Europa's Ocean Secrets, Gravitational Waves & Black Hole Mysteries
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Archived Insights: Europa Clipper, Gravitational Waves, and Black Hole Mysteries
In this special episode of Space Nuts, hosts Andrew Dunkley and Professor Fred Watson take a fascinating journey through some of the most compelling questions and discoveries in astronomy. As they explore the Europa Clipper mission, the nature of gravitational waves, and the enigmatic world of black holes, listeners are treated to a rich tapestry of cosmic knowledge. This episode originally aired in 2019.
Episode Highlights:
- Europa Clipper Mission: Andrew and Fred discuss NASA's exciting approval for the Europa Clipper mission, aimed at exploring Jupiter's icy moon Europa. They delve into the spacecraft's objectives, including investigating the moon's potential subsurface ocean and the challenges posed by Jupiter's intense radiation.
- Gravitational Waves Explained: The hosts explore the recent detection of gravitational waves, speculating on their origins, including a possible black hole-neutron star merger. They discuss the significance of these findings and the ongoing efforts of astronomers to understand the universe's most violent events.
- Black Hole Chris: Listener questions about the nature of black holes spark a lively discussion on topics such as infinite density, event horizons, and the complexities of capturing images of these cosmic phenomena. Andrew and Fred clarify misconceptions and provide insightful explanations.
- Space Travel and Relativity: The episode wraps up with an intriguing listener question about the effects of traveling near the speed of light. Andrew and Fred clarify how relativistic mass works and dispel myths surrounding the transformation of spaceships into black holes.
For more Space Nuts, including our continuously updating newsfeed and to listen to all our episodes, visit our website. Follow us on social media at SpaceNutsPod on Facebook, X, YouTube Music Music, Tumblr, Instagram, and TikTok. We love engaging with our community, so be sure to drop us a message or comment on your favorite platform.
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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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Andrew Dunkley: Hi, Andrew Dunkley here. Fred and I are
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taking a little bit of a break over the
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Christmas New Year period just to catch our
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breath. We'll be back, uh, sometime around
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mid January. In the meantime, we've been
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digging through the archives at some of the
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most perplexing and popular
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episodes that we've done in recent times. So
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sit back and enjoy. 15
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seconds. Guidance is internal.
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Professor Fred Watson: 10, 9. Ignition
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sequence start. Space nets.
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Andrew Dunkley: 5, 4, 3.
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Professor Fred Watson: 2. 1, 2, 3, 4, 5, 5, 4, 3,
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2, 1.
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Andrew Dunkley: Space nuts astronauts report it feels
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good. Hi there and thanks for joining us on
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the Space Nuts podcast. My name's Andrew
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Dunkley, your host. And joining me, uh, as
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always, Professor Fred Watson, Astronomer at
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Large from the department of Da da da da da
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da da. It's a pretty long title. That's what
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we'll call it from now on. G', day, Fred.
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Professor Fred Watson: You could call me the Aaliyah.
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Andrew Dunkley: Aal.
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Professor Fred Watson: Yeah, when I was Astronomer in Charge, I was
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aic. Um, the only trouble is
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AAL actually has another significant
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meaning in Australian astronomy because it
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doesn't only stand for Astronomer at Large,
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it also stands for Astronomy Australia
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Limited. So, uh, just throw that idea out.
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That's a rubbish idea. I'll just be
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astronomer.
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Andrew Dunkley: Yeah, I was once given the title urrs.
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But anyway, um,
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some people will understand that.
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Professor Fred Watson: Yeah, you've got lovely friends, haven't you?
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Andrew Dunkley: I've got a lot of good friends, yes.
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Now today we're going to talk about some very
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exciting things. It looks like black holes
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are still in people's minds. So we're going
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to be talking about, um, a couple of
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questions that have come in from people about
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infinite density. Uh, density. I
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keep getting it mixed up with destiny. I
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don't know why. Might have been a Back to the
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Future movie that confused me on that front.
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Uh, uh, and issues, uh, photographing a black
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hole. Why were they issues at all? And uh,
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another question about space travel and uh,
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near light speed travel. Uh, we're also
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going to, uh, look at,
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um, the cause of a gravitational
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wave that was detected recently. This is
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exciting because they think they've
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pinpointed, uh, an actual cause.
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And we're going to start off today.
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Professor Fred Watson: Fred, by talking about, uh, this rather.
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Andrew Dunkley: Exciting mission that's one step closer to
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happening. A mission to Jupiter's ice
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moon Europa. And that's what we'll start
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with. This, uh, well, this afternoon, this
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morning, tonight, this evening, yesterday.
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Professor Fred Watson: Whenever. Whenever it is. Yeah, it's,
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yeah. So look, a terrific story. Very good
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news from uh, NASA that they,
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um, the powers that be within NASA have uh,
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given the go ahead um, for a
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mission called Europa Clipper, which is, is
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one of the uh, missions that's been
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uh, postulated or sorry proposed is a better
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word for um, exploring the moons of the outer
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planets. There are a number that are kind of
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on the, on the table at the moment, some
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further advanced than others. But Europa
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Clipper is pretty well advanced and
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as you can tell its target, its main target
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is Jupiter's moon Europa, which is one of
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these um, ocean moons. Ice, uh,
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ocean moons. Uh, we believe it has
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a covering of ice and we don't know whether
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it's thin ice or thick ice. So that would be
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one of the things that Europa Clipper would
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find out. Um, and an ocean underneath it
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and a rocky core. Uh, so
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Europa Clipper, I think they are
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talking about having it ready for launch in
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2023 which is
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um, you know, fantastic if they can
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do that. That's right. Uh, but apparently
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um, that's the
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baseline commitment as it's called, supports
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a launch readiness date by 2025.
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Um, it's all being done at ah, the Propulsion
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Laboratory in Pasadena. That's where the
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spacecraft will be built. So they've got the
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go ahead, um, it's
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got the next step,
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uh, in approval from NASA, which
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I think is a pretty solid one. So I
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think you and I, back in 2025
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we'll be talking a lot about Europa Clipper.
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Andrew Dunkley: Maybe what will be the
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basis of the mission? Are they just going
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there to have a look?
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Professor Fred Watson: Because it is a bit like uh, but it's
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a very good look. Um, so it's not going to
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land on Europa. It is a proposal to go into
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orbit around Europe, actually to go into
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orbit around Jupiter. Uh and of course
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orbiting Jupiter is always hazardous because
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of um, the
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intense uh, radiation belts that Jupiter
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has. It's got a magnetic field thousands of
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times bigger than the Earth and has these
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high energy radiation belts around it that
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threaten to melt the innards of spacecraft.
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Uh, so like the uh, Juno mission which
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is currently in orbit around Jupiter, this
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uh, Europa Clipper will go into a very
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elongated uh, orbit, um, which
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will uh, give it 45
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flybys of Europa. Uh and
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their altitudes will vary from
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2700km to 25km.
