12:32 Jupiter, which is where the Trojan asteroids

00:12:32 --> 00:12:35 hang out. Uh, so you need big solar

00:12:35 --> 00:12:37 panels to collect all the energy. Yeah.

00:12:37 --> 00:12:39 Andrew Dunkley: The other problem with solar panels on Mars

00:12:39 --> 00:12:42 would be dust, because it's

00:12:42 --> 00:12:43 a pretty grubby place.

00:12:43 --> 00:12:46 Professor Fred Watson: Yeah, that's what, um, probably brought an

00:12:46 --> 00:12:49 end to. Uh, so Spirit and Opportunity both

00:12:49 --> 00:12:52 had solar panels. Uh, and there were

00:12:52 --> 00:12:55 certainly times when the amount of dust was

00:12:55 --> 00:12:57 stopping the power generation. And uh, that

00:12:57 --> 00:13:00 was cleared by, uh, Willy Willies, as they're

00:13:00 --> 00:13:03 called. Uh, the um, dust

00:13:03 --> 00:13:05 devils. That's right. On Mars. Yeah.

00:13:05 --> 00:13:05 Andrew Dunkley: Fascinating.

00:13:05 --> 00:13:08 All right, so the um, the directive has

00:13:08 --> 00:13:11 been put to NASA to start working on this,

00:13:11 --> 00:13:14 uh, and it comes from the White House. So,

00:13:14 --> 00:13:16 um, it's all systems go and they hope to have

00:13:16 --> 00:13:19 something operational as soon as 20,

00:13:19 --> 00:13:22 28. So they're not mucking around. In fact, I

00:13:22 --> 00:13:24 think NASA, after this was released, were

00:13:24 --> 00:13:25 given one month to it.

00:13:26 --> 00:13:28 Professor Fred Watson: Uh, that's, uh, exactly right. That's the 30

00:13:28 --> 00:13:29 days that I mentioned.

00:13:29 --> 00:13:30 Andrew Dunkley: No mucking around.

00:13:30 --> 00:13:31 Professor Fred Watson: Get going.

00:13:31 --> 00:13:33 Andrew Dunkley: Yep. Uh, you can read all about

00:13:33 --> 00:13:35 it@spacenews.com.

00:13:36 --> 00:13:38 this is Space Nuts with Andrew Dunkley and

00:13:38 --> 00:13:40 Professor Fred Watson Watson.

00:13:44 --> 00:13:45 Space Nuts.

00:13:46 --> 00:13:48 Well, we mentioned the moon. We'll stick with

00:13:48 --> 00:13:51 the moon. This storey though has nothing to

00:13:51 --> 00:13:53 do with people on the moon. It's got uh,

00:13:53 --> 00:13:56 everything to do with people that are not on

00:13:56 --> 00:13:58 Earth or the Moon or, or Mars for that

00:13:58 --> 00:14:00 matter. Uh, they're out there somewhere.

00:14:00 --> 00:14:02 We're looking for them. We're talking about

00:14:02 --> 00:14:05 the search for extraterrestrial intelligence

00:14:05 --> 00:14:07 and the dark side of the moon. The far side

00:14:07 --> 00:14:10 of the moon is um, the best place

00:14:10 --> 00:14:11 to start looking.

00:14:13 --> 00:14:15 Professor Fred Watson: Uh, that's right. So we've been looking for

00:14:15 --> 00:14:16 this for 60 years

00:14:18 --> 00:14:20 and using ground, uh, based

00:14:21 --> 00:14:24 antennas here on planet Earth, uh,

00:14:24 --> 00:14:26 which are very, uh, very capable.

00:14:28 --> 00:14:30 Um, once the Square Kilometre Array

00:14:30 --> 00:14:32 Observatory comes on stream towards the end

00:14:32 --> 00:14:34 of the decade, uh, we'll have the

00:14:34 --> 00:14:37 finest, most capable radio

00:14:37 --> 00:14:40 telescope in the world, uh, which will not

00:14:40 --> 00:14:43 directly engage with SETI programmes, but

00:14:43 --> 00:14:46 it will uh, have the

00:14:46 --> 00:14:49 sensitivity to detect. Well the thing that

00:14:49 --> 00:14:51 my colleagues tell me is it'll detect an

00:14:51 --> 00:14:53 airport radar at 50 light years.

