Episode Transcript
Transcripts are displayed as originally observed. Some content, including advertisements may have changed.
Use Ctrl + F to search
0:01
What's the furthest start that we can
0:03
see with the naked eye? To answer
0:05
this question, you have to make some
0:08
assumptions about your have been a And they could
0:10
Why can't we predict the sun's Why field?
0:12
I'm gonna say good question probably for
0:14
the last time this year. say good
0:16
question, probably for the last time
0:18
this year. and welcome to the the
0:20
supermassive podcast Astronomical Society with me
0:22
with me science journalist Isie astrophysicist Dr.
0:24
Becky Dr. Becky Smetherst. Now the Eagle-eyed or among
0:26
you you notice that our
0:28
last podcast of of 2024 is not an
0:30
not an episode about the
0:32
scientific search for extraterrestrial life
0:34
we we promised. A slight change slight
0:37
change of plan. We weren't
0:39
quite ready for that one.
0:41
it it turns out getting, you
0:43
know, someone who studies, like,
0:45
the search for alien you know...
0:47
I trying to the - universe down
0:49
in December down in December trying to
0:51
find the aliens themselves. to find the aliens
0:53
themselves. just swap things around things around.
0:55
So we're going to tackle some
0:57
of your brilliant questions for
0:59
this episode and obviously we can't
1:01
have an episode without without Dr. Robert
1:03
the Deputy Director of the
1:05
Royal Astronomical Society. Astronomical going to
1:07
kick things off with an easy
1:09
question for the both of
1:11
you. for you have a you festive
1:13
astronomy fact? fact? Well, I don't have
1:16
a huge I don't have a huge number,
1:18
but I think there is a sort
1:20
of night sky object, which which is the genuinely
1:22
named named Christmas of cluster which has of NGC
1:24
as well. It just which has got a to
1:26
as well. It just happens to be
1:28
visible right now as in the Monoceros, the
1:30
the unicorn to the east of the So if of in
1:32
So if you're in the North event,
1:35
looking to the left of it. And
1:37
it just so happens that infrared images, some
1:39
telescopes of this Christmas tree cluster tree
1:41
to be coded to show it in
1:43
green. to show to why they do that. in
1:45
their why they would do it's a really lovely object and it
1:47
does look a little bit like the lights of
1:49
a Christmas tree. does look a little bit make
1:51
lights of a Christmas tree. Yeah, why don't
1:54
they make that false color in this show?
1:56
It's impossible to guess, I think. Yeah, my
1:58
fact for this week, week. come
2:00
on the No Such Things a Fish
2:02
podcast. This is great. My fact for
2:04
this week was in 2017 undergraduate students
2:06
at the University of Leicester calculated the
2:08
number of Christmas lights you would need
2:10
to add to the outside of your
2:12
house to make it visible from space.
2:14
Amazing. Yeah, I'm like I want to
2:16
find these students and I want to
2:18
shake their hands because this is fantastic.
2:20
So it turns out if you're interested
2:22
you would need 10,060. lumens, so it's
2:24
the like, you know, magnitude of lights
2:26
you would need, or the equivalent of
2:28
2,638 LED. Christmas lights. Oh my gosh,
2:30
I know. It's wonderful. They were inspired
2:32
by the Christmas film from 2006, they
2:34
decked the halls for those who've seen
2:36
it, because I think that's the whole
2:38
premise of the film and they were
2:40
like, well, let's visit this. We could
2:42
do this. Yeah. Also, speaking of Christmas
2:44
films, easy, did you? Did you? Have
2:47
you seen the new Netflix Christmas films?
2:49
Well, with Lindsay Lohan, it's called Our
2:51
Little Secret? And the premise of the
2:53
film is like, like, like, something happened.
2:55
in 2014 and they have to zoom
2:57
through to 2024 and the opening credits
2:59
of the scene is then basically going
3:01
through like you know a load of
3:03
like world events to show time passing
3:05
and three astronomy news stories made it
3:07
in there and they were the only
3:09
science things that were shown in that
3:11
global sort of news recap from 2014
3:13
to 2024 in an episode. Yeah it
3:15
was Pluto's so the New Horizons fly-by
3:17
of Pluto with that first image of
3:19
Pluto we got was perseverance landing on
3:21
Mars and then the first ever image
3:23
of a black hole in Messier 87.
3:25
There was also William Shatner going to
3:27
space which I guess you could also
3:29
count but I didn't. obviously the era's
3:31
tour from Taylor Swift at the end
3:33
of it. But I figured that one
3:35
of the projection team on the film
3:37
must have been a big astronomy fan,
3:39
you know, maybe they're listening now, who
3:41
knows? Amazing, I mean that's just maybe
3:43
even more excited to watch this, Lizzie,
3:45
Christmas, I'm too honest. Actually, I'm gonna
3:47
throw something in here as well, because
3:49
I was looking at Christmas on the
3:52
ISS, and then I got into a
3:54
bit of. rabbit hole so my fact
3:56
that I want to bring to the
3:58
table is in 1973 on board the
4:00
Skylab orbital station astronauts Gerald Carr William
4:02
Polk and Edward Gibson made their own
4:04
Christmas tree they used discarded food cans
4:06
and sort of pushed them all together
4:08
to create a stem and then like
4:10
various branches of the tree and then
4:12
use little stickers as decorations and put
4:14
a cardboard cut out of a comet
4:16
on top. that once they were back
4:18
to earth, they were like, yeah, your
4:20
Christmas tree is nice, but it's not
4:22
as good as the one we made,
4:24
but in space. Exactly, exactly. Nothing ever
4:26
compares to it, ever. Yeah, totally. Okay,
4:28
so let's get on to the listener
4:30
questions. And Robert, Matt P. 24601, wants
4:32
to know which star or planet do
4:34
you think was most likely to have
4:36
been the star of Bethlehem? Well, Matt,
4:38
Matt P. 24601, definitely a perennial question
4:40
there, one that funny enough. of every
4:42
year at this time of year. I
4:44
think the answer is, you know, something
4:46
we'll never know for sure. And as
4:48
an atheist, I'm probably going to get
4:50
into at least warm water over this.
4:52
I'm treading carefully. But on the other
4:55
hand, I'd be genuinely interested in astronomical
4:57
phenomena that coincide with the suggested date
4:59
or dates, actually, of the birth of
5:01
Jesus. Now, there's actually a nice piece
5:03
on the Vatican Observatory website, which is
5:05
a respectable. but it's just on astronomical
5:07
institution actually and it invites us to
5:09
use our sense of wonder over what
5:11
it might have been and I think
5:13
that's absolutely fine. Yeah, it's a totally
5:15
reasonable way of looking at it and
5:17
happy Christmas to the astronomers in the
5:19
Holy Zay. But turning to the suggested
5:21
ideas, so it ranges from it didn't
5:23
exist at all to all manner of
5:25
things and it could have been invented
5:27
as this so-called pious fiction or midrash
5:29
where the star was added in to
5:31
emphasize Jesus's divine nature. And in astronomy
5:33
though, there are quite a few obviously
5:35
significant things in the sky that could
5:37
be candidates. And for example, there was
5:39
a really incredibly close conjunction of Jupiter
5:41
and Saturn in 7BCE, or an even
5:43
ridiculously close. conjunction in Jupiter and Venus
5:45
in 2 BC where the two worlds
5:47
would actually have a pitch pit of
5:49
merge that's very very rare indeed so
5:51
I imagine if you were looking at
5:53
that in the sky thinking the astrological
5:55
significance run the astronomical significance you know
5:58
if you're thinking about the mythology associated
6:00
with that you would have thought wow
6:02
or something something very unusually is happening
6:04
here and that came after Jupiter and
6:06
Venus were close together a year earlier
6:08
and they were also near the star
6:10
regular the bright star regular in Leo
6:12
as well. Another idea is a comet,
6:14
although there don't seem to be records
6:16
and the Chinese are really really good
6:18
at keeping those records at the time,
6:20
of anything that bright in that period
6:22
of time, there's possibly one in five
6:24
BCE, you know, just again really quite
6:26
uncertain what it might have been like.