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So it will really be skimming over the
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surface. Oh well, and it's got this huge
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science package with all the kind of,
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you know, the gubbins that you would expect
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to find on board something like that,
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a mass spectrometer, uh, which
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basically measures, you know the weights
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of atoms, as you might guess. Uh,
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it, um, that is interesting because
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Europa, like Saturn's moon Enceladus,
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is thought to have, although it hasn't really
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been properly confirmed, but thought to have
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ice, uh, fountains coming out of
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it, um, which are water that's
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squirting up through its, uh, through its icy
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shell and instantly freezing. It's not
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frozen. But if you fly through it, as
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Cassini did with Enceladus, then you can
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sample what the atomic makeup is. And so
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the mass spectrometer will help with that.
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Uh, and also, um, it's got this ground
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penetrating radar and that's going to be
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crucial in characterizing
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Europa's crust, um, and
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revealing how much of, you know, the
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potential water within is oceanic, as
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is expected, uh, or whether it is just
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pockets of water as we find in Antarctica
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and indeed around the South Pole of Mars.
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Andrew Dunkley: Will they be able to tell what kind of water
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it is?
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Professor Fred Watson: Um, uh, to some
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extent they will. Um, it may
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require a bit of, you know,
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inference from other measurements, but if
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you've got, uh, samples of ice crystals,
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uh, then you can do exactly that. You can,
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you know, you can uh, basically
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tell whether it's saline water or fresh water
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because you can see the, you can measure the
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salt content of it.
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Andrew Dunkley: It.
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Professor Fred Watson: So like um, Saturn's moon
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Enceladus, uh, which is actually quite
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rich in minerals and it's the silicates in
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that that tells you that this water was once
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in contact with rock. Uh, I think
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the Europa Clipper will be able to sample
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exactly those things too. Assuming these
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plumes are real, because they're not
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well observed. There is evidence. I've seen
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images that seem to show these plumes
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coming from Europa. Uh, assuming they're real
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when they fly through, um, hopefully we will
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be able to tell what kind of water it is.
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Exactly.
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Andrew Dunkley: And will they be able to tell how much
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water there is underneath the surface?
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Professor Fred Watson: Yes they will because that will very
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much be revealed by the um, the ground
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penetrating radar in exactly the way
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that, um, um, one of the spacecraft in orbit
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around Mars, I think it was the, I think it
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was, might even have been Mars Reconnaissance
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Orbiter, I'm not sure, detected this
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lake of liquid water underneath the ice cap
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of the southern ice cap of Mars about a year
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ago you and I spoke about it. Um, and
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they can tell exactly how much there is there
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because you can see the boundary with this
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sort of radar. You can see the boundary
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between an ice surface and a water surface.
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And that's crucial to doing this so.
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Andrew Dunkley: This mission won't actually be looking
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for life, but it will be looking
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for, uh, the potential for life
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to perhaps exist on a moon
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like this.
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Professor Fred Watson: Exactly. So as the blurb,
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um, on the NASA website says, uh, it
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will help scientists investigate the chemical
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makeup of Europa's potentially habitable
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environment while minimizing the need to
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drill through layers of ice so that what
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they're going to try and do is as much as
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they can from orbit. Um, and
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then if there's like, if they find
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lipids and amino acids and all this sort of
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thing, uh, in the plumes of ice coming,
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coming from Europa, then clearly the next
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step will be a lander, uh, that starts
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digging holes in the ice.
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Andrew Dunkley: Yes.
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Professor Fred Watson: I mean, you know, before you do that, the
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first thing you need to know is how thick the
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ice is. Yes.
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Andrew Dunkley: If it's a couple of miles thick.
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Professor Fred Watson: Well, actually, a couple of miles
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is better than what they're expecting.
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Andrew Dunkley: Oh, is that right?
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Professor Fred Watson: More like 25 or 30 miles
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or kilometers. M. That's right. Choose your
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units. Um, yes. So, yes,
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a thinner layer of ice will be
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pretty, pretty, um, good to, you know, to
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cope with. You could probably do that. I mean
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by thin, I mean less than a kilometer,
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probably. Yes.
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Andrew Dunkley: But the likelihood, uh, is it's, it's
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probably more, but I guess we'll, we'll have
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to wait and see.
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Professor Fred Watson: Um, Europa's covered in all these cracks that
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are, that are brownish in color.
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Andrew Dunkley: Yes.
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Professor Fred Watson: That's thought to be the effect of sunlight
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on brine, on basically on salt water. So
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you've already got a hint there that, uh,
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it's probably a salty ocean underneath the
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surface.
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Andrew Dunkley: Well, salt's probably not that uncommon in
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the universe really.
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Professor Fred Watson: Um, that's right. It's not.
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Andrew Dunkley: It's one of, one of the base materials, isn't
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it? Uh, of course, this doesn't guarantee
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they're actually going to go. This is just
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another step forward in the approval process.
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Professor Fred Watson: It does, it does.
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Andrew Dunkley: Very longitudinal process and they have to
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get over a lot of hurdles before they
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actually hit the launch button. So, uh,
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hopefully they're, um, they're going to get
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there and um, it's. It's a long trip too.
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Professor Fred Watson: Yes, it is. That's the other thing.
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Andrew Dunkley: So they've got to time it right. They've got
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to get in the right place at the right time.
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Professor Fred Watson: Exactly. All of the above. That's right. So,
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uh, at least what it, you know, at least, uh,
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it's not a knockback. That's the good news.
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Andrew Dunkley: Indeed. All right, well, we'll keep an eye on
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this story because I'm sure there'll be more
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to report in the not too distant future about
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uh, a mission to Europa. You're listening
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00:10:48.440 --> 00:10:51.080
to Space Nuts with Andrew Dunkley and Fred
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00:10:51.080 --> 00:10:51.720
Watson.
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Professor Fred Watson: Space Nuts.
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Andrew Dunkley: Now Fred, we've uh, discussed
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00:12:51.860 --> 00:12:54.410
uh, gravitational waves before and
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uh, a few of those have been detected in
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recent times. The problem with them
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is what is the cause?
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And now in a recently detected
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gravitational wave they think they've got a
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candidate.
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Professor Fred Watson: That's, that's right. This is so this is, you
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know, it's a, an ongoing story. Uh,
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what I like about this story is it's got a
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nice Australian component because there is
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um, there's a, basically
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a collaboration here in Australia which is
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called osgrav, uh, which is about
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gravitational waves. It's a kind of fairly
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predictable name but um, it includes people
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from the Australian National University and
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I think University of Western Australia Other
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places which are strong in gravitational wave
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astronomy. So, um, it's very nice
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that it's. It has this Australian component.
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So what's the story? Well, uh, the large.
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Sorry, uh, the Laser Interferometer
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Gravitational Wave Observatory, Otherwise
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known as LIGO, um, has been operating
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since, uh, 2015 in its
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sort of current state. It's actually
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technically called Advanced LIGO because I
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think it took 15 years of development to get
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to this stage. But they have,
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uh, now, not quite regularly, but at, uh,
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fairly infrequent intervals. Sorry,
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fairly moderately moderate intervals.