00:14:54 --> 00:14:56 So that's the kind of sensitivity

00:14:57 --> 00:14:59 uh, that you're talking about. Um, but

00:15:00 --> 00:15:02 the main problem with ground based, with

00:15:02 --> 00:15:05 Earth based uh, radio telescopes

00:15:05 --> 00:15:07 is that they're compromised by all the

00:15:07 --> 00:15:10 cacophony of radio signals that

00:15:10 --> 00:15:12 surrounds us. From your mobile phones, from

00:15:12 --> 00:15:15 broadcasts from people like you and

00:15:15 --> 00:15:17 me doing this, going out into the ether,

00:15:18 --> 00:15:21 WI fi routers, WI fi, uh, the whole thing,

00:15:21 --> 00:15:23 microwave ovens, it all provides this

00:15:23 --> 00:15:26 noisy radio background and that's not getting

00:15:26 --> 00:15:29 any better with the um, satellite mega

00:15:29 --> 00:15:32 constellations. Uh, I was in uh, a meeting

00:15:32 --> 00:15:35 yesterday. It's

00:15:35 --> 00:15:37 a meeting of the um, International

00:15:37 --> 00:15:40 Astronomical Union Centre, uh, for the

00:15:40 --> 00:15:43 protection of the dark and quiet sky from

00:15:43 --> 00:15:45 satellite interference. Uh, and it

00:15:45 --> 00:15:48 was um, you know one of the things that's

00:15:48 --> 00:15:51 raising anxiety is the idea of uh, Elon

00:15:51 --> 00:15:52 Musk's million satellites for

00:15:55 --> 00:15:57 um, orbital data centres and

00:15:57 --> 00:16:00 this mirror in the sky idea, sunlight on

00:16:00 --> 00:16:02 demand, that also has a million satel mirrors

00:16:02 --> 00:16:05 on it. So that's more for the optical

00:16:05 --> 00:16:07 astronomers. But it's all a concern,

00:16:07 --> 00:16:10 uh, and it basically is eroding our

00:16:10 --> 00:16:13 capability slowly but surely to

00:16:13 --> 00:16:16 detect uh, faint extraterrestrial

00:16:16 --> 00:16:18 signals. Uh, so that

00:16:18 --> 00:16:21 brings us to currently possibly

00:16:21 --> 00:16:24 the best place to do this sort of thing from

00:16:25 --> 00:16:27 which is the far side of the moon.

00:16:28 --> 00:16:31 Uh, and um, uh,

00:16:31 --> 00:16:34 we have one uh, spacecraft.

00:16:34 --> 00:16:36 By we, I mean humankind have one

00:16:36 --> 00:16:39 spacecraft on the far side of the moon. Uh,

00:16:39 --> 00:16:41 it is China's Chang' e 4,

00:16:41 --> 00:16:44 uh, which soft landed on the far side of the

00:16:44 --> 00:16:47 moon back in 2019. Can you believe it?

00:16:47 --> 00:16:50 It's been there uh, seven

00:16:50 --> 00:16:53 years. It's quite Extraordinary. Um,

00:16:53 --> 00:16:55 but uh, now that, that

00:16:56 --> 00:16:58 um. Spacecraft was not set up

00:16:58 --> 00:17:01 uh specifically for uh,

00:17:01 --> 00:17:04 looking for um, SETI search for

00:17:04 --> 00:17:07 extraterrestrial intelligence but

00:17:07 --> 00:17:09 it's got a low frequency radio

00:17:09 --> 00:17:12 spectrometer on board um that

00:17:12 --> 00:17:15 actually has been used to conduct the first

00:17:15 --> 00:17:18 ever SETI search from the lunar far

00:17:18 --> 00:17:21 side. Um and so the

00:17:21 --> 00:17:23 goal, uh, the idea

00:17:24 --> 00:17:26 is to use that equipment which is

00:17:26 --> 00:17:29 designed to do natural sciences

00:17:29 --> 00:17:32 but to look for those

00:17:32 --> 00:17:35 ah, technosignatures, uh

00:17:35 --> 00:17:38 technomarkers they're sometimes called, uh,

00:17:38 --> 00:17:40 which might suggest that you're getting a

00:17:40 --> 00:17:43 signal from an artificially generated

00:17:43 --> 00:17:45 source. And what you're really looking for

00:17:46 --> 00:17:48 are ah, periodic

00:17:49 --> 00:17:52 um, bursts of radiation with perhaps

00:17:52 --> 00:17:53 regular intervals

00:17:54 --> 00:17:57 um, that are not easily explained

00:17:57 --> 00:18:00 by natural processes. And you've got to

00:18:00 --> 00:18:03 think back to Jocelyn Bell Burnell and her

00:18:04 --> 00:18:06 discovery uh, of the first pulsar because

00:18:06 --> 00:18:08 that's what she saw. Narrow um, band.