6:28
And there could also have been a
6:30
supernova, although... you know, again, he sort
6:32
of imagined somehow that would have had
6:34
more of an impact in historical text.
6:36
But anyway, there could have been one
6:38
in the 4 BC that happened to
6:40
create the system with the unromantic name
6:42
PSR 1913 plus 16, which happens to
6:44
be the first binary pulsar discovered. So,
6:46
but all these things, my personal hinges,
6:48
either the star never existed at all,
6:50
or it's probably, you know, the Jupiter
6:52
Venus conjunction seems to me like a
6:54
good explanation, because the idea of which
6:56
I don't think... anything like that happened
6:58
in the 20th century, it certainly hasn't
7:01
happened yet in the 21st century, the
7:03
idea that two planets are so close
7:05
together that they're actually touching is extraordinarily
7:07
rare. So maybe that was so significant
7:09
that people drew on that. Yeah, there
7:11
was a Jupiter Venus conjunction. Was it
7:13
like a few Christmases ago now, like
7:15
two, three Christmases ago? And I remember
7:17
that was really nice to see that
7:19
they were coming so close together and
7:21
they were so bright. But I mean,
7:23
they came still like a thumb width
7:25
apart or something. I can't even imagine
7:27
what it would look like if they
7:29
overlapped completely from our perspective here on
7:31
earth. Absolutely. And even the Jupiter Saturn
7:33
one that we all got very excited
7:35
about that. you know they were very
7:37
close they were well under you know
7:39
somewhat of a fairly small fraction of
7:41
a degree but they were still not
7:43
touching and it must be so extraordinarily
7:45
rare. that happens. I want to look
7:47
now when the next time that's going
7:49
to happen, like is it going to
7:51
happen in our lifetime? We'll get back
7:53
to you in the future. I have
7:55
a feeling from memory not but we
7:57
can check. So not my lifetime at
7:59
least. Well at least now we'll have
8:01
an answer when someone asks like if
8:04
you could go in the future if
8:06
you could go anywhere to see the
8:08
web and I'll go to the next
8:10
conjunction. Okay well we'll stick on the
8:12
theme of spotting things in the night
8:14
sky because Robert there's a question What
8:16
a brilliant name can we just say?
8:18
And their question is, what's the furthest
8:20
star that we can see with the
8:22
naked eye? Yeah, I mean, perring Posa,
8:24
a great name, great question. Well, I
8:26
started, funnily enough with the Google search,
8:28
because it's not the sort of thing
8:30
Astronomers. collate in papers and part of
8:32
the reason is you know it depends
8:34
how good your eyes are and circumstances
8:36
to what the faintest thing you can
8:38
see with the naked mind. Mine is
8:40
not very good. Yeah yeah see but
8:42
you can probably see the Andromeda galaxy
8:44
right two and a half million light
8:46
years away so on you know for
8:48
non-stars for big things it's a really
8:50
long way. But, so when I looked
8:52
around, there were several articles saying, oh,
8:54
this is variable style v762 Cassiope, which
8:56
means it's in the constellation Cassiopea, 16,000
8:58
light years away, but then you dig
9:00
around quickly and the Wikipedia article said,
9:02
oh, actually it's 2,500 light years. So
9:04
I went into the Simbag database, which
9:06
has things like parallax. looking at how
9:09
it shifts back and forth as the
9:11
earth goes around the sun, measured by
9:13
the Gai satellite, and indeed that comes
9:15
up with two and a half thousand
9:17
light years, so a lot closer. You
9:19
can get these numbers for yourself if
9:21
you good luck remembering this, but if
9:23
you put HD 7389 into that Simbad
9:25
database, you get those numbers and then
9:27
there are calculations to help you work
9:29
it out. So then I was looking
9:31
around a bit more and there isn't...
9:33
I don't think there's any definitive answer
9:35
to this yet at least. Somebody needs,
9:37
probably it needs to be some sort
9:39
of, you know, post-op with time on
9:41
their hands. I think, well, Jackie doesn't
9:43
really have time on their hands, but
9:45
you know, yeah, exactly. But, and that's
9:47
because the stars get fainter, we see
9:49
a lot more of them, so unless
9:51
something is very luminous or very notable,
9:53
you know, we can just about see
9:55
if they're naked. we might not have
9:57
a record of it. Two examples are
9:59
stars in Cepheus, which happens to be
10:01
visible at this time of year quite
10:03
well, and one of them is Mucefi,
10:05
famous as an incredibly red Garnet star,
10:07
and it might be about 3,000 light
10:09
years away, but it's actually quite hard
10:12
to tell the measurements are not that
10:14
good. as it happens that one is
10:16
also so large that you know even
10:18
without uncertainty it would fill the solar
10:20
system as far out as Jupiter absolutely
10:22
enormous colossal star the other one called
10:24
New Cephi and that's a white blue
10:26
super giant that might be as far
10:28
away as 4,700 light years you know
10:30
with again with a lot of uncertainty
10:32
but you know both of those are
10:34
actually comfortably a lot brighter than the
10:36
naked eye limit of a... about magnitude
10:38
6.5 and even the fainter one is
10:40
about seven and a half times brighter
10:42
so somebody really needs to go out
10:44
there and trawl through the catalogs right
10:46
some crawler software or something to try
10:48
and work this out. And the one
10:50
thing I'd add is if you get
10:52
a supernova then they're obviously visible over
10:54
much greater distances and exploding star is
10:56
really very bright indeed. The one in
10:58
1987 which I remember but didn't see
11:00
down in the large Magellanic cloud, seen
11:02
for months in the southern hemisphere and
11:04
that was 170,000 light years away. So
11:06
supernova, single star, really are so bright,
11:08
you see them a long long way
11:10
off, but nothing like that around the
11:12
moment. I really hope I get to
11:15
see one in my lifetime. That is
11:17
just like a fingers cross, 2025, amazing,
11:19
but lifetime. Yeah, that'll be great. Since
11:21
we have one in our galaxy, four
11:23
centuries. So we are overdue. Yeah. Oh,
11:25
and Becky in true Q&A style. We
11:27
have a question for you about black
11:29
holes and I think we've got quite
11:31
a few on the way to this.
11:33
I've been disappointed if we didn't come
11:35
through it. And do you know one
11:37
wants to hear about black holes this
11:39
episode? Kelsbury's. No. So Joe has a
11:41
question about planet X, which is also
11:43
known as the solar systems planet 9.
11:45
We did an episode about this back
11:47
in May 2021 2021. do go and
11:49
have a listen back to that. I
11:51
thought that was more recent than that,
11:53
but time is doing its thing. Anyway,
11:55
Joe says, I have a question about
11:57
the possibility that Yeah Joe, this is...
11:59
the dream, right? So if the solar
12:01
system did have this baby black hole
12:03
just hanging around, you know, and if
12:05
you work out the maths from sort
12:07
of like, okay, the reason we think
12:09
this black hole might be the edge
12:11
of the solar system is because, you
12:13
know, there's all these dwarf planets at
12:15
the edge of the solar system, sort
12:18
of like, like, asteroid-style things, and their
12:20
orbits are being affected by something, and
12:22
we don't know why, and we can't
12:24
explain it, and people have like, like,
12:26
like, like, like, like, 400 to 800
12:28
A-U distance. So an A-U is the
12:30
distance from Earth to the sun. So
12:32
400 to 800 times more distant than
12:34
the Earth is from the sun. That's
12:36
like 10 to 20 times the distance
12:38
of Pluto from the sun to give
12:40
you an idea. The voyage probes, which
12:42
launched at the end of the 70s,
12:44
are not that far out yet. There's
12:46
some figure out while you're around 115
12:48
70-ish, something like that A-U. So we
12:50
would definitely need to send something quicker.