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Let me put it that way. They've been
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detecting gravitational wave events. And for
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the last couple of years they've had an
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additional string to their bow. Remember,
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there are two of these detectors at opposite
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corners of the United States,
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um, which, um, you need because,
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uh, otherwise you've got no idea where these
355
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things come from or even if they're real. You
356
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need to see the gravitational wave pass one
357
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and then the other with the right kind of
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time interval in between. Um, but they've
359
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been joined in the last few years by
360
00:14:44.970 --> 00:14:47.770
something called, uh, uh, Virgo, which,
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uh. In fact, I think it's called Advanced
362
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Virgo. Like Advanced ligo. Virgo is an
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Italian gravitational wave detector. And of
364
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course, having three detectors widely spread
365
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over the surface of the Earth, uh, means you
366
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can pinpoint things much more accurately in
367
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terms of the direction in which these
368
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gravitational waves come in.
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Andrew Dunkley: From triangulating the signal.
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00:15:07.200 --> 00:15:09.280
Professor Fred Watson: Exactly. That's exactly what it is.
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Um, what's interesting about this one though,
372
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is that the signal seems to be
373
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from a black hole absorbing
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a neutron star.
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Um, we actually had a false alarm on
376
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this, which is embarrassing because, um, my
377
00:15:27.240 --> 00:15:29.200
book has just gone to the printer saying,
378
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yes, we've observed a neutron star being
379
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absorbed by a black hole. Um, and
380
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that I think disappeared because it turned
381
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out to be, um, terrestrial noise. It was
382
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sort of, you know. So I don't know whether it
383
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was a train going underneath oven probably,
384
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or. Yeah, something like that. That's the
385
00:15:46.140 --> 00:15:48.780
usual story, isn't it? A microwave oven. Um,
386
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that was earlier this year. And that,
387
00:15:51.540 --> 00:15:54.300
um, has now gone away. But it looks as
388
00:15:54.300 --> 00:15:57.300
though this one might actually be the
389
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real thing. A black hole and a neutron star.
390
00:16:00.220 --> 00:16:02.860
We've had two black holes merging. Uh,
391
00:16:03.930 --> 00:16:06.170
that's probably been the commonest source of,
392
00:16:06.200 --> 00:16:07.730
uh, gravitational waves. There've been
393
00:16:07.730 --> 00:16:09.570
several of those. We've had a couple of
394
00:16:09.570 --> 00:16:12.090
neutron stars merging as well. And that
395
00:16:12.090 --> 00:16:14.570
actually comes with celestial fireworks that
396
00:16:14.650 --> 00:16:17.490
you can observe with other types of
397
00:16:17.490 --> 00:16:19.850
telescope like neutrino telescopes, visible
398
00:16:19.850 --> 00:16:22.250
light telescopes, radio Telescopes, X ray
399
00:16:22.250 --> 00:16:25.050
telescopes, all of the above. Um, and
400
00:16:25.050 --> 00:16:27.730
that was a big story actually late last year
401
00:16:27.730 --> 00:16:30.570
if I remember rightly. But, um, until
402
00:16:30.570 --> 00:16:32.250
now we haven't had a confirmed,
403
00:16:33.670 --> 00:16:36.250
um, observation of a neutron star
404
00:16:36.490 --> 00:16:38.290
being absorbed by a black hole. And we still
405
00:16:38.290 --> 00:16:41.050
don't have. It's still a bit speculative,
406
00:16:41.370 --> 00:16:44.210
but from the masses that are inferred by the
407
00:16:44.210 --> 00:16:45.930
signal. And remember what you get is this
408
00:16:45.930 --> 00:16:48.430
weird gravitational chirp, uh,
409
00:16:48.430 --> 00:16:51.370
it's uh, the frequency of a sound wave
410
00:16:51.370 --> 00:16:54.330
going as the two things come
411
00:16:54.330 --> 00:16:56.850
together. Um, and it's that. That gives you
412
00:16:56.850 --> 00:16:58.920
all the details of what it is that that are
413
00:16:58.920 --> 00:17:01.480
colliding. The suspicion is it's two
414
00:17:01.480 --> 00:17:04.080
objects, one of which is three solar
415
00:17:04.080 --> 00:17:06.880
masses and the other is five
416
00:17:07.200 --> 00:17:10.000
solar masses. I think I'm right in saying
417
00:17:10.000 --> 00:17:12.560
that I should uh, check those numbers. But
418
00:17:12.560 --> 00:17:15.440
anyway, uh, that is the current
419
00:17:16.080 --> 00:17:18.960
expectation, uh, of what is colliding. So
420
00:17:19.040 --> 00:17:21.880
something three solar masses would have to
421
00:17:21.880 --> 00:17:24.000
be a neutron star because it's two
422
00:17:24.959 --> 00:17:27.519
lightweight uh, to be a black hole.
423
00:17:27.599 --> 00:17:30.239
And so, uh, that is what's making this
424
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interesting. What's
425
00:17:32.799 --> 00:17:35.359
perhaps, um, a bit surprising,
426
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uh, is that
427
00:17:38.719 --> 00:17:40.879
you might expect there to be once again
428
00:17:41.279 --> 00:17:43.639
radiation, uh, coming from this, not just
429
00:17:43.639 --> 00:17:46.639
gravitational radiation, but uh, noise
430
00:17:46.639 --> 00:17:49.050
in the X ray spectrum or uh,
431
00:17:49.050 --> 00:17:51.999
neutrinos, uh, particles, things of that
432
00:17:51.999 --> 00:17:54.650
sort, but it hasn't been
433
00:17:54.810 --> 00:17:57.250
observed. And um,
434
00:17:57.610 --> 00:17:59.930
one of the Australian astronomers, uh,
435
00:18:00.610 --> 00:18:02.170
uh, I've forgotten her first name. That's
436
00:18:02.170 --> 00:18:04.730
embarrassing, isn't it? Susan. Susan Scott.
437
00:18:04.910 --> 00:18:07.690
Uh, she's at um, anu Australian
438
00:18:07.690 --> 00:18:10.250
National University. Uh, she says that
439
00:18:10.650 --> 00:18:13.610
uh, if she said. Well
440
00:18:13.610 --> 00:18:15.090
what she says is we've looked for light
441
00:18:15.090 --> 00:18:16.930
signatures of the event, but no one has found
442
00:18:16.930 --> 00:18:19.490
any up to this point. That indicates that if
443
00:18:19.490 --> 00:18:22.290
it is a black hole and a neutron star, then
444
00:18:22.290 --> 00:18:24.690
very likely the neutron star has been
445
00:18:24.690 --> 00:18:27.370
swallowed whole by, by the black hole. Uh,
446
00:18:27.450 --> 00:18:29.750
uh, he said, and she says this could happen
447
00:18:29.750 --> 00:18:32.310
if the objects were of different masses.
448
00:18:32.870 --> 00:18:35.550
So it's. The smaller object gets sucked in
449
00:18:35.550 --> 00:18:37.590
more quickly and, and is swallowed whole. So
450
00:18:37.590 --> 00:18:40.390
you know, it's not strung out into, into this
451
00:18:41.410 --> 00:18:44.230
um, mess of material that does emit
452
00:18:44.490 --> 00:18:46.590
um, uh, signals in the
453
00:18:46.590 --> 00:18:49.100
electromagnetic uh, wave bands. Uh,
454
00:18:49.270 --> 00:18:52.070
if it gets sucked in hole, maybe you don't
455
00:18:52.070 --> 00:18:53.870
get any signal at all except for the
456
00:18:53.870 --> 00:18:55.070
gravitational wave signal.