00:18:09 --> 00:18:12 Um. Sorry, narrow uh, band

00:18:12 --> 00:18:14 in time signatures, uh, or

00:18:14 --> 00:18:17 bursts of radiation which we now know is the

00:18:17 --> 00:18:19 pulsar, the kind of light ass beam of

00:18:19 --> 00:18:22 radiation from the pulsar sweeping around and

00:18:22 --> 00:18:25 passing the earth. Um, she didn't know that

00:18:25 --> 00:18:27 then. So she wrote little green men in her

00:18:27 --> 00:18:30 uh. On her chart record of very,

00:18:30 --> 00:18:33 very famous words. Um,

00:18:33 --> 00:18:36 so that's what basically uh, the uh,

00:18:36 --> 00:18:39 Chang', E, um Low Frequency Radio

00:18:39 --> 00:18:41 Spectrometer has been looking for. Uh, and

00:18:41 --> 00:18:44 it's things that um, you know, that speak

00:18:44 --> 00:18:47 of an artificial generated source.

00:18:47 --> 00:18:50 And so um, what they've

00:18:50 --> 00:18:52 done, uh the scientists working on this,

00:18:52 --> 00:18:55 uh basically they built an algorithm

00:18:56 --> 00:18:58 uh that ah, uh trawled through the data

00:18:59 --> 00:19:02 looking for anything that might

00:19:02 --> 00:19:05 be artificial. With no

00:19:05 --> 00:19:08 credible candidates revealed,

00:19:08 --> 00:19:11 uh, nothing that couldn't be explained either

00:19:11 --> 00:19:14 by you know, natural phenomena or by

00:19:14 --> 00:19:16 instrument, uh, issues.

00:19:17 --> 00:19:20 Um, there's a nice comment though

00:19:20 --> 00:19:22 from uh, phys.org who is carrying this

00:19:22 --> 00:19:25 storey. Uh, this is,

00:19:25 --> 00:19:28 I'll quote this. This is not a failure, it is

00:19:28 --> 00:19:30 a beginning. As Carl Sagan once put it,

00:19:30 --> 00:19:33 absence of evidence is not evidence of

00:19:33 --> 00:19:35 absence. Brilliant. Really good point.

00:19:36 --> 00:19:39 Andrew Dunkley: I had a lot of time for Carl Sagan, uh, very

00:19:39 --> 00:19:42 wise man and um. Yeah, he uh, he did a lot

00:19:42 --> 00:19:45 for astronomy during his time. But um,

00:19:45 --> 00:19:48 that's a valid point and, and I suppose you

00:19:48 --> 00:19:50 and I have spoken about it in the past. The

00:19:50 --> 00:19:52 big problem is distance. There might,

00:19:53 --> 00:19:55 there might be civilizations out there that

00:19:55 --> 00:19:58 are advanced and capable of communication but

00:19:58 --> 00:20:00 they're so far away we will never hear from

00:20:00 --> 00:20:01 them. Maybe that.

00:20:02 --> 00:20:04 Professor Fred Watson: Yeah, um, that's right. Uh,

00:20:04 --> 00:20:07 and you know, and time is the other issue.

00:20:07 --> 00:20:09 It's a needle in A haystack both in distance

00:20:09 --> 00:20:11 and in time because you've got to hit your

00:20:11 --> 00:20:14 civil station just at the right time. Yes.

00:20:15 --> 00:20:17 Uh, when uh, they are uh, technologically

00:20:17 --> 00:20:19 enough to have airport radar, uh, for

00:20:19 --> 00:20:22 example, but haven't wiped themselves out

00:20:22 --> 00:20:23 because of the loonies that they've

00:20:23 --> 00:20:24 generated.

00:20:24 --> 00:20:26 Andrew Dunkley: Yeah, you're more, you're more likely to get

00:20:26 --> 00:20:29 a um, a tick tock of some

00:20:29 --> 00:20:31 kid doing a stupid raps hole. That's

00:20:31 --> 00:20:34 probably, that's what you'll get from,

00:20:35 --> 00:20:38 from an extraterrestrial intelligence, um.