12:52
Well, we said voyage of probes. Big
12:54
problem there, though, is slowing something down
12:56
once it's that far out so that
12:58
you could actually maybe like orbit this
13:00
little baby black hole from, you know,
13:02
a safe enough distance for the probe,
13:04
for example. Otherwise, essentially, you're just going
13:06
to each something straight past it. which,
13:08
you know, is not what you want.
13:10
This is why we haven't put a
13:12
probe in orbit around Neptune or Uranus,
13:14
or even Pluto, right? The New Horizons
13:16
probate did a flyby of Pluto. Voyager
13:18
did, the Voyager probes did flybyes of
13:21
Uranus and Neptune. Because it's very hard
13:23
to slow down. And people have sort
13:25
of talked about this idea of... atmospheric
13:27
breaking, almost kind of like skimming a
13:29
stone off the surface of the pond,
13:31
right? It's kind of like what you
13:33
do to your probe. You just skim
13:35
into the top of your in a
13:37
sun atune atmosphere to slow it down.
13:39
No look there though with a black
13:41
hole. So assuming we can solve that
13:43
problem, then yes, we would totally send
13:45
a probe to orbit around this black
13:47
hole if it was there on the
13:49
edge of the solar system. Of course
13:51
we send a camera, I think it
13:53
would be stupid if we didn't. It's
13:55
not like they're overly expensive, right? It's
13:57
not the most expensive part of sending
13:59
a probe is the camera these days.
14:01
And I think, if you're thinking, would
14:03
we really even see anything? Like, yes,
14:05
I think we would. We would definitely
14:07
see the black calls impact on the
14:09
light from stuff behind it, for example.
14:11
So as it passed in front of,
14:13
you know, stars in the Milky Way,
14:15
for example, we would basically have this
14:17
sort of this sort of perfect. gravitational
14:19
lens telescope, right? It's the light room
14:21
stars behind it, got sort of bent
14:23
by the gravity of the black hole.
14:26
In terms of other things you'd send
14:28
though, like one thing we want to
14:30
test for is gamma rays, because if
14:32
this, so it's a black hole that's
14:34
thought to be a primordial black hole,
14:36
someone that was forming in the very
14:38
early days of the universe, like, you
14:40
know, 13.8 billion years ago, let's say.
14:42
And so because it's been around for
14:44
that long, it... sort of would have
14:46
collected like a little halo of matter
14:48
over the years. Like it's just sort
14:50
of wandering through the solar system and
14:52
empty space like you know it is
14:54
the vacuum space but it's not quite
14:56
empty it's like one particle every huge
14:58
volume right it would have slowly sort
15:00
of gathered those things like close to
15:02
it and around it. So it would
15:04
have gathered matter, but it also would
15:06
have gathered like antimatter, right? And antimatter
15:08
and matter when they collide and meet,
15:10
they annihilate and produce gamma rays. So
15:12
you might expect if there's quite a
15:14
bit of a halo of stuff around
15:16
that black hole from over the years,
15:18
it might annihilate and we might see
15:20
those annihilations going on, which would be
15:22
really cool to see as well. And
15:24
finally the spigetification question. I think we'd
15:26
be stupid if we didn't send something
15:29
into water back off. Like if we've
15:31
got a probe orbiting it from a
15:33
safe distance and then we just send,
15:35
you know, like a little cube set
15:37
or something. almost do like
15:39
the the test where
15:41
it's like okay
15:43
you've got got an Alice who's
15:45
observing Bob fall into a black hole
15:47
and they'd be called be
15:49
called Alice and Bob
15:51
it it would be
15:53
the most most physics
15:55
ever right you sent
15:57
this little cube set
15:59
that would probably
16:01
have a camera on
16:03
board as well board
16:05
as also probably send
16:07
out some sort
16:09
of beep of a
16:11
signal that we would
16:13
probably be able
16:15
to see to of
16:17
have that time dilation
16:19
to it where
16:21
we would where we that
16:24
that. beep was going off every minute gets
16:26
slower and slower because of the gravitational effects because of
16:28
the black hole and things like that. We
16:30
could almost directly test it. got closer right, you think,
16:32
well, at some point it's gonna get like around
16:34
a black hole like that. But, you know, it's
16:37
like sending probes into atmosphere, well,
16:39
right? it's at some point it's going to get lyric
16:41
acid, right? We still did it, a
16:43
you know? I think like that. to
16:45
the extreme. like I was just
16:47
like, we're sending something to break
16:49
it. Yes. right? Yeah. Just a good way.
16:51
In a great way for some weird
16:53
always say learn something more if it breaks you
16:55
go to fix it. to fix it. Well,
16:57
there we go. Joe, I hope that
16:59
answered your question. that And we have
17:01
this question from Matt in Australia. question
17:04
from Becky Izzy, Robert Becky, Izy, Robert, and producer
17:06
that Richard always appreciates that always So
17:08
there we go. the Christmas, Richard.
17:10
go. Merry Christmas Richard. Maybe this is it. In
17:12
the last bonus last bonus episode,
17:14
19 had a had a question
17:16
about accelerating particles with
17:18
mass to the speed of
17:20
light. So I thought
17:22
I'd throw a wrinkle at
17:24
Dr a wrinkle at you accelerated
17:26
an uncompressed an potato to
17:28
99 % the speed of
17:31
light, would that potato
17:33
become a black hole due
17:35
to Einstein's mass hole due to
17:37
Einstein's mass energy equivalents?
17:39
this question. so much Matt and it was
17:41
much was like was undergraduate undergraduate
17:43
maths question a with a
17:45
puzzle in the morning
17:47
newspaper, like all in one. damned I was
17:49
in heaven, honestly. right so let's
17:51
go through this go through this.
17:54
not aware for those not aware, first
17:56
of all, let's do a little Einstein's
17:58
generalativity 101 as you excel objects close
18:00
to the speed of light, the more
18:02
energy you put in, it doesn't go
18:05
into increasing an object speed, but instead
18:07
increases the objects mass, at least when
18:09
you get close to the speed of
18:12
light. So that's what we were talking
18:14
about in last month's bonus episode. So,
18:16
as for our potato. Sadly, no, the
18:19
potato would not become a black hole
18:21
at 99% of the speed of light.
18:23
So essentially, the equation for this is
18:26
quite simple. You have the mass of
18:28
the potato originally, and it gets timed
18:30
by this thing called the gamma factor
18:33
to give you the relativistic mass, right?
18:35
So, the gamma factor is one over
18:37
the square root of one minus the
18:40
speed over the speed of light all
18:42
squared. Okay? So, if our speed is...
18:44
0.99 times the speed of light, 99%
18:47
of the speed of light, then our
18:49
gamma factor is about seven-ish. So our
18:51
potato only increases by mass about seven
18:54
times and that's not heavy enough to
18:56
become a black hole. Like potatoes aren't
18:58
that heavy in the first place. I
19:01
don't know if you've noticed. I've seen
19:03
lumps of metal that are seven times
19:05
in the other than a potato. So,
19:08
so... You might ask, is he and
19:10
Matt, and Robert, since everyone's here, how
19:12
fast does a potato need to be
19:15
travelling to become so heavy? Well, yeah.