457
00:18:55.070 --> 00:18:56.870
Andrew Dunkley: It's extraordinary how sudd
458
00:18:58.210 --> 00:19:01.050
impact be. I mean, you know, neutron
459
00:19:01.050 --> 00:19:03.330
stars, we've talked about them and they're
460
00:19:03.330 --> 00:19:05.890
pretty volatile individuals and
461
00:19:06.130 --> 00:19:08.590
quite dense, um,
462
00:19:08.850 --> 00:19:09.570
quite dense.
463
00:19:09.730 --> 00:19:11.890
Professor Fred Watson: It's just a slight understatement there.
464
00:19:12.770 --> 00:19:13.570
Yes, indeed.
465
00:19:13.930 --> 00:19:16.850
Andrew Dunkley: Um, so I imagine
466
00:19:16.850 --> 00:19:19.010
it'd be quite a cataclysmic collision.
467
00:19:19.170 --> 00:19:22.130
Professor Fred Watson: Yeah, that's right. Um, in fact, so
468
00:19:22.130 --> 00:19:25.090
when you've got two black holes, um, what you
469
00:19:25.090 --> 00:19:27.010
get at the end of it is a more massive black
470
00:19:27.010 --> 00:19:30.010
hole. Uh, and, um, you're
471
00:19:30.010 --> 00:19:32.850
talking there though about, you
472
00:19:32.850 --> 00:19:35.330
know, infinitely small, infinitesimally small
473
00:19:35.330 --> 00:19:38.330
points merging, uh, their event horizon.
474
00:19:38.890 --> 00:19:41.210
There are two event horizons merge as well,
475
00:19:41.210 --> 00:19:42.890
and you get something called the ring down
476
00:19:42.890 --> 00:19:45.130
where the event horizon itself vibrates.
477
00:19:45.810 --> 00:19:48.690
Um, I think with a neutron star you wouldn't
478
00:19:48.690 --> 00:19:51.020
have the event horizon, but it will be
479
00:19:51.020 --> 00:19:53.380
possible for the neutron star just basically
480
00:19:53.380 --> 00:19:55.100
to disappear. Over the black holes event
481
00:19:55.100 --> 00:19:57.210
horizon, you don't see anything. But, uh,
482
00:19:57.340 --> 00:19:59.260
neutron stars themselves, as you and I have
483
00:19:59.260 --> 00:20:01.020
talked about many times, are active in the
484
00:20:01.020 --> 00:20:02.900
sense that they've got highly intense
485
00:20:02.900 --> 00:20:05.580
magnetic fields on their surfaces and they
486
00:20:05.580 --> 00:20:07.940
beam this radiation out, which we see as
487
00:20:08.260 --> 00:20:11.060
pulsars. So they're not particularly
488
00:20:11.060 --> 00:20:13.700
quiet things. I mean, this thing could be a
489
00:20:13.700 --> 00:20:16.220
pulsar whose lighthouse beam of
490
00:20:16.220 --> 00:20:19.180
radiation is missing the Earth, if I can put
491
00:20:19.180 --> 00:20:21.300
it that way. Because the only reason we see
492
00:20:21.300 --> 00:20:23.380
pulsars is when you've got a neutron star
493
00:20:23.780 --> 00:20:26.540
whose, uh, beams of radiation from their
494
00:20:26.540 --> 00:20:28.780
poles actually sweeps across the Earth. And
495
00:20:28.780 --> 00:20:30.810
that of course, is a particular, uh,
496
00:20:30.820 --> 00:20:33.780
circumstance. Maybe this one wasn't like
497
00:20:33.780 --> 00:20:36.340
that and it's just got chewed up, uh, and
498
00:20:37.220 --> 00:20:40.140
we haven't seen its demise other than in
499
00:20:40.140 --> 00:20:41.380
the gravitational waves.
500
00:20:41.380 --> 00:20:43.140
I think there'll be more about this story,
501
00:20:43.220 --> 00:20:45.460
Andrew, and, um, I hope you and I can bring
502
00:20:45.460 --> 00:20:48.140
it to our, uh, Space Nuts
503
00:20:48.140 --> 00:20:50.950
listeners or listeners, our fraternity.
504
00:20:52.390 --> 00:20:54.810
Andrew Dunkley: Yes, uh, well, um,
505
00:20:55.590 --> 00:20:58.310
the more we can gather in terms of data,
506
00:20:58.550 --> 00:21:01.230
uh, on gravitational waves, the more we
507
00:21:01.230 --> 00:21:04.190
will learn and who knows what
508
00:21:04.190 --> 00:21:05.790
sort of problems it could solve down the
509
00:21:05.790 --> 00:21:06.470
track, so.
510
00:21:06.950 --> 00:21:09.310
Professor Fred Watson: Exactly. It's always my comment that you
511
00:21:09.310 --> 00:21:12.110
never know what you're setting in store for
512
00:21:12.110 --> 00:21:13.670
the future from all this knowledge.
513
00:21:13.830 --> 00:21:14.430
Andrew Dunkley: Exactly.
514
00:21:14.430 --> 00:21:14.790
Professor Fred Watson: Yeah.
515
00:21:14.790 --> 00:21:16.450
Andrew Dunkley: I, uh, mean, you just, just gather the
516
00:21:16.450 --> 00:21:18.430
knowledge. One day it might just go, you, ah,
517
00:21:18.570 --> 00:21:20.250
know, a penny will drop with someone else,
518
00:21:20.250 --> 00:21:23.050
maybe a generation down the track, who knows?
519
00:21:23.370 --> 00:21:25.970
It's all useful. And even if it's not, it's
520
00:21:25.970 --> 00:21:28.930
good to be able to gather it and they
521
00:21:28.930 --> 00:21:29.850
use it. Some, some.
522
00:21:29.850 --> 00:21:32.730
Professor Fred Watson: That's right. It's um, you know, all these
523
00:21:32.730 --> 00:21:34.770
things are constantly testing Einstein's
524
00:21:34.770 --> 00:21:36.890
theory of relativity. And that's
525
00:21:38.010 --> 00:21:39.730
very, um, important because we know there's
526
00:21:39.730 --> 00:21:41.050
something wrong with it, but we haven't found
527
00:21:41.050 --> 00:21:43.050
anything wrong with it yet. Even though it's
528
00:21:43.050 --> 00:21:45.250
been tested within an inch of its life, it's
529
00:21:45.250 --> 00:21:46.620
still holds up.
530
00:21:46.940 --> 00:21:48.140
Andrew Dunkley: Yeah, fascinating.
531
00:21:48.140 --> 00:21:51.100
All right, you're listening to the Space Nuts
532
00:21:51.100 --> 00:21:54.060
podcast With Andrew Dunkley and Fred Watson.
533
00:21:56.380 --> 00:21:58.860
Professor Fred Watson: Okay, we checked all four systems and being
534
00:21:58.860 --> 00:22:00.300
with a girl, Space Nuts.