00:20:38 --> 00:20:40 What, what, what I wonder

00:20:40 --> 00:20:43 is with the far side of the moon? Yes, it's

00:20:43 --> 00:20:45 radio silent, but does it cover enough

00:20:45 --> 00:20:48 of the spectrum of the universe to

00:20:48 --> 00:20:51 pick up something or is it fairly

00:20:51 --> 00:20:53 narrow in its scope?

00:20:53 --> 00:20:56 Professor Fred Watson: Do you mean in terms of direction or.

00:20:56 --> 00:20:58 Andrew Dunkley: Yeah, being able to pick something up.

00:20:58 --> 00:21:00 Professor Fred Watson: Has it got like a wide array? Yeah, I mean

00:21:00 --> 00:21:03 the far side of the moon, um, you know,

00:21:03 --> 00:21:06 if you plunk something on the equator of the

00:21:06 --> 00:21:08 moon on the far side over a month

00:21:08 --> 00:21:11 you cover the entire sky. If you're,

00:21:11 --> 00:21:14 yeah, if you're um, if your

00:21:14 --> 00:21:17 uh, equipment is broadband enough

00:21:17 --> 00:21:20 and all the SETI stuff is, it's got a very

00:21:20 --> 00:21:22 wide range of spectral, of uh, frequencies

00:21:22 --> 00:21:25 although they do tend to concentrate on

00:21:26 --> 00:21:29 what uh, we call the 21 centimetre line. This

00:21:29 --> 00:21:32 is the frequency, the specific frequency

00:21:32 --> 00:21:34 that's radiated by called hydrogen.

00:21:34 --> 00:21:37 Uh and they do tend to concentrate on that

00:21:37 --> 00:21:39 because everybody in the universe will be

00:21:39 --> 00:21:41 aware of that 21 centimetre

00:21:42 --> 00:21:44 uh, wavelength because

00:21:44 --> 00:21:47 that's called hydrogen. Which is the same

00:21:47 --> 00:21:48 everywhere.

00:21:48 --> 00:21:51 Andrew Dunkley: Yeah, makes sense. All right,

00:21:51 --> 00:21:54 fascinating. Um, storey, um, nothing yet.

00:21:54 --> 00:21:56 But that doesn't mean, that doesn't mean

00:21:56 --> 00:21:57 it'll always be nothing.

00:21:57 --> 00:22:00 Professor Fred Watson: So it's not evidence of

00:22:00 --> 00:22:01 absence. That's right.

00:22:01 --> 00:22:04 Andrew Dunkley: M exactly. You can read all about it as

00:22:04 --> 00:22:05 Fred Watson said at the phys

00:22:06 --> 00:22:08 phys.org website,

00:22:08 --> 00:22:11 this is Space Nuts Andrew Dunkley here with

00:22:11 --> 00:22:12 Professor Fred Watson Watson.

00:22:15 --> 00:22:17 Professor Fred Watson: Okay, we checked all four systems and

00:22:17 --> 00:22:19 Andrew Dunkley: being with a go, Space Nuts, our uh,

00:22:19 --> 00:22:22 final storey. Fred Watson brings uh, us back

00:22:22 --> 00:22:25 to that old debate about the Hubble

00:22:25 --> 00:22:28 tension. Now the Hubble tension is measured

00:22:28 --> 00:22:30 in two different ways and they come up with

00:22:30 --> 00:22:33 two different answers. And that's troubled

00:22:33 --> 00:22:36 people for a while. Although we did a storey

00:22:36 --> 00:22:38 not so long ago that suggested. Hang on a

00:22:38 --> 00:22:40 minute, the differences aren't uh, that

00:22:40 --> 00:22:43 significant. So they're probably both right

00:22:43 --> 00:22:46 if you allow for the um, you know, the, the

00:22:46 --> 00:22:49 variables. But this storey is saying.

00:22:49 --> 00:22:51 Hang on a minute, we, we think there's a

00:22:51 --> 00:22:52 better way.

00:22:53 --> 00:22:56 Professor Fred Watson: Yes, that's right. Uh, in

00:22:56 --> 00:22:58 Exactly. That it's all about. So

00:22:59 --> 00:23:02 let's just, uh, backtrack. What is the Hubble

00:23:02 --> 00:23:05 tension? Uh, so the

00:23:05 --> 00:23:07 expansion rate of the universe, uh,

00:23:07 --> 00:23:10 basically is a number that we was

00:23:10 --> 00:23:13 first measured by Edwin hubble back in 1929.