19:17
It becomes a black hole. It's on
19:19
my mind for Christmas. Yeah, you know,
19:22
I just can't fall asleep thinking of
19:24
all the presents I've got a wrap
19:26
and how big a potato and need
19:29
to move. Okay, seriously. To answer this
19:31
question, you have to make some assumptions
19:33
about your potato. Okay, so Matt said
19:36
a medium-sized potato. So, you know, not
19:38
a new potato, not a baked potato,
19:40
a medium-sized potato. I've got loads of
19:42
those in my cupboard, ready for roasted
19:45
on Christmas Day. Is it a flowery
19:47
or waxy? It's a Maris Piper, I
19:49
don't know. Flowery, flowery. Anyway, so I
19:52
grabbed a few, I had a little
19:54
measure. I basically decided on some round
19:56
numbers in the end because I was
19:59
like well let's say roughly it's about
20:01
a 10 centimetre wide potato let's assume
20:03
it's this fear because I'm a physicist
20:06
and that's what we do and let's
20:08
assume it's around about 100 grams for
20:10
those saying at home I should have
20:13
done it properly and taken a specific
20:15
potato and I should have got the
20:17
numbers right you will very quickly see
20:20
the numbers don't matter so we are
20:22
going to go with a 10 centimetre
20:24
potato that's about 100 grams so Because
20:27
we know that black holes collapse when
20:29
you squish an object into a volume
20:31
that's less than it's what's called it
20:34
swatch shield radius, right? So that's essentially
20:36
like the radius of which you'd have
20:38
to be traveling fast in the speed
20:41
of light to escape it, right? So
20:43
we need to work out the mass
20:45
of a 10 centimetre, diameter, potato. So
20:48
that's a swatch shield radius of 5
20:50
centimetres. Which if you do the mass
20:52
is 30 trillion kilograms. It's about 5.6
20:55
times the mass of Earth. Or instead
20:57
of you remember our gamma factor before
20:59
being 7-ish, it would be 300 trillion
21:02
trillion potatoes, so a gamma factor of
21:04
300 trillion trillion trillion. Which unfortunately it
21:06
actually makes the math very very difficult
21:09
because if you try to get back
21:11
from your gamma factor to what the
21:13
velocity would be, remember I said gamma
21:15
was like one over the square root
21:18
of one minus the velocity over the
21:20
speed of light or squared. To get
21:22
back to it you need to do
21:25
like one over gamma squared, which if
21:27
you've got a gamma factor of 300
21:29
trillion trillion, if you square that number
21:32
and then do one over that massive
21:34
massive number, most calculators are going to
21:36
be like, you've got zero, if you're
21:39
going to do one minus zero, you've
21:41
got one. So I managed to hack
21:43
this with Python code, thankfully, that lets
21:46
you go out to a ridiculous number
21:48
of decimals to get you an accurate
21:50
answer. Well, that's potato. And it is
21:53
99.9.9. 52.9s. percent of
21:55
the speed of light.
21:57
Is the speed
22:00
a medium -sized potato
22:02
would have to be
22:04
traveling at two?
22:07
collapse into a black hole. And
22:09
there you go, That's Christmas of. I
22:11
mean, who knew that that's where it would
22:13
lead us? Matt in Australia, thank you
22:15
so much. Honestly, Matt had an absolute joy
22:17
answering that question and that's all I'm
22:19
going be able to think about Christmas Day
22:21
making my roasties. We know what you're
22:23
going be talking about around the dinner table.
22:25
Did you know? OK,
22:28
Robert, Jane Payne
22:30
on Instagram asks, What
22:32
do we need a moment to regroup?
22:34
We probably do. I'm just thinking whether it
22:36
applies to sprouts or what size of
22:38
turkey would be. kind kind like of a had
22:41
a sized sprout. Exactly. Big or a
22:43
small turkey, geese, you know, nuts, things, nut
22:45
you you know. Oh,
22:47
brilliant. Okay, Robert, Robert
22:49
J. Payne on Instagram
22:52
has a question and they ask. Is
22:54
there a certain criteria for a
22:56
planet or moon to become tidally
22:58
locked? Yeah. Well,
23:00
I'm going to say good question, probably for the
23:02
last time this year. Yeah,
23:04
the answer is yes. But first of
23:06
all, should say what it is. So tidal
23:08
locking is or captured rotation is where the
23:11
rotation period of a body or how long
23:13
it takes to spin on its axis matches
23:15
its revolution period or how long it takes
23:17
to complete an orbit around its parent
23:19
body. So the example being the moon and
23:21
the earth the classic one, because the moon
23:23
more or less keeps the same face to
23:25
us. And we see a bit more than
23:27
half of it because if you're further north.
23:29
or or depending on where you're looking
23:31
at moon rise or moon set or
23:33
the fact the moon's orbit is an ellipse
23:36
you get to see a bit round
23:38
the back but there are still two -fifths
23:40
of the moon we never see from Earth
23:42
for this reason because its face is
23:44
locked towards us. Now it happens because you
23:46
get energy dissipated through tidal heating the
23:48
object and stretching and so on and that
23:50
eventually eventually over a long time scale
23:52
typically billions of years it depends on the
23:54
system means that the rotation that object
23:56
slows down until it locks into place and
23:58
that happens to both of them actually so you
24:00
know it will happen to the earth as
24:02
well in about about billion years time which
24:04
is much much longer than the than of the
24:07
of the sun the earth moon would do the same thing
24:09
and the thing the the both be moon would both
24:11
each other locked with each other to give you a
24:13
kind of number for when it happens is
24:15
quite hard what it depends on what the
24:17
objects made rigid it is. What you on how rigid
24:19
it is you know, you can it, is that
24:21
more massive will happen, the quicker it will happen, and closer the quicker
24:23
it will happen it, the closer the quicker it the
24:25
quicker and the closer well, and it's very strongly
24:28
dependent on that it goes to the power
24:30
going to, when it is going to, when it going to, when it is know
24:32
if it's it is going to, when is going to
24:34
rapidly it's going to, think it's going the it's system that
24:36
might have happened going quickly as well because we
24:38
think the moon was much it's closer to
24:40
the to, when it formed when it's in this big
24:42
collision between the proto the and a mars sized
24:44
body a the debris forming the moon debris know
24:46
it may have been that the moon locked
24:49
into place quite quickly as a result moon
24:51
really hard to say exactly how long though as
24:53
a if you sat around if you had
24:55
an infinite amount of time then in theory
24:57
all if you eventually end up like this it's
24:59
just time, then in theory, all very long time if
25:01
they're further apart and if the body
25:03
is less rigid and all of those
25:05
things very, very no easy answer but the
25:07
criteria is just really that they're in
25:09
orbit around each other and this process is
25:11
going to happen if you sit around
25:13
long enough long you know that could
25:15
be know that could guess hundreds or even billions
25:17
or even trillions of years in of
25:19
cases. We do by the way also
25:21
see it with lots of satellite planet
25:23
systems in the solar system and famously
25:25
Pluto and and its biggest moon Sharana already mutually locked they
25:27
keep the same face to each other.
25:30
there all the time as they orbit round. And you
25:32
know we see it with other know we see it with
25:34
other moons in the solar system I think
25:36
it's about them of them doing that particularly big
25:38
moons of and Saturn and Saturn. also with planets going
25:40
going stars as well because if you get
25:42
say a planet say, a a very near to star
25:44
then it's locked in place in the same
25:46
way way. So I'm not not giving you a very
25:48
precise answer but the criteria are essentially you
25:50
know pretty much everything will do if you've
25:52
got enough time to wait to wait. know what you
25:54
should have done, Robert? should have worked out how long it would have
25:56
took to a medium how long it would have took a
25:59
medium-sized potential. It probably is the more than
26:01
the lifetime of the years, but yeah, right now
26:03
that is another, that is another Christmas dinner question,
26:05
is it? Or a sprout. Well, we should do
26:07
with a sprout this time. Yeah, it's no sprout.
26:10
Yeah, it would make more sense. I
26:13
want to take a moment to break from
26:15
the questions and reflect on the year in
26:17
space. So for the JOV, what have been
26:19
some of your favorite astronomy moments of 2024?