535
00:22:00.300 --> 00:22:02.500
Andrew Dunkley: Now Fred, I do want to shout out once again
536
00:22:02.500 --> 00:22:05.380
to our patrons, um, that number
537
00:22:05.380 --> 00:22:08.260
39 now thank uh, you so
538
00:22:08.260 --> 00:22:10.420
much for supporting the Space Nuts podcast.
539
00:22:10.420 --> 00:22:13.020
We so appreciate it. And if you're interested
540
00:22:13.020 --> 00:22:14.920
in becoming a patron, you can, can do
541
00:22:14.920 --> 00:22:17.920
so@patreon.com spacenuts
542
00:22:17.920 --> 00:22:19.400
that's patreon.com
543
00:22:20.520 --> 00:22:23.240
spacenuts and um, thank you to
544
00:22:23.240 --> 00:22:25.720
everybody who has joined the Space Nuts
545
00:22:25.720 --> 00:22:28.400
podcast group. They number in their hundreds.
546
00:22:28.400 --> 00:22:31.360
Now Fred, we've only had the page going for
547
00:22:31.360 --> 00:22:33.920
a bit over a week and uh, already we've
548
00:22:33.920 --> 00:22:35.880
tracked the century and
549
00:22:36.760 --> 00:22:39.400
have over 100 people that are all Space Nuts
550
00:22:39.400 --> 00:22:41.440
fans who are all now talking to each other
551
00:22:41.440 --> 00:22:43.580
and uh, answering each other's questions and,
552
00:22:43.730 --> 00:22:46.690
and uh, having a fair bit of fun. So I'm
553
00:22:46.690 --> 00:22:49.410
so pleased we were able to put um, those
554
00:22:49.410 --> 00:22:51.410
people together and who uh, knows friends,
555
00:22:51.570 --> 00:22:54.530
friendships may be forged. Uh, that's
556
00:22:54.530 --> 00:22:56.610
great. Or collaborations that might solve
557
00:22:56.610 --> 00:22:58.210
some of the mysteries of the universe. Who
558
00:22:58.210 --> 00:23:01.010
knows, uh, that would be a lovely legacy I
559
00:23:01.010 --> 00:23:03.970
think. Uh, let's um, and of course if
560
00:23:03.970 --> 00:23:06.410
you would like to be a member uh, of the
561
00:23:06.410 --> 00:23:09.110
Space Nuts podcast group, um, just find it,
562
00:23:09.180 --> 00:23:11.780
it, it's on Facebook, uh, Space Nuts podcast
563
00:23:11.780 --> 00:23:14.380
group in your search engine and um, yes, just
564
00:23:14.380 --> 00:23:17.060
ask to join and we will click the approve
565
00:23:17.060 --> 00:23:19.780
button. Everybody seems to be like minded and
566
00:23:19.780 --> 00:23:21.660
enjoying themselves. So uh, that's what it's
567
00:23:21.660 --> 00:23:22.060
all about.
568
00:23:23.500 --> 00:23:26.460
Now Fred, some questions if you
569
00:23:26.460 --> 00:23:29.380
will. Um, hello again fellow nutters.
570
00:23:29.380 --> 00:23:31.340
I have a question I'm hoping you can help me.
571
00:23:31.500 --> 00:23:33.860
Um, understanding an old
572
00:23:33.860 --> 00:23:36.780
chestnut black holes. If a black hole is
573
00:23:36.780 --> 00:23:39.380
an infinite dense point, why does it have a
574
00:23:39.380 --> 00:23:42.240
diameter? I don't why astronomers refer
575
00:23:42.240 --> 00:23:44.400
to black holes by their size in terms of
576
00:23:44.400 --> 00:23:46.240
diameter. When it's meant to be a point of
577
00:23:46.240 --> 00:23:48.960
infinite density, are they
578
00:23:48.960 --> 00:23:51.560
mistakenly referring to the event horizon?
579
00:23:51.560 --> 00:23:54.440
Mario from Melbourne. Hello Mario. Thanks for
580
00:23:54.440 --> 00:23:54.840
the question.
581
00:23:55.720 --> 00:23:57.880
Professor Fred Watson: And the answer is yes, thank you Mario.
582
00:23:57.880 --> 00:23:58.760
Andrew Dunkley: Thanks for the question.
583
00:23:59.420 --> 00:24:02.320
Professor Fred Watson: Um, Mario then goes on to uh, you
584
00:24:02.320 --> 00:24:05.000
know, everything he says is absolutely right,
585
00:24:05.000 --> 00:24:07.850
that um, uh, if you've got a, a
586
00:24:07.850 --> 00:24:10.170
point of infinite density, it's got zero
587
00:24:10.250 --> 00:24:12.970
dimensions, so you can't refer to its
588
00:24:12.970 --> 00:24:15.890
diameter. Uh, what you can refer to is
589
00:24:15.890 --> 00:24:18.560
its mass because the mass is uh,
590
00:24:19.050 --> 00:24:21.970
variable. Uh, but the fact that
591
00:24:21.970 --> 00:24:24.930
it has no volume means that when you, you
592
00:24:24.930 --> 00:24:26.450
know, when you look at the mass per unit
593
00:24:26.450 --> 00:24:27.970
volume, you've got something of infinite
594
00:24:27.970 --> 00:24:30.330
density, which is how density is defined.
595
00:24:30.650 --> 00:24:33.530
So Mario is absolutely right. Uh, what
596
00:24:33.530 --> 00:24:36.170
does vary though? With the maps is the event
597
00:24:36.170 --> 00:24:38.290
horizon, the diameter of the event horizon,
598
00:24:38.290 --> 00:24:40.920
which you and I have spoken before. Um,
599
00:24:41.360 --> 00:24:44.150
uh, uh, it's a
600
00:24:44.150 --> 00:24:47.110
quantity that I suppose is
601
00:24:47.190 --> 00:24:49.990
important because if we are observing,
602
00:24:50.380 --> 00:24:52.910
um, a black hole, as we did with the Event
603
00:24:52.910 --> 00:24:54.790
Horizon telescope, then that's what you see.
604
00:24:55.300 --> 00:24:56.870
Uh, so a big one is going to be easier to
605
00:24:56.870 --> 00:24:58.630
observe than a smaller one. And that's why a
606
00:24:58.630 --> 00:25:00.950
supermassive black hole, uh, in the center of
607
00:25:00.950 --> 00:25:03.590
a galaxy called M M87 was chosen for the
608
00:25:03.590 --> 00:25:05.630
first target for that Event Horizon
609
00:25:05.630 --> 00:25:07.750
Telescope. But no, Mario, you're quite right.
610
00:25:07.910 --> 00:25:10.750
Um, it is that, uh, astronomers, when,
611
00:25:10.750 --> 00:25:12.350
if they talk about the diameter of a black
612
00:25:12.350 --> 00:25:14.510
hole, and that probably includes me as well,
613
00:25:14.890 --> 00:25:16.870
uh, are actually really referring to the
614
00:25:16.870 --> 00:25:19.390
event horizon because that's the parameter.