00:23:13 --> 00:23:15 Um, he got the wrong answer because he was

00:23:15 --> 00:23:17 only looking at a very small number of

00:23:17 --> 00:23:20 galaxies. But it comes about because, as

00:23:20 --> 00:23:23 you look at galaxies, ah, in the

00:23:23 --> 00:23:26 wider universe, uh, they get,

00:23:26 --> 00:23:29 um. Their velocity away from us

00:23:29 --> 00:23:31 is bigger the further away they are.

00:23:32 --> 00:23:34 And that comes about when you've got a

00:23:34 --> 00:23:36 universe that's expanding. That's the natural

00:23:36 --> 00:23:39 assumption and we've believed that ever

00:23:39 --> 00:23:41 since. Yeah. Excuse me. So.

00:23:42 --> 00:23:44 So, um, I've got a bit of Hubble tension in

00:23:44 --> 00:23:47 my chest there. Um, so that's how

00:23:47 --> 00:23:50 it's normally measured, measured the Hubble

00:23:50 --> 00:23:52 constant, this number,

00:23:53 --> 00:23:56 which is in slightly bizarre units, it's

00:23:56 --> 00:23:58 in megapas, uh, kilometres per second per

00:23:58 --> 00:24:01 megaparsec. Kilometres per second is

00:24:01 --> 00:24:04 the recession speed of a galaxy.

00:24:04 --> 00:24:06 A megaparsec is,

00:24:07 --> 00:24:09 uh, it 3.26. I can never remember the

00:24:09 --> 00:24:11 name. Million light years.

00:24:12 --> 00:24:14 It's the units that astronomers use for

00:24:14 --> 00:24:17 measuring distance parsecs. And it's a

00:24:17 --> 00:24:20 million parsecs. So, um, kilometres

00:24:20 --> 00:24:23 per second per megaparsec tells you how

00:24:23 --> 00:24:25 the velocity of a galaxy

00:24:25 --> 00:24:28 increases with distance and that's the

00:24:28 --> 00:24:30 result of the expansion of the universe. So

00:24:30 --> 00:24:33 the Hubble constant tells you how fast the

00:24:33 --> 00:24:35 universe is expanding. Now,

00:24:35 --> 00:24:38 now you can. The normal way of

00:24:38 --> 00:24:41 doing this is, uh. And it's actually why the

00:24:41 --> 00:24:44 Hubble telescope was created and why it got

00:24:44 --> 00:24:47 its name. Uh, we. Excuse me, we

00:24:47 --> 00:24:50 measure the brightness. Sorry, I've

00:24:50 --> 00:24:52 got my. Got my tension back there.

00:24:53 --> 00:24:55 If you want to cut this bit out, Huw, you're

00:24:55 --> 00:24:56 more than welcome to,

00:24:58 --> 00:25:01 um. It's fine now, uh,

00:25:02 --> 00:25:05 uh, the tension comes about. So, no, let me

00:25:05 --> 00:25:07 step back again. The measure, uh, where

00:25:07 --> 00:25:10 it's measured is you build up a sort of

00:25:10 --> 00:25:12 distance scale ladder. So the direct

00:25:12 --> 00:25:15 measurement of star distances in outer

00:25:15 --> 00:25:18 space comes about by the parallax

00:25:18 --> 00:25:21 method. As the Earth goes around the sun, we

00:25:21 --> 00:25:24 see stars, uh, apparently changing their

00:25:24 --> 00:25:26 position relative to very distant

00:25:26 --> 00:25:29 background stars. And that changing position

00:25:29 --> 00:25:31 you can measure. Uh, and in fact

00:25:31 --> 00:25:34 it's that. That gives the parsec its name.