26:21
Well, mine's from the very start of the
26:23
year. I'm still not over it. And that
26:25
is that Neptune is not as blue as
26:27
we all collectively thought it was. Do you
26:29
remember this story? So wild. Yeah, so this
26:31
was, we met there was one in Oxford
26:33
actually, it was by Irwin and collaborators. And
26:35
the thing that makes me laugh about this
26:37
is that they started wanting to study Uranus
26:39
and then they were like, oh, this thing
26:41
about Neptune, and we're like, oh no. But
26:43
yeah, they were trying essentially to work out
26:46
sort of with the seasons on Uranus as
26:48
it orbits the sun. How does that the
26:50
color of Uranus change? And so to do
26:52
that, you need obviously like observations of Uranus
26:54
over the past like, you know, as many
26:56
decades as you can get your hands on
26:58
from the ground. But then essentially you need
27:00
to calibrate all of that data from the
27:02
ground with the voyage of probes fly by
27:04
of Uranus that actually took like true color
27:06
images, like true color images from. from Voyager
27:08
and they were like, oh okay, well we
27:10
should probably reprocess them ourselves again. And they
27:12
were like, wow we're here, we're doing Uranus,
27:14
should we do Neptune as well? We grabbed
27:16
the Voyager images and they did it and
27:18
they realized, oh. the true color of Neptune
27:20
isn't like the blue image that we you
27:22
know is like the image that you know
27:24
that you always show for Neptune and they
27:27
realize that NASA like very clearly communicated like
27:29
in the press conference from the voyage of
27:31
probes back at the end of the 80s
27:33
like oh hey we fiddled with the sort
27:35
of levels here and the saturation just to
27:37
show you the features in Neptune's atmosphere that
27:39
like Uranus is super smooth and Neptune has
27:41
all these features but and you can only
27:43
see them if we like with the levels.
27:45
And they released that image to be like,
27:47
hey look, you can see the features. And
27:49
people were like, great, that's Neptune. Yeah. And
27:51
like amazing blue color. And instead, like if
27:53
you actually make like a true color image
27:55
of Neptune, yeah, you don't see the features
27:57
as much because the color difference, you know,
27:59
isn't quite as apparent. But actually the color
28:01
looks more like what we're used to seeing
28:03
for Uranus. That's what hazy pale blue rather
28:06
than that sort of dark royal blue. But
28:08
that's Neptune's identity. Yeah, I know. I have
28:10
to reprogram my brain. Except that, no. That's
28:12
why it's, you know, it's, it's still, it's
28:14
like I'm in 11 months that I'm still
28:16
thinking about it. And Robert, how about you?
28:18
Well, hopefully not not. quite such a, you
28:20
know, traumatic also. No, I think, look, I
28:22
mean, this year, wow, we had two, just
28:24
two displays, the Northern Lights. Honestly, when does
28:26
that happen if you live in the South
28:28
of England? This is absolutely unprecedented. And we
28:30
had a bright comet as well, so, you
28:32
know, really brilliant, actually. It just shows what
28:34
I knew and my powers of prediction were
28:36
completely useless. Again. But wasn't there a clip
28:38
in the US though this year? I wanted
28:40
to be like... I wanted to be like...
28:42
I wanted to taste a trick from it.
28:44
Yes, because that was going to be one
28:47
of my highlights. That was going to be
28:49
one of my highlights. It was just like
28:51
honourable mention to you. Yeah, it's fair. I
28:53
know. I'm just resenting my colleagues across the
28:55
Atlantic who had that too. And the aurora
28:57
and the comet. But I loved... I also,
28:59
but not a discovery, but I did not
29:01
a discovery, but I did love the Jedi,
29:03
but I did, but I did, but I
29:05
did, but I did, but I did, I
29:07
did, I did, I did, I did, I
29:09
did, I did, I did, I did, I
29:11
did, I did, I did, I did, I
29:13
did, I did, I did, I did, I
29:15
did, I did, I did, I did, I
29:17
did, I did, I did, I did, I
29:19
did, I did, I It's taking a really
29:21
really powerful telescope and pointing it at something
29:23
familiar is great. It's always just fun as
29:26
well. Did you see the recent released a
29:28
sombrero image as well? I did. The sombrero
29:30
galaxy, sorry. Yeah, no, I'm a sombrero. I
29:32
can imagine hanging it in front of the
29:34
top. But that one was wonderful for
29:36
was wonderful for me
29:38
to see, because I
29:40
studied galaxies they're stuff. So
29:42
it was really cool
29:44
to see the differences
29:46
between the Hubble image
29:48
that you get, which
29:50
is just looking at
29:52
the the Hubble and then
29:54
the that image that
29:56
they released just at the
29:58
at the star light, and then that
30:00
was giving off by
30:02
dust that was glowing,
30:04
and it's a completely
30:07
different shape. Like, it's
30:09
completely lost that, like,
30:11
that shape that the
30:13
Hubble image dust famously has.
30:15
light So image that really
30:17
nice to see that,
30:19
you know, the dust
30:21
is doing very different
30:23
things to the stars,
30:25
which was quite cool. Yeah,
30:27
Yeah, very cool. back onto the back onto
30:29
the questions. a great we've had
30:31
a great question here from Instagram, Instagram,
30:34
the which is, do with an are there
30:36
jobs you can do with an
30:38
astrophysics degree outside of academia? to go
30:40
to both of you, think I'll to go to
30:42
both of you else to add. Yeah, if I
30:44
have anything else to add. this first. I mean,
30:46
the answer is definitely answer this first. mean, the
30:48
answer is definitely emphatically going to be working you
30:50
know, you're probably not going to be
30:52
working in astronomy, but hey, you know,
30:54
there's loads of things you can do
30:57
with it. with I mean, the big
30:59
secret is that most PhD students, let alone
31:01
let alone... astronomy and then graduates
31:03
go on to work in completely different areas.
31:05
That shouldn't really surprise us. Only a limited
31:07
number of hired astronomers or there's a vast
31:09
number of only a number of people
31:11
that are interested in it. And we at the
31:13
a actually collect examples every so often because we
31:15
wanna know what people are doing. And
31:17
the last time we did it, we found
31:19
people using their skills in this amazing number
31:21
of areas. And they were doing things like
31:23
data science in the to So no surprise And
31:25
kind of processing all these big data sets,
31:27
doing that in the home office so often because we
31:30
want to know cancer cells, you know, using machine learning
31:32
learning techniques to try and identify
31:34
cancer cells cells done that with done that
31:36
well It's just a as of just a
31:38
right? of imaging, right? Exactly, School teaching teaching definitely,
31:40
really inspiring for teachers, really good subject
31:42
for them, and even conserving paintings in the
31:44
National Gallery. I think even you know, it's
31:46
a fact that the technique is being
31:48
used in National a whole range of things
31:50
they could really do with them. So that
31:52
is a good course to do for that
31:54
reason, you know, you don't have to
31:56
use their skills in those areas, but you're
31:58
going to get do with them. degree. You're going to to
32:01
be a literate. literate. You're going to be
32:03
able to do a lot of different
32:05
things. if if good enough to do astrophysics,
32:07
you're pretty much good enough to try try
32:09
at a lot of other things, a too.
32:11
other I'm going to have to say, my
32:13
case, I'm not recommending, say, in my music,
32:15
for example, because the world say I doesn't
32:17
need that. But, know, example because the world really doesn't of
32:20
astronomers yeah but there are very of astronomers who do that very
32:22
not going to encourage me to sing.
32:24
I can encourage me to sing I can tell you. Becky will
32:26
come. I time will come promise that you ate is waiting.
32:28
yeah, I mean yeah I for this question,
32:30
though, I always say Astro is
32:32
basically is basically Like applied many things, right? things,
32:34
data science, science, problem problem solving,
32:36
applied software development as days as
32:38
well. Applied teaching, applied there's so
32:40
so many skills that you
32:43
learn from doing astrophysics. like Robert
32:45
was was saying, like you've been in
32:47
many different things. things. And I
32:49
mean, even I'm an example,
32:51
right? Fresh out of my
32:53
undergraduate degree degree and astronomy at
32:55
Durham, I got hired on
32:58
an engineering graduate scheme. graduate scheme,
33:00
right. So that was like in the world of
33:02
work in engineering and they of of their process was
33:04
like, yeah, we hire both physicists and engineers
33:06
because almost the physicists haven't learned the bad
33:08
habits at university. We could like train you
33:10
up fresh, you know, you know how we want want
33:12
you to be trained. obviously I realized that
33:14
wasn't for me and I did come back
33:16
to academia academia I have got mates that
33:18
did, you know, know physics astronomy at uni
33:20
with me that are in data science, teaching,
33:22
you finance, you know, there could be anything
33:24
from like and all and all the stats
33:27
that come with that to, you know, or
33:29
or anything like that medical physics Rob said, said, It's
33:31
just whether that's working with the big
33:33
machines the doing a lot of the sort
33:35
of research side of things for side of things for
33:37
of... sort of... skills you've learned from master physics.