615
00:25:19.470 --> 00:25:22.350
And I love the way Mario signs off by saying
616
00:25:22.350 --> 00:25:25.130
thanks in advance to Dave and Fred. Uh,
617
00:25:25.130 --> 00:25:27.470
although he does say, AKA Andrew.
618
00:25:27.950 --> 00:25:29.790
Andrew Dunkley: Yes, that one's going to stick for a while,
619
00:25:30.750 --> 00:25:33.630
sorry to say. Thank you, Mario.
620
00:25:35.190 --> 00:25:37.550
Moving on. Uh, hi, Andrew and Fred. It's
621
00:25:37.550 --> 00:25:39.590
Andrew from Newcastle with another question,
622
00:25:39.670 --> 00:25:42.430
if I may. Just watched a doco on the quest
623
00:25:42.430 --> 00:25:44.430
to capture the first photograph of a black
624
00:25:44.430 --> 00:25:47.350
hole, uh, rather accurately, the shadow of a
625
00:25:47.350 --> 00:25:49.830
black hole, as Fred so eloquently explained.
626
00:25:49.830 --> 00:25:52.150
And I didn't understand one thing.
627
00:25:52.550 --> 00:25:54.710
Amongst others, of course, with the multiple
628
00:25:54.710 --> 00:25:56.750
observatories around the world and the use of
629
00:25:56.750 --> 00:25:58.550
atomic clocks to synchronize the data
630
00:25:58.630 --> 00:26:01.630
acquisition, why were they, uh, on
631
00:26:01.630 --> 00:26:04.420
tenterhooks, uh, regarding the weather
632
00:26:04.420 --> 00:26:06.740
at all the sites, with, uh, bad weather at
633
00:26:06.740 --> 00:26:09.060
just one, putting the whole venture in peril.
634
00:26:09.060 --> 00:26:11.580
I understand from the show and other sources
635
00:26:11.580 --> 00:26:13.780
that they were collecting radio wavelength
636
00:26:13.780 --> 00:26:16.220
data. And I thought that this was unaffected
637
00:26:16.220 --> 00:26:18.980
by the weather and atmospheric conditions. I
638
00:26:18.980 --> 00:26:21.700
thought that, uh, was the intrinsic beauty of
639
00:26:21.700 --> 00:26:23.820
radio astronomy. Day and night, rain and
640
00:26:23.820 --> 00:26:26.540
shine. Hope you can enlighten me.
641
00:26:26.620 --> 00:26:29.540
Wait for it. But over the radio. Dear,
642
00:26:29.540 --> 00:26:31.580
oh, dear. Uh, Andrew Broadhurst. Thank you,
643
00:26:31.580 --> 00:26:31.960
Andrew.
644
00:26:32.590 --> 00:26:33.950
Professor Fred Watson: That's a great question. Andrew.
645
00:26:33.950 --> 00:26:35.150
Andrew Dunkley: Leave the jokes to me, man.
646
00:26:37.710 --> 00:26:39.790
Professor Fred Watson: Yeah, well, I always leave them to you. So.
647
00:26:41.490 --> 00:26:42.910
Andrew Dunkley: Um, some to live. They're good.
648
00:26:43.390 --> 00:26:46.190
Professor Fred Watson: Oh, gosh. When was the last. Oh, never mind.
649
00:26:48.050 --> 00:26:49.950
Uh, Andrew's on the money. There is, you
650
00:26:49.950 --> 00:26:52.030
know, I thought radio waves were unaffected
651
00:26:52.030 --> 00:26:54.150
by the weather. And the answer is that radio
652
00:26:54.150 --> 00:26:56.910
waves come in different flavors. Uh, and
653
00:26:56.990 --> 00:26:59.190
so, uh, what you might call low frequency
654
00:26:59.190 --> 00:27:01.790
radio waves, um, which are still
655
00:27:01.870 --> 00:27:04.680
relatively, you know, they're way outside the
656
00:27:04.680 --> 00:27:06.880
medium wave band of radio and things of that
657
00:27:06.880 --> 00:27:09.520
sort. But low frequency in radio astronomy,
658
00:27:09.850 --> 00:27:12.600
um, I guess goes up to a couple of gigahertz
659
00:27:12.600 --> 00:27:15.280
or something like that. Um, those
660
00:27:15.360 --> 00:27:17.960
are largely unaffected by weather. That's
661
00:27:17.960 --> 00:27:19.680
absolutely right. So that's why it can be
662
00:27:19.680 --> 00:27:22.480
pouring down at Parkes, the radio dish there.
663
00:27:22.480 --> 00:27:24.000
And the astronomers are still happily
664
00:27:24.000 --> 00:27:26.720
observing through that. But the Event Horizon
665
00:27:26.720 --> 00:27:29.570
Telescope used higher frequencies. Uh, in
666
00:27:29.570 --> 00:27:32.010
fact, one of the telescopes that was
667
00:27:32.010 --> 00:27:34.850
incorporated into it was alma. The Atacama
668
00:27:34.850 --> 00:27:37.530
Large Millimeter Array, which has featured
669
00:27:37.530 --> 00:27:40.450
very, uh, very widely on space knots. That is
670
00:27:40.450 --> 00:27:43.290
a high frequency, uh, radio
671
00:27:43.530 --> 00:27:46.010
array. In fact, they have
672
00:27:46.090 --> 00:27:48.770
receivers that go up to, uh, more than
673
00:27:48.770 --> 00:27:51.330
900 gigahertz. So that's like, you know,
674
00:27:51.330 --> 00:27:53.890
nearly a thousand times higher frequencies
675
00:27:53.890 --> 00:27:56.170
than what we've just been talking about. And
676
00:27:56.170 --> 00:27:58.850
those sorts of frequencies, uh, the weather
677
00:27:59.010 --> 00:28:01.650
plays a very important role. Because water
678
00:28:01.650 --> 00:28:04.130
vapor actually dramatically
679
00:28:04.130 --> 00:28:06.930
absorbs the microwave signals.
680
00:28:07.250 --> 00:28:09.010
Andrew Dunkley: And that's what experience that watching
681
00:28:09.010 --> 00:28:11.090
satellite television. If there is a storm
682
00:28:11.810 --> 00:28:14.810
and it rains heavily, the wavelengths of the
683
00:28:14.810 --> 00:28:17.210
raindrops can absorb the signals from the
684
00:28:17.210 --> 00:28:18.450
satellite and you get nothing.
685
00:28:19.440 --> 00:28:21.610
Professor Fred Watson: Uh, that's interesting. I've never tried to
686
00:28:21.610 --> 00:28:24.040
watch satellite television. So that's, that's
687
00:28:24.040 --> 00:28:25.000
good thing to know.
688
00:28:25.420 --> 00:28:27.560
Andrew Dunkley: Um, it's one of the pitfalls.