00:25:34 --> 00:25:37 It's a parallax of 1/ arc second is what

00:25:37 --> 00:25:39 it's short for. And so that's a direct

00:25:39 --> 00:25:42 geometrical way of measuring the distance to

00:25:42 --> 00:25:44 certain stars. If you can do that to

00:25:44 --> 00:25:47 stars whose intrinsic brightness, you know,

00:25:47 --> 00:25:49 and these are typically, uh, Cepheid variable

00:25:49 --> 00:25:52 stars, then you can extend it because you

00:25:52 --> 00:25:54 know their brightness, uh, their intrinsic

00:25:54 --> 00:25:57 brightness, how much uh, light they radiate,

00:25:57 --> 00:25:59 then you can look at how faint they are

00:25:59 --> 00:26:02 further and further on. Um, and that's the,

00:26:02 --> 00:26:04 that's how we started off because Hubble

00:26:05 --> 00:26:08 measured um, um. In fact in

00:26:08 --> 00:26:11 1923 used these variable stars to

00:26:11 --> 00:26:12 measure the distance of the Andromeda, um,

00:26:12 --> 00:26:15 galaxy. Once again, he got it a bit wrong by

00:26:15 --> 00:26:17 today's standards. But that uh, was when we

00:26:17 --> 00:26:19 realised that galaxies weren't little things

00:26:19 --> 00:26:22 frutaling around in our own Milky Way. They

00:26:22 --> 00:26:25 are very distant objects. So, so that's the

00:26:25 --> 00:26:27 basic process and that has now been

00:26:28 --> 00:26:31 uh, basically elaborated by

00:26:31 --> 00:26:34 additional things which involve supernovae,

00:26:34 --> 00:26:37 the exploding stars, all sorts of other

00:26:37 --> 00:26:40 uh, cosmic phenomena. And that's the

00:26:40 --> 00:26:43 basis of what this storey is about

00:26:43 --> 00:26:46 because uh, that

00:26:46 --> 00:26:48 technology has now been

00:26:49 --> 00:26:51 absolutely refined to the nth degree,

00:26:52 --> 00:26:55 uh, by the scientists who are uh,

00:26:55 --> 00:26:57 uh, who are um, um,

00:26:57 --> 00:27:00 basically reporting this work. It's

00:27:00 --> 00:27:03 a study in astronomy and astrophysics, one of

00:27:03 --> 00:27:05 the leading journals, actually a European

00:27:05 --> 00:27:08 journal. Uh, and these scientists

00:27:08 --> 00:27:10 have spent a lot of time

00:27:11 --> 00:27:14 getting uh, the answer right from

00:27:14 --> 00:27:16 this method, what we call the distance ladder

00:27:16 --> 00:27:19 or the distance scale, by invoking

00:27:19 --> 00:27:22 objects of all kinds. And so they

00:27:22 --> 00:27:24 have produced a number for the Hubble

00:27:24 --> 00:27:27 constant which has a very, very

00:27:28 --> 00:27:30 small error. In fact they quote it as Ah,

00:27:30 --> 00:27:32 73.50

00:27:33 --> 00:27:36 kilometres per second per megaparsec

00:27:36 --> 00:27:39 plus or minus point zero, sorry,

00:27:39 --> 00:27:42 0.81 kilometres per

00:27:42 --> 00:27:44 second per megaset parsec. So they're talking

00:27:44 --> 00:27:47 about something that's either somewhere

00:27:47 --> 00:27:50 between 72.0 and 74. Sorry,

00:27:50 --> 00:27:52 72.5 and 74. 4.5

00:27:52 --> 00:27:55 thereabouts, which is a very, very

00:27:55 --> 00:27:57 tight uh, estimate of this

00:27:57 --> 00:28:00 velocity. Uh, so what's

00:28:00 --> 00:28:03 the tension about until somebody debunks

00:28:03 --> 00:28:06 them? Yeah, uh,

00:28:06 --> 00:28:09 well, it's true. Um, I do remember,

00:28:09 --> 00:28:11 um, back in the 70s, and I've told you this

00:28:11 --> 00:28:14 before, Andrew, there were two schools of

00:28:14 --> 00:28:17 thought, both offering measurements with very

00:28:17 --> 00:28:19 tight error limits, one of which said that

00:28:19 --> 00:28:22 the number was 50 and the other which said

00:28:22 --> 00:28:25 the number was 100. And lo and behold, when

00:28:25 --> 00:28:26 the Hubble telescope gave us the right

00:28:26 --> 00:28:28 answer, it was basically the average of those

00:28:28 --> 00:28:31 two around about 75. And it's now been

00:28:31 --> 00:28:31 refined.

00:28:31 --> 00:28:33 Andrew Dunkley: It's kind of what they're doing with this,

00:28:33 --> 00:28:33 isn't it?