33:39
people in publishing in well, whether that's
33:41
that's you know, publishing public science books,
33:43
like books, or books, or it's publishing, like,
33:45
as in academic publishing. people working in people
33:47
working in the civil service. people who've
33:49
got a friend that works at
33:51
the works at the right? Office, right? Because whether, again, again,
33:54
it's satellites, you're just pointing the
33:56
satellites in a different direction, right? looking
33:58
down at at earth not open to space. And
34:00
I I think one thing I want to
34:02
get across right now is that there is
34:04
a weird that of is a that of like idea that like
34:06
if you do that a you do degree like
34:08
a science PhD, and then you don't go
34:10
on to be a scientist. It's it's.
34:12
weirdly as a failure, don't see it
34:15
like that at all. that at like, I'm if
34:17
you wanna spend three years doing a PhD a
34:19
PhD in know, some area of research, or four
34:21
years doing an undergraduate doing you love the
34:23
subject and you think it's really cool and
34:25
you wanna contribute to the tiny, know, in
34:27
your tiny way to the sort of collective
34:29
human knowledge that we have, you know a great
34:31
way to spend three years of your life.
34:33
Do you know what I mean? And then
34:36
if you go on and do something else
34:38
that's another great way of spending to many years
34:40
of your life, of your life. That's great. It's
34:42
mine to change direction. I I totally agree because I
34:44
think, so I did did physics at Nottingham. I
34:46
I did a master's, I didn't do
34:48
a do a because I knew that
34:50
I didn't want to do a PhD,
34:52
a but I still loved physics. I
34:54
didn't let that. that... you know know, I
34:56
just thought of a different way that
34:58
made it more suitable to my skills
35:00
and what I could do. But I've
35:03
got friends that have gone on to
35:05
be that have gone attorneys and medical attorneys and
35:07
Some are doing coding for are doing coding for
35:09
like massive well. it's just like, and it's
35:11
This is just really, there are so
35:13
many skills that you pick skills that you pick
35:15
path from from to Google, by the way,
35:17
Google by the way is worrying if so up working at
35:19
Google. them working at Google. yeah, exactly. So I
35:22
think, I I mean, I think. I totally
35:24
agree with you you both that... if
35:26
you can get your head around around I
35:29
think you can get your head around
35:31
quite a lot of things and it's
35:33
totally fine if that is not something
35:35
in academia. and it's can make podcasts, if that
35:37
is not something in know. doing it, You but
35:39
not this one. hey, I'm not doing it,
35:41
but nod this one. Okay, just really contributing to
35:43
the whole, do you wanna be
35:45
when you grow up to the whole, a do
35:47
want to be can be anything you wanna
35:50
be. can be a they say, You an
35:52
astrophysics degree and then do a want
35:54
they'll blame you, is he? Yeah, hey, that's
35:57
fine, it's It's fun.
35:59
Okay, so Becky can you help with
36:02
this follow-up question from Sam after listening
36:04
to our fast radio bus episode and
36:06
they've written to say After listening to
36:08
your podcast on fast radio bursts, I
36:10
would like to know more about how
36:12
experts decide where to look for fast
36:14
radio bursts. Your guest Stuart mentioned being
36:16
able to get time on JWST and
36:18
a sample skyshot, but since FRBs are
36:20
so short and so unpredictable, how do
36:22
experts decide where to aim? Yeah, so
36:24
I mean, it's a great question, Sam,
36:26
so the big radio telescopes that detect
36:28
these flash radio bursts like... they don't
36:30
aim right they stare at the biggest
36:32
patch of sky that they count at
36:34
one time in the hope of detecting
36:37
one and the hope of you know
36:39
pointing in the right direction at the
36:41
right time and but you know they
36:43
could easily be missing so many fast
36:45
radio bursts in a night just because
36:47
wrong place wrong time right In terms
36:49
of J-D-B-S-T follow-up, like the field of
36:51
view of J-D-B-S-T, compared to a radio
36:53
telescope, it's really, very small, right? This
36:55
isn't something you can, like, you can't
36:57
search for F-R-B-s in the hope of
36:59
detecting one with J-D-B-I-I-T, because you just
37:01
can't mobilize the telescope quick enough to,
37:03
like, What it's more about is finding
37:05
the host galaxy that the fast radio
37:07
burst has gone off in. So whatever
37:09
object is producing this fast radio burst,
37:12
which galaxy does it live in basically?
37:14
And oftentimes there doesn't seem to be
37:16
a galaxy in the direction that the
37:18
fast radio bursts seems to have come
37:20
from, at least in sort of like
37:22
the archive imaging we have from like
37:24
ground-based telescopes, right, that obviously, you know,
37:26
can't see things as faint as JDAST
37:28
counter in any sort of resolution. So
37:30
what we do with JDAUST is this
37:32
sort of, as you said, like a
37:34
sky shot where we point JDAUST in
37:36
the direction we think that the fast
37:38
radio radio bursts has come from and
37:40
just sort of like collects as much
37:42
light as much light as possible as
37:44
possible and be like possible and be
37:47
like Is there a galaxy there that
37:49
we can now? to take the generous
37:51
tea. Or sometimes we do find that
37:53
there's a smudge of a galaxy there
37:55
in the direction we think the fast
37:57
radio verses come from, but we don't
37:59
know the distance very well because again
38:01
we can't really resolve it. We've not
38:03
been able to get what's known as
38:05
a spectrum where you take the light
38:07
and you split it into its like.
38:09
trace of how much light each wavelength
38:11
you're receiving. And from that you can
38:13
pinpoint things to say how much has
38:15
the light been redshifted by the expansion
38:17
of the universe to work out how
38:19
far away it is. And so with
38:21
JWST we can actually look at their
38:24
galaxy more detailed, get that spectrum that
38:26
we need to pinpoint where the fast
38:28
radio burst is coming from and how
38:30
far away it is. And that gives
38:32
us a lot of information because if
38:34
we know how far away the fast
38:36
radio burst is, then from how bright
38:38
it appeared to us when it went
38:40
off. and so we can put some
38:42
limits on like how much energy was
38:44
involved in the production of this fast
38:46
radio burst and things like that. That
38:48
gives us a better idea of like
38:50
what's producing them, you know, is it
38:52
magnetars, like everybody suspects. And also perhaps
38:54
if that's changing with how distant we
38:56
go out as well and with how
38:59
distant we find fast radio bursts, is
39:01
there different things that produce them and
39:03
does that change with time in the
39:05
universe? Like lots of questions like that.
39:07
Amazing, thanks Becky. And Robert Lucy on
39:09
Instagram asks, why can't we predict or
39:11
understand the sun's magnetic field? Yeah, thank
39:13
you Lucy. When I read this I
39:15
thought, how is that Lucy Green's solar
39:17
physicist who I know quite well, trying
39:19
to catch me out, but probably not.