689
00:28:27.800 --> 00:28:30.120
Professor Fred Watson: Yes, yes. In fact, I seldom watch television
690
00:28:30.120 --> 00:28:32.640
at all. So that's probably why. Um,
691
00:28:33.000 --> 00:28:35.960
but the bottom line is, um, you know, it's
692
00:28:35.960 --> 00:28:38.880
why facilities like ALMA and some
693
00:28:38.880 --> 00:28:41.480
of the other radio telescopes that were used,
694
00:28:41.900 --> 00:28:44.600
uh, to become the Event
695
00:28:44.600 --> 00:28:46.320
Horizon Telescopes, why they're all at high
696
00:28:46.320 --> 00:28:48.760
altitudes. Alma is at almost
697
00:28:48.840 --> 00:28:51.410
5,000 meters above sea level. Level,
698
00:28:51.840 --> 00:28:54.770
um, that's, you know, 15, 16,000ft.
699
00:28:54.770 --> 00:28:57.290
And at that height, there is very little
700
00:28:57.290 --> 00:28:59.770
water vapor in the atmosphere. Uh, but you
701
00:28:59.770 --> 00:29:01.770
can still get weather. And that's why they
702
00:29:01.770 --> 00:29:03.810
were indeed on tenterhooks about the weather.
703
00:29:03.810 --> 00:29:06.330
Because they don't want any of these, uh, if
704
00:29:06.330 --> 00:29:09.250
you lose one of those arrays, and
705
00:29:09.250 --> 00:29:10.810
I think there were eight of them that came
706
00:29:10.810 --> 00:29:12.810
together all around one hemisphere of the
707
00:29:12.810 --> 00:29:15.370
Earth, uh, to make up the Event
708
00:29:15.370 --> 00:29:17.530
Horizon Telescope. If you lose one of them,
709
00:29:17.680 --> 00:29:20.080
them, you lose a significant amount of your
710
00:29:20.080 --> 00:29:22.200
ability to reconstruct the image that they're
711
00:29:22.200 --> 00:29:24.760
seeing. Uh, and so that was why they were
712
00:29:24.760 --> 00:29:26.800
worried that the weather on just one of them
713
00:29:26.800 --> 00:29:29.760
might be, uh, moist, uh, or damper
714
00:29:29.760 --> 00:29:31.680
than they can cope with. And that would have
715
00:29:31.680 --> 00:29:33.160
screwed up the whole thing. But as it
716
00:29:33.160 --> 00:29:35.480
happened, it wasn't. It didn't happen. And it
717
00:29:35.480 --> 00:29:36.240
was great.
718
00:29:36.480 --> 00:29:38.160
Andrew Dunkley: They got global good weather.
719
00:29:38.480 --> 00:29:40.280
Professor Fred Watson: They did global good weather at these high
720
00:29:40.280 --> 00:29:41.960
altitude sites. That's right. The job.
721
00:29:41.960 --> 00:29:44.750
Andrew Dunkley: All right, there you are, Andrew. Uh, thank
722
00:29:44.750 --> 00:29:46.910
you for your question. And we've got one
723
00:29:46.910 --> 00:29:49.750
more. We'll squeeze in from John Sputh. I
724
00:29:49.750 --> 00:29:51.390
hope I pronounced that correctly. John,
725
00:29:51.390 --> 00:29:52.230
thanks for your question.
726
00:29:52.230 --> 00:29:52.590
Professor Fred Watson: Hi.
727
00:29:52.590 --> 00:29:54.510
Andrew Dunkley: I have a question that's been bugging me for
728
00:29:54.510 --> 00:29:56.990
some time and I need an expert to help me
729
00:29:56.990 --> 00:29:59.190
out. I think we should stop there. Fred.
730
00:30:00.150 --> 00:30:01.990
Professor Fred Watson: There's nobody here, is there? Who's that?
731
00:30:01.990 --> 00:30:03.430
Hang on. I'll go and see if I can find
732
00:30:03.430 --> 00:30:03.910
somebody.
733
00:30:04.310 --> 00:30:06.150
Andrew Dunkley: The cat could probably answer this one.
734
00:30:07.030 --> 00:30:09.990
Now, imagine, um, a spaceship traveling close
735
00:30:09.990 --> 00:30:12.110
to the speed of light. Disregarding that we
736
00:30:12.110 --> 00:30:13.910
don't have that sort of propulsion just yet.
737
00:30:14.310 --> 00:30:16.150
Would the increase in its
738
00:30:16.710 --> 00:30:19.670
relativistic mass at some point turn
739
00:30:19.670 --> 00:30:22.310
the spaceship into a black hole? And if so,
740
00:30:22.710 --> 00:30:25.430
would that spell the end of the ship and its
741
00:30:25.430 --> 00:30:27.950
crew? Or would they be able to slow down to
742
00:30:27.950 --> 00:30:30.710
reverse the process? What a great question.
743
00:30:30.790 --> 00:30:32.550
Professor Fred Watson: It is a fantastic question. Do you want to
744
00:30:32.550 --> 00:30:33.350
have a go at it?
745
00:30:33.660 --> 00:30:34.900
Andrew Dunkley: Uh, the answer is no.
746
00:30:36.010 --> 00:30:38.090
Professor Fred Watson: It is. You got right. Yeah, you're right on
747
00:30:38.090 --> 00:30:40.010
the money. They see. See, there is an expert.
748
00:30:40.010 --> 00:30:42.796
It's called Andrew Dunkley or Dave 50.
749
00:30:42.864 --> 00:30:43.690
Andrew Dunkley: 50 chance.
750
00:30:45.730 --> 00:30:48.650
Professor Fred Watson: Um, it's a great question. And it,
751
00:30:48.650 --> 00:30:51.450
it. The answer is a little bit, um,
752
00:30:51.450 --> 00:30:53.690
prosaic, I think. And that is that
753
00:30:54.250 --> 00:30:56.610
in the, in the rest frame of the
754
00:30:56.610 --> 00:30:59.250
spacecraft, you know. So if you're on the
755
00:30:59.250 --> 00:31:01.170
spacecraft and you're going at almost the
756
00:31:01.170 --> 00:31:04.030
speed of light, your mass doesn't change.
757
00:31:04.590 --> 00:31:07.230
It's only in the rest frame of
758
00:31:07.710 --> 00:31:10.230
a stationary observer. And by that I mean
759
00:31:10.230 --> 00:31:12.270
somebody watching you go past, somebody
760
00:31:12.270 --> 00:31:15.110
watches you hurl past. And your mass gets
761
00:31:15.110 --> 00:31:17.590
very much higher to the
762
00:31:17.590 --> 00:31:19.870
observer. But to the,
763
00:31:20.350 --> 00:31:23.270
the inhabitants of the spacecraft or the
764
00:31:23.270 --> 00:31:25.470
spacecraft itself, your mass doesn't change.
765
00:31:25.470 --> 00:31:25.870
Andrew Dunkley: It's.
766
00:31:25.870 --> 00:31:27.820
Professor Fred Watson: You're still normal. It is still normal.
767
00:31:28.290 --> 00:31:31.090
Yeah. And the same story is true with time
768
00:31:31.090 --> 00:31:33.850
dilation. You know that when you go
769
00:31:33.850 --> 00:31:36.530
nearer the speed of light, your clocks tick
770
00:31:36.530 --> 00:31:39.530
slower. Uh, that's a. Seen by a stationary
771
00:31:39.530 --> 00:31:42.370
observer. Uh, and so it's the same sort of
772
00:31:42.370 --> 00:31:43.809
thing. If you're on the spacecraft, your
773
00:31:43.809 --> 00:31:45.610
clock is ticking at the same rate as it ever
774
00:31:45.610 --> 00:31:47.690
was. But to a stationary observer, your
775
00:31:47.690 --> 00:31:48.850
clocks tick slower.