00:28:34 --> 00:28:37 Professor Fred Watson: A little bit. Although they're really giving

00:28:37 --> 00:28:39 tight, very tight

00:28:39 --> 00:28:42 um, estimates based on everything that

00:28:42 --> 00:28:45 we can observe. Uh, whereas the previous

00:28:45 --> 00:28:47 this with the difference between 50 and 100

00:28:47 --> 00:28:49 and that was a kind of Hubble tension. We

00:28:49 --> 00:28:51 didn't call it the ah, that but that's sort

00:28:51 --> 00:28:54 of what it was. That was uh, based on

00:28:54 --> 00:28:57 uh, just individual, individual measurements

00:28:57 --> 00:29:00 from you know, their own particular school of

00:29:00 --> 00:29:02 thought. One was galaxies, one was supernovae

00:29:02 --> 00:29:04 or something. I can't remember how it worked,

00:29:04 --> 00:29:06 I can't remember the details. Probably could

00:29:06 --> 00:29:08 if I thought about it. Uh, but this brings

00:29:08 --> 00:29:11 them all together to get this super accurate

00:29:11 --> 00:29:14 so called value of 73.5.

00:29:14 --> 00:29:17 So the tension is that there is another way

00:29:18 --> 00:29:21 of determining uh, the Hubble

00:29:21 --> 00:29:23 constant and it involves uh, observing

00:29:23 --> 00:29:26 the cosmic microwave background radiation.

00:29:26 --> 00:29:28 That's the radiation that we see from the Big

00:29:28 --> 00:29:31 Bang. We're looking back 13.8 billion years

00:29:31 --> 00:29:33 to see that. What's sometimes called the

00:29:33 --> 00:29:35 afterglow of the Big Bang. It's really still

00:29:35 --> 00:29:37 the light of the Big Bang that you can see

00:29:37 --> 00:29:39 because you're looking so far back in time.

00:29:40 --> 00:29:43 And that gives us a different number. You

00:29:43 --> 00:29:46 can look at the, the, it's what's

00:29:46 --> 00:29:47 called the power spectrum. The cosmic

00:29:47 --> 00:29:49 microwave background radiation has these

00:29:49 --> 00:29:52 tiny, tiny fluctuations and by tiny

00:29:52 --> 00:29:54 I mean the amount fluctuations in

00:29:54 --> 00:29:56 temperature. You can measure the temperature

00:29:56 --> 00:29:59 of the radiation and they form in little

00:29:59 --> 00:30:02 blobs and we think that's where the galaxies

00:30:02 --> 00:30:04 came from. The cooler parts were where

00:30:04 --> 00:30:07 galaxies formed, the warmer parts were not.

00:30:07 --> 00:30:10 Uh, and so the microwave

00:30:10 --> 00:30:12 background radiation when you look at,

00:30:13 --> 00:30:16 looks like a wallpaper, uh, which is

00:30:16 --> 00:30:18 why I sometimes call it the cosmic wallpaper.

00:30:18 --> 00:30:20 Partly because it's behind everything else.

00:30:20 --> 00:30:22 Just like the wallpaper in a room is behind

00:30:22 --> 00:30:25 everything. But it's also got these patterns.

00:30:25 --> 00:30:27 So you can use those patterns to make another

00:30:27 --> 00:30:30 estimate of the uh, Hubble

00:30:30 --> 00:30:30 constant.

00:30:30 --> 00:30:33 And the answer that you get is 67

00:30:33 --> 00:30:36 kilometres per second per megaparsec, which

00:30:36 --> 00:30:39 is well outside the error

00:30:39 --> 00:30:41 band of the sort of traditional method.

00:30:41 --> 00:30:44 Method. And so I think

00:30:44 --> 00:30:47 what the direction this is going

00:30:47 --> 00:30:50 in is. So uh, as you and I have

00:30:50 --> 00:30:53 spoken about before, people have done a lot

00:30:53 --> 00:30:56 of work to try and look for where we've

00:30:56 --> 00:30:58 gone wrong here because these two numbers

00:30:58 --> 00:30:59 should give you the same answer. But they

00:30:59 --> 00:31:02 don't. But they don't. So

00:31:02 --> 00:31:04 now people are turning it upside down and

00:31:04 --> 00:31:06 saying maybe the fact that they don't give

00:31:06 --> 00:31:08 the same answer is telling us something

00:31:08 --> 00:31:10 about, about the physics of the universe that

00:31:10 --> 00:31:11 we don't know

00:31:12 --> 00:31:14 Andrew Dunkley: or we're just not accounting for everything

00:31:14 --> 00:31:16 we need to put into the formula.