39:21
She's secretly marking you. Exactly. I definitely
39:23
feel judged. I definitely feel judged. But
39:25
it is a very fair question. I
39:27
mean, the answer is we can predict
39:29
the 11-year solar cycle of activity reasonably
39:31
well. So we know that the number
39:34
of sunspots rises and falls over that
39:36
time, and then when there are a
39:38
lot of sunspots, the sun is generally
39:40
more active, so there are more There
39:42
are more coronal mass ejections when big
39:44
eruptions of material are rejected in space
39:46
and those rise and fall over that
39:48
time. And then a new cycle begins
39:50
with the poles of the magnetic field
39:52
reverse. So you go north to south
39:54
and south to north. And right now
39:56
we are at solar maximum. That's why
39:58
we've had two major... displays of a
40:00
roaring this year. we've
40:02
also already we've signs seen signs of the
40:04
next up and there up, and there was a
40:07
researcher presenting at our National Astronomy meeting in Hull back in
40:09
in July. details are But the details are
40:11
much, much harder. And I remember a
40:13
decade ago harder. And I physicists were absolutely adamant
40:15
that solar activity was headed to record
40:17
lows. And that was going to happen
40:19
in the next few years, and it
40:21
was going to be like the kind
40:23
of very low numbers we saw back
40:25
in the few years. And it century, was going long
40:28
after people kind started observing the we saw back
40:30
in the 17 telescopes and it didn't work out
40:32
like that like know it was low was
40:34
it's high again high again we also also... definitely
40:36
predict exactly when a large when a large is
40:38
going to produce a flare you know
40:40
we see them a don't know exactly
40:42
when they're going to eruptive at all
40:44
when a coronal mass ejection will happen at
40:46
direction it'll take ejection we can only
40:48
guess that it'll probably be only guess we
40:50
see a big Sunspot group in the
40:52
first place we just don't know exactly
40:54
when group that's because the Sun is not
40:56
this sort of super smooth that's because the
40:58
model not this a of plasma to model particles
41:00
of fields, currents of material, you know, know,
41:02
flows in and out of the atmosphere, in and out
41:04
of the and under even tornadoes on
41:06
and under its surface, and trying to
41:08
work out how that that we together
41:11
is really hard. processes that the sense that
41:13
we don't understand a lot of
41:15
the processes that make it happen on
41:17
a or but understanding will predicting how
41:19
it will change over time is quite
41:21
hard. So we do understand how
41:23
the magnetic fields work. We do understand
41:25
that, you know, the interaction with
41:27
charged particles, the fact they're tied together
41:29
with electromagnetic forces, that's okay. But trying to But trying
41:32
to estimate those long is trends is
41:34
really very, very difficult that that cycle or cycle
41:36
or 22 -year cycle, if you prefer, you
41:38
know, when the polls go know, when the the back
41:40
to the position they were in before.
41:42
you know, So Lucy, you know, frankly, doing, but if
41:44
I don't know what you're doing, a
41:46
but if you take up a solve this problem,
41:48
then you solve this problem, on probably be
41:50
on your way to for a a Nobel
41:52
because because astronomers are really struggling with
41:54
it. with it. Okay and Becky we I'm thinking
41:56
we have another black coal question
41:58
for you. you. Amazing. Yeah. Obviously. Abby Girl
42:00
Smith says, hi, love of the podcast.
42:03
My question is, why do black holes
42:05
expand and shrink? Oh, good question. So,
42:07
I mean, expand and shrink. I think
42:09
you mean they're like the size of
42:11
them. So like the size of the
42:14
event horizon, which was like inside that
42:16
we class as the black hole, right?
42:18
So the size of the event horizon
42:20
is actually correlated with the mass of
42:22
the black hole. So how heavy it
42:24
is. Blackhaws expand if they grow in
42:27
mass. So if they take in more
42:29
material over time, so we see that
42:31
in what we call x-ray binaries where
42:33
you've got two stars that are orbiting
42:35
around each other, one goes supernova, becomes
42:38
a black hole, and the other star
42:40
is close enough to start almost like
42:42
feeding the black hole and like the
42:44
black hole is material off that one.
42:46
And so in that respect, the black
42:48
hole will expand its radius, its vent
42:51
horizon will grow, and therefore... the black
42:53
hole is expanding if you will as
42:55
it's growing in mass. Shrinking however is
42:57
an interesting question because you think okay
42:59
well if black calls expand because they
43:02
get heavier then they should shrink when
43:04
they get lighter and they lose mass.
43:06
But the whole point of a black
43:08
hole is that all the material and
43:10
the light and everything is trapped there
43:12
right? That's the point of a black
43:15
hole. However, enter Stephen Hawking stage left
43:17
because Stephen Hawking was very concerned about
43:19
like the fact that black holes seemed
43:21
to break one of the fundamental laws
43:23
of physics, the fundamental laws of thermodynamics,
43:26
right? And is that entropy, it's almost
43:28
like the chaos in the universe should
43:30
increase over time, whereas black holes that
43:32
they're sort of like the Marie condos
43:34
of the universe. They really organize little
43:36
boxes, right? And the entropy seems to
43:39
go down. And so when he was
43:41
looking at the mass of trying to
43:43
figure this out, he sort of came
43:45
up with this hypothesis that essentially there's
43:47
sort of like an interaction of the
43:50
black hole with sort of what's going
43:52
on in terms of quantum physics, sort
43:54
of in this sort of like vacuum
43:56
energy of space. I won't go into
43:58
the details here because it gives me
44:00
a headache every time I try and
44:03
it takes me a good chapter of
44:05
a book every time I try to
44:07
explain this. But essentially what happens is
44:09
you then get radiation given off at
44:11
the event horizon of a black hole.
44:14
You get like a pair of particles
44:16
created, one of which escapes and one
44:18
of which ends up going back into
44:20
the black hole. As Einstein told us,
44:22
E equals MC Squares, if you've got
44:25
lights, energy, escaping, you've also got mass
44:27
escaping. So Stephen Hawking's theory is that
44:29
you have what's known as Hawking radiation
44:31
that allows the black coal to evaporate
44:33
over time or to shrink, as Abigail
44:35
put it, right? That, however, is still
44:38
just complete hypothesis. Like those papers were
44:40
published in the early 70s. We have
44:42
no observational evidence that this does happen.
44:44
that we've ever detected like this kind
44:46
of radiation that you could get from
44:49
a black hole. It could just be
44:51
that it's so red that this ever
44:53
happens that of course we haven't ever
44:55
detected it yet or there's not a
44:57
black hole close enough for us to
44:59
detect the tiny amount of radiation that
45:02
you would expect. Maybe if there's a
45:04
planet 9, 9, that's a planet of
45:06
the source system that would be an
45:08
ideal place. That would be an ideal
45:10
place to test for this system. That
45:13
would be an ideal place to test
45:15
for this as well. We know what
45:17
about calls expand, whether they can shrink
45:19
or not is another thing entirely. Okay,
45:21
thank you. And a final one for
45:23
both of you from Samdowns on Instagram,
45:26
do you think there are aliens out
45:28
there? Robert? You know, I kind of
45:30
do, but with the caveat that they
45:32
might be really simple aliens, you know,
45:34
really much harder question is whether there's
45:37
any advanced life, even remotely like us,
45:39
which might be extraordinarily rare. I mean,
45:41
I have to say a cause as
45:43
well, we... At this point in time,
45:45
we haven't found any evidence for any
45:47
life. There's no hard evidence anyway. We
45:50
found hints of things, you know, we
45:52
found worlds that could support it, chemical
45:54
processes that allude to it, but no
45:56
more than that. So, you know, we're
45:58
a long way. from this. this.
46:01
But you know, they're not here. The They're
46:03
not here. The Fermi paradox is
46:05
is applying, know, the aliens haven't haven't
46:07
visited the earth, whatever, whatever you might on
46:09
on some channels. And that's not really
46:11
surprising given how big how are. It's
46:13
a really difficult thing to travel between
46:15
the stars. to travel between the
46:17
stars. Becky. Sorry, one second. some
46:19
strange noise a now I'm convinced that the
46:22
cat's in here with me. The cat
46:24
is in there because I saw it
46:26
in here with me. The cat is in there because I saw
46:28
the background. walk open! Oh, didn't even rail phone.
46:30
Yeah, I saw her watching in the background. Yeah,
46:32
your cat saw her cat used to, my
46:34
cat, I can't use to play
46:36
the piano her by walking, that used
46:38
to terrify me Yeah, your cat is in the
46:40
on the far back of the
46:42
sofa? used to play the piano at that was
46:44
That interrupted your previous answer, being
46:46
like, oh, hello. Anyway, pips in the room. Aliens aren't
46:48
in the room with us, but the cat in the
46:50
room. with aren't in the room
46:52
with us, but the cat is. has
46:54
to be I agree with has I
46:56
think... on another has to
46:59
be life that has started on
47:01
another planet in our own in the universe.