776
00:31:48.850 --> 00:31:51.010
Andrew Dunkley: And this has been proven with atomic clocks,
777
00:31:51.010 --> 00:31:51.490
hasn't it?
778
00:31:51.810 --> 00:31:54.170
Professor Fred Watson: It has. And indeed with mass as well. You can
779
00:31:54.170 --> 00:31:56.210
do this, you can see this sort of phenomenon
780
00:31:56.210 --> 00:31:58.920
with, um, uh. With uh,
781
00:31:58.920 --> 00:32:01.280
cosmic rays which travel very close to the
782
00:32:01.280 --> 00:32:02.520
speed of light. You can see their mass
783
00:32:02.520 --> 00:32:05.480
change. So, um, that's
784
00:32:05.480 --> 00:32:07.800
from the point of view of somebody who's, you
785
00:32:07.800 --> 00:32:10.000
know, not moving at the same speed. If you're
786
00:32:10.000 --> 00:32:11.920
moving at the same speed, you don't see any
787
00:32:11.920 --> 00:32:12.640
change at all.
788
00:32:13.680 --> 00:32:16.640
Andrew Dunkley: That's pretty boring. The more we Discuss
789
00:32:16.800 --> 00:32:18.840
black holes and the number of questions we
790
00:32:18.840 --> 00:32:21.760
get about them. People are really quite
791
00:32:22.160 --> 00:32:25.040
captivated by the strangeness of
792
00:32:25.040 --> 00:32:27.320
them. I suppose they throw up all these
793
00:32:27.320 --> 00:32:30.220
things that seem so alien to what we consider
794
00:32:30.300 --> 00:32:32.900
normal. Uh, and that's because we've only
795
00:32:32.900 --> 00:32:35.700
experienced um, what's happening on our
796
00:32:35.700 --> 00:32:38.660
planet at any given time. So to try
797
00:32:38.660 --> 00:32:41.380
and comprehend um, enough gravity to
798
00:32:41.380 --> 00:32:44.300
warp time to slow things down
799
00:32:44.459 --> 00:32:47.260
to the observer and increase mass. Just,
800
00:32:47.980 --> 00:32:49.020
it's really whack.
801
00:32:50.780 --> 00:32:53.740
Professor Fred Watson: Sad on the brain. That's true. But uh,
802
00:32:53.740 --> 00:32:56.060
look, John's question there is a great
803
00:32:56.060 --> 00:32:58.660
question because it's not intuitively
804
00:32:58.660 --> 00:33:01.610
obvious what is happening uh,
805
00:33:01.650 --> 00:33:04.010
in a situation like something traveling close
806
00:33:04.010 --> 00:33:06.810
to the speed of light. And it, and so he's
807
00:33:06.810 --> 00:33:09.570
right to ask would that mass actually turn it
808
00:33:09.570 --> 00:33:11.890
into a black hole? Uh, but the answer is no
809
00:33:11.890 --> 00:33:13.370
because of the reasons that I've outlined.
810
00:33:13.370 --> 00:33:14.610
But it's great, great thinking.
811
00:33:14.610 --> 00:33:16.490
Andrew Dunkley: It is indeed. Thank you John. Thanks for the
812
00:33:16.490 --> 00:33:18.330
question. Do appreciate it. Keep your
813
00:33:18.330 --> 00:33:20.650
questions coming in. We're trying to um, run
814
00:33:20.650 --> 00:33:23.570
them down but they, it's, it's, it's an ever
815
00:33:23.570 --> 00:33:25.360
growing mass really.
816
00:33:25.360 --> 00:33:27.760
Professor Fred Watson: It's. All right, look, as you said earlier
817
00:33:27.760 --> 00:33:30.120
Andrew, um, all the space nutters are going
818
00:33:30.120 --> 00:33:31.760
to get together and sort them out for
819
00:33:31.760 --> 00:33:33.720
themselves and we'll be, that'll be
820
00:33:33.960 --> 00:33:34.520
encouraged.
821
00:33:34.520 --> 00:33:36.840
Andrew Dunkley: Actually if uh, people want to ask questions
822
00:33:36.920 --> 00:33:39.600
of the group uh, and discuss it,
823
00:33:39.600 --> 00:33:42.280
they. Yeah, by all means. Um, that, that's
824
00:33:42.280 --> 00:33:44.080
part of the reason we set up the Space Nuts
825
00:33:44.080 --> 00:33:46.880
podcast group. So um, it's a good opportunity
826
00:33:46.880 --> 00:33:49.840
to not only meet like minded people who enjoy
827
00:33:49.840 --> 00:33:52.160
these, these topics, but also to maybe come
828
00:33:52.160 --> 00:33:54.020
up with your own ideas on, on what might,
829
00:33:54.170 --> 00:33:55.970
might be and you know, I'll keep an eye on it
830
00:33:55.970 --> 00:33:57.570
and if something pops in there that we think
831
00:33:57.570 --> 00:34:00.090
is worthy of further discussion, we will
832
00:34:00.170 --> 00:34:03.090
certainly investigate that. Thanks
833
00:34:03.090 --> 00:34:05.490
to everyone who um, who sent in their
834
00:34:05.490 --> 00:34:08.450
questions, uh, and uh, contributed and joined
835
00:34:08.450 --> 00:34:10.930
the Space Nuts podcast group and Patreon and
836
00:34:10.930 --> 00:34:13.140
everything else. We really appreciate it. Uh,
837
00:34:13.210 --> 00:34:15.210
but most of all we appreciate you Fred. Thank
838
00:34:15.210 --> 00:34:15.770
you so much.
839
00:34:16.330 --> 00:34:18.730
Professor Fred Watson: It's a pleasure, thank you for having me as
840
00:34:18.730 --> 00:34:19.050
always.
841
00:34:19.290 --> 00:34:22.059
Andrew Dunkley: And we will catch you next week. Professor
842
00:34:22.059 --> 00:34:24.779
Fred Watson, uh, astronomer at large and from
843
00:34:24.779 --> 00:34:27.099
me Andrew Dunkley. Thank you again and we'll
844
00:34:27.099 --> 00:34:29.539
catch you next time on another edition of
845
00:34:29.619 --> 00:34:32.339
SpaceNuts. Uh, you'll be
846
00:34:32.339 --> 00:34:34.579
listening to the Space Nuts podcast
847
00:34:36.099 --> 00:34:38.899
available at Apple Podcasts, Spotify,
848
00:34:39.059 --> 00:34:41.819
iHeartRadio or your favorite podcast
849
00:34:41.819 --> 00:34:43.579
player. You can also stream on
850
00:34:43.579 --> 00:34:45.299
demand@bytes.com.
851
00:34:45.619 --> 00:34:47.659
Professor Fred Watson: This has been another quality podcast
852
00:34:47.659 --> 00:34:49.779
production from bytes.com.