00:31:16 --> 00:31:19 Professor Fred Watson: Yeah, yeah there's that too. And, but I think

00:31:19 --> 00:31:22 that's. So as time goes on people are ticking

00:31:22 --> 00:31:24 off all those things uh, simply because

00:31:24 --> 00:31:27 there's a lot more work being done on this

00:31:27 --> 00:31:29 topic. So the Hubble tension could turn out

00:31:29 --> 00:31:32 to be, uh, the gateway

00:31:32 --> 00:31:35 into new physics. That might tell us about

00:31:35 --> 00:31:38 dark matter and dark energy and all the other

00:31:38 --> 00:31:41 dark stuff that we think about. Yeah.

00:31:41 --> 00:31:44 So it's potentially, uh, something

00:31:44 --> 00:31:46 that I think, uh, scientists everywhere will

00:31:46 --> 00:31:49 keep an eye on. But, uh, it is really, um,

00:31:49 --> 00:31:51 really, uh, in many ways getting quite

00:31:51 --> 00:31:53 exciting that this Hubble tension is not

00:31:53 --> 00:31:55 going away. No, definitely not.

00:31:55 --> 00:31:57 Andrew Dunkley: It's come up a few times in the last 10 years

00:31:57 --> 00:31:59 that we've been doing this. So they keep

00:31:59 --> 00:32:01 looking at it and that's. And very good

00:32:01 --> 00:32:04 reasons to do so. Uh, for the record, a

00:32:04 --> 00:32:07 megaparsec is approximately 3.0 million light

00:32:07 --> 00:32:08 years. I think that's what you said.

00:32:08 --> 00:32:10 Professor Fred Watson: It is what I said. Yeah. I could never

00:32:10 --> 00:32:12 remember. I think it's 3.26.

00:32:12 --> 00:32:14 Andrew Dunkley: I thought that's what I found. Yes.

00:32:14 --> 00:32:15 Professor Fred Watson: Yeah. Very good.

00:32:16 --> 00:32:18 Andrew Dunkley: All right, uh, hopefully they've finally

00:32:18 --> 00:32:20 cracked the Hubble tension debate. Uh, I

00:32:20 --> 00:32:22 guess we'll find out if they keep coming up

00:32:22 --> 00:32:24 with different numbers in, in the future.

00:32:24 --> 00:32:26 But, uh, you can look it up@, uh,

00:32:26 --> 00:32:28 dailygalaxy.com or you can read the

00:32:28 --> 00:32:30 published paper at Astronomy and

00:32:30 --> 00:32:31 Astrophysics.

00:32:32 --> 00:32:34 Fred Watson, that brings us to the end of the

00:32:34 --> 00:32:35 programme. Thank you so much.

00:32:36 --> 00:32:38 Professor Fred Watson: A great pleasure, Andrew. Uh, we've covered

00:32:38 --> 00:32:41 some great topics today and, uh, it's always

00:32:41 --> 00:32:42 a delight.

00:32:42 --> 00:32:45 Andrew Dunkley: Yeah, it's very. A few different types of

00:32:45 --> 00:32:47 storeys this time around, which we like.

00:32:48 --> 00:32:49 We'll catch you on the next one, Fred Watson.

00:32:50 --> 00:32:52 Professor Fred Watson: I guess we will. Yes. Sounds good.

00:32:52 --> 00:32:54 Andrew Dunkley: Professor Fred Watson Watson, astronomer at

00:32:54 --> 00:32:56 large. And thanks to Huw in the studio. He

00:32:56 --> 00:32:58 couldn't be with us today because he caused a

00:32:58 --> 00:33:01 bit of, of hubby tension at home

00:33:03 --> 00:33:04 and he's been sent to the naughty corner.

00:33:05 --> 00:33:08 Don't, uh, forget to visit us online or, um,

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00:33:10 --> 00:33:12 forget to send us your comments and questions

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00:33:13 --> 00:33:16 nutspodcast.com or

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00:33:19 --> 00:33:21 reviews from your favourite podcasting

00:33:21 --> 00:33:23 platform in the meantime, from me, Andrew

00:33:23 --> 00:33:24 Dunkley. Thanks for your company. We'll see

00:33:24 --> 00:33:27 you on the very next episode of Space Nuts.

00:33:27 --> 00:33:27 Professor Fred Watson: Bye. Bye.

00:33:28 --> 00:33:31 Andrew Dunkley: You've been listening to the Space Nuts

00:33:31 --> 00:33:34 podcast, available at

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00:33:42 --> 00:33:44 Professor Fred Watson: this has been another quality podcast

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