47:03
the Whether that's in our don't the Milky
47:05
Way, I don't know, or, you know,
47:07
more likely a I think I think just
47:09
because everything we see see it comes
47:11
to life, life, like... Do I? She's scratching it again again.
47:13
Like, tar degrades, like surviving in, you know, the
47:15
vacuum of space on the outside
47:17
of the interstellar space station. Space We
47:19
recently saw that, you know, saw that, you
47:22
a a chunk of asteroid that we
47:24
brought back from the asteroid on the right,
47:26
on the Hayabusa -2 mission, Jax's
47:28
mission went to the asteroid and brought it
47:30
back to brought it back to Earth. Earth life colonised
47:32
the surface of that of that asteroid and
47:34
quickly and very happily. you know, alien
47:36
rock that know, alien rock to, has
47:39
never been exposed to, you
47:41
know, a clean room and been in a
47:43
clean room it's got got slight
47:45
contamination that all of a sudden
47:47
just proliferated. So. So think
47:49
as Ian Malcolm and Jurassic Park so wonderfully
47:51
puts it, life puts it, life way, away.
47:54
And I and I think it would
47:56
be very rare indeed if nothing, if we'd
47:58
be the only one. you know. where those
48:00
conditions are right. I think if you think about
48:02
the numbers of how many stars there are and how
48:04
many galaxies in the universe and how many planets they
48:06
must have, blah blah blah. Yes, I think life must
48:09
exist somewhere, but I do not think that they have
48:11
visited us. at all. Okay, well we'll be getting into
48:13
that topic more in January 2025. I'm so excited.
48:15
So thank you to everyone for your questions. Do keep
48:17
sending them in. And Robert, as always, what can we
48:20
see in the night sky over the holidays? Over the
48:22
holidays, well, the bleak mid-winter, you know, accuse carols or
48:24
something, I'm not going to sing. But it is just
48:26
after the December solstice. So for the Northern Hemisphere, it's
48:28
the longest nights the year, pretty much. the other way
48:31
around if you're in the southern hemisphere, wherever you
48:33
are in the word, Ryan is now really dominant in
48:35
the late evening, so I have the brightest consolation, the
48:37
whole sky, two first magnitude stars, Beekle, Juice, and Rigel,
48:39
the belt term, you know, a wonderful thing to see,
48:42
particularly, it's a signpost of the stars around it, so
48:44
you can, you know, you can follow up and
48:46
down and all that kind of thing. do look at
48:48
the Nepidr under the belt and definitely have a look
48:50
around if you were given a pair of binoculars that
48:52
we recommended for Christmas, you know as a potential gift
48:55
or maybe you got some for yourself or borrow some
48:57
but you know really opens up your enjoyment of it.
48:59
Why are you there if you're in the Northern Hemisphere
49:01
look down from the belt stars down to Sirius
49:03
which is the the brightest star in the whole night
49:06
sky. Now apart from that Jupiter is sitting above Orion
49:08
and Taurus it's completely look at it, look at the
49:10
belt, the weather systems. And you might also, if it's
49:12
half decent, be able to see things like the moons
49:15
passing in front of it and their shadows. And
49:17
I was looking up, there's a predictor on the Sky
49:19
and telescope website, which we should probably link to actually,
49:21
but on Boxing Day, the closest in Moon IO does
49:23
this for people in the UK, starts at 816 in
49:25
the evening and it moves away by 1048. So it's
49:28
really well placed. So if you have a clear sky
49:30
that night. have a look. It's really quite a nice
49:32
thing to see the shadow moving on and off.
49:34
Venus is high in the sky after sunset, looks slightly
49:36
fatter than a half moon through a telescope, obviously dazzlingly
49:39
bright, and it's good for the next couple of months.
49:41
And if you're up before dawn, and you've got a
49:43
good for the next couple of months, and you've got
49:45
a good for the next couple of months, and
49:47
you've got a good for the next couple of months,
49:49
and if you're up before dawn, and you've got a
49:52
good for the next couple of your up before dawn,
49:54
dawn, dawn, you've got a good for the next couple
49:56
of the next couple of a good for the next
49:58
couple of months, dawn, dawn, dawn, and if you've
50:00
got a good for the next couple of a good
50:03
for the next couple of a good for the next
50:05
couple of a dawn, dawn, dawn, dawn, dawn, dawn, dawn,
50:07
dawn, dawn, dawn, and if you've got a good for
50:09
the next couple of a good for the And finally,
50:11
do look out for the quadrantids meteor shower that's peaking
50:14
on the night, the second to the third of January,
50:16
more or less, it depends on where you are
50:18
in the world. It's very, very sharp in its peak
50:20
and that's actually best for the Pacific this year. But
50:22
even if you're in the UK, you might see say
50:25
25 meteors an hour and helpfully the moon is a
50:27
thin crescent, a waning thin crescent, so it won't interfere
50:29
too much. Now I have to say I've always
50:31
really struggled struggled to see it. Not always what it
50:33
could be. What are you talking about? I'm going to
50:36
try again. I'm going to try, I'm determined to try
50:38
again and I encourage you to do the same. Do
50:40
go and have a look, you know, wouldn't it be
50:42
great if we actually got that? It's really quite a
50:44
strong shower. It's just, I've never managed to see it
50:47
in 50 years, well maybe not 50 years, 40
50:49
years of trying. I have something to add to this
50:51
as well for the Christmas star gazing period. I want
50:53
to give a warning. to all the parents of children
50:55
out there that the International Space Station can look very
50:58
convincingly like Father Christmas's sleigh. And I wouldn't want anybody
51:00
to confuse the two because it was very fast,
51:02
it's very bright. So there is actually an International Space
51:04
Station Passover of the UK at 6am on Christmas morning.
51:06
So if you have been... gotten up that early because
51:08
you have children maybe a little look out of the
51:11
window to see it passing directly overhead just past six
51:13
o'clock and you know just be very careful that
51:15
your children don't confuse it for Santa Claus because I
51:17
obviously wouldn't wouldn't want that. to to happen.
51:19
a good public health a good a
51:22
health warning. They're public safety if
51:24
you'd like if you'd like to
51:26
know own own that no that
51:28
no confusion happens, spot station from NASA is
51:30
the the website that you
51:33
should Google, or you can put
51:35
in your area and see
51:37
where to look and when
51:39
to look as well. as well. Yeah.
51:41
it's brilliant. Well I think that's I
51:44
think that's it for
51:46
this episode and for this
51:48
year. be back in be back in
51:50
a month's time with the with
51:52
the search for life. will come
51:55
back with that. It is
51:57
gonna happen. We've said it
51:59
so much that it's We've have
52:01
to go and find
52:03
people to talk to. I have to
52:05
people to talk to, the
52:08
people to talk to are
52:10
like, sorry, we're busy with
52:12
searching for the alien life.
52:14
the people to talk to say. like
52:16
sorry will get that to
52:19
you. But thank you to
52:21
everybody who sent in questions
52:23
for this episode. I really
52:25
enjoyed this episode. Thank you
52:27
so much. We do have
52:30
a growing pile of questions we
52:32
we will keep adding
52:34
to it as well. So
52:36
please do because we have
52:38
these bonus episodes, right, where
52:41
we always do the Q &A
52:43
as well. the So if
52:45
you have a burning question
52:47
for the team, email it
52:49
to team, email it to .at at r-a-s.ac.ac.uk or
52:52
you you can find us
52:54
on on Instagram at Super Massive Pod and we'll of
52:56
course try and cover your
52:58
questions in a future episode.
53:00
episode. if I can be
53:02
really cheeky and ask for a
53:05
a Christmas present for us, us,
53:07
if if anyone wouldn't mind
53:09
rating and reviewing the podcast
53:11
and it really helps really we
53:14
love seeing all of your
53:16
your So thank you So
53:18
already done that. That's already done that.
53:20
we will be back with
53:22
more episodes for you in for
53:24
you as well. but then, everybody,
53:27
happy holidays and most importantly,
53:29
importantly, happy start gazing.
Podchaser is the ultimate destination for podcast data, search, and discovery. Learn More