Episode Transcript
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0:02
The cosmic web is kind of like the
0:04
skeleton of the universe. The
0:06
clusteriest of clusters and the voidiest of
0:08
voids is the things that come to
0:10
mind, right? If you get things that challenge
0:12
that, well then we just rethink the physics. Hello
0:19
and welcome to the Supermassive podcast
0:21
from the Royal Astronomical Society with
0:23
me, science journalist Izzy
0:25
Clark and astrophysicist Dr Becky Smithers.
0:28
This month we're untangling the cosmic web,
0:30
not the James Webb Space Telescope, but
0:32
the large scale structure of the universe.
0:34
What do we know about it and
0:36
what can it tell us? Yeah, I
0:38
just thought it was about time we
0:40
got into something really complicated because we'd
0:43
just be taking a bit too easy
0:45
with all this planetary science and our
0:47
tour of the solar system. What, is
0:49
your head not hurt very recently Izzy when you've
0:51
been recording? No, I'm due another headache so here
0:53
we go. As always,
0:55
Dr Robert Massey, the deputy director of the
0:58
Royal Astronomical Society is here. So Robert,
1:01
how would you describe the
1:03
cosmic web? Because it
1:05
might not be something that everyone is
1:07
familiar with. So let's begin this brain
1:10
stretch right now. Exactly. Brain stretch
1:12
headache questions that I struggle to answer.
1:14
You know, everything that makes a good
1:16
Supermassive episode. The good question. Exactly. The
1:18
good questions. The good questions. Yeah.
1:20
So look, I mean, if you take a kind
1:22
of casual look at the sky, a very quick
1:24
line of sight, you think, okay, randomly distributed stars,
1:26
but even in our own galaxy, you look a
1:29
bit longer, you see the band of the Milky
1:31
Way. So you can quite easily deduce there's some
1:33
structure in the way the stars are distributed. And
1:35
if you look on a much bigger scale, if
1:38
you map galaxies on a huge scale and you
1:40
do that in 3D, then it turns out they
1:42
grouped into these huge clusters and those clusters are
1:44
on this filaments of this giant web. And there
1:46
are these filaments and voids and
1:48
that's the sort of bubbly structure of the
1:50
universe on the bigger scale. And we didn't
1:52
know about it until the 1980s because that
1:54
was when we got better telescopes and we
1:56
were able to measure those distances more reliably
1:58
and push them out further. than before. And
2:00
those galaxies, the galaxies like the one we live
2:03
in, they're concentrated into these huge clusters. They tend
2:05
to be concentrated along the nodes or the knots
2:07
and strands of the web. And they're around voids
2:09
where there are far fewer of them. And these
2:12
are really big. These are billions of light years
2:14
across. So they're certainly the biggest
2:16
structures in the whole universe. So understandably, there's
2:18
a lot of interesting understanding things on the
2:20
biggest scales. Yeah. I like to joke that,
2:22
you know, instead of like turtles all the way down, it's just filaments
2:24
all the way. It's exactly filaments, bubbles,
2:27
soap, what do you describe it as?
2:29
I don't know, soap or spongy or
2:31
something like that. Yeah. I've always looked at it as
2:33
like a big sponge. Right. And I like how you were
2:35
saying, you know, we didn't discover this to the eighties because
2:37
we almost couldn't zoom out far enough to see it. Right.
2:40
Cheers Robert. We'll catch up with you later in
2:42
the show for some more questions. And this month's
2:44
stargazing tips. So buckle up everyone.
2:47
The mind stretching continues because we're going to
2:49
dive into the world of cosmology. So far,
2:51
we've sort of talked about the structure of
2:53
the cosmic web, but you're about to hear
2:55
a little bit more on that. Why
2:58
is it important and what is it made
3:00
of and where the heck has it come
3:02
from? These are all questions that I
3:04
put to Dr. Kiara Mingarelli from Yale
3:07
University. The cosmic web is the name
3:09
that we give to this structure
3:12
that we can see on very large
3:14
scales, on the largest scales. So
3:16
let's just start where we are right now
3:18
and then zoom out. Okay. So we're
3:20
on the earth. We're in the Milky
3:22
Way galaxy. Next door is the Andromeda galaxy,
3:25
but we're part of a galaxy
3:27
cluster. And then if you zoom out of
3:30
our galaxy cluster, far away,
3:32
there's another galaxy cluster. And there's like
3:34
these filamentary structures that can connect these
3:36
galaxies. And then if you zoom out
3:38
again, you can see even
3:40
more galaxy clusters with more of these filamentary
3:43
structures that connect them. So they kind of
3:45
looks like a brain with all
3:47
of these bundles of neurons that are
3:49
sort of talking to each other. Now, I'm
3:51
not saying that we can talk to each
3:53
other through the cosmic web, but we are
3:55
all connected. And so it
3:58
begs the question, like, why is that? there and
4:00
how did that form? Okay, so we've got
4:02
this big connection of galaxies, galaxy
4:04
class A. I can just picture this like we
4:07
start as a little spot and we move out
4:09
and we've got this, I don't
4:11
want to say a tangle, but it's
4:13
kind of like a tangle. Some people
4:15
might want to think of it as
4:17
like a net kind of structure. That's
4:19
exactly right. So to picture this, is
4:22
it a physical structure? What is it made
4:25
of? Do we know? Right.
4:28
So it's kind of like the skeleton
4:30
of the universe, right? If you were
4:32
to take this kind of skeleton and
4:34
then paint on hydrogen gas, then you
4:36
would see it. And so
4:38
it's mostly made up of gas, like
4:41
the filamentary structures are really largely made
4:43
up of gas. But then
4:45
the big nodes, you know, that are the things
4:47
that are being connected, there's a
4:49
lot of hydrogen, but then you have
4:52
other heavier elements that help to make
4:54
up galaxies. And that's all formed by
4:56
the early stars. So the earliest stars
4:58
were only made up of hydrogen, because
5:00
that's like a primordial element that was
5:02
there in the beginning, hydrogen and helium.
5:04
And then as stars burn, they can create
5:07
these heavier elements. And so everything that we
5:09
have was created in these
5:11
early burning stars, and then in supernova
5:13
explosions. And then recently, we also know
5:15
that some of the heaviest elements like
5:18
gold and platinum were created
5:20
by merging dead
5:22
cores of stars called neutron stars.
5:24
That's also really exciting. Where
5:27
has this come from? Where does this begin?
5:29
How do we even begin to unpack this?
5:32
Yeah, that's a great question. So
5:34
it all started about 380,000 years
5:37
after the Big Bang. There was
5:39
this cosmic soup, and
5:41
the universe was so hot, that
5:44
light and particles that make
5:46
up you and I like protons and neutrons
5:48
and you know, things that we call baryonic
5:50
material, which is just stuff that you can
5:53
touch with your hands, right, your desk, your
5:55
watch, your headphones. All of this
5:57
was in this primordial goop, right, which includes
6:00
It was so hot that even light couldn't escape
6:02
from this really hot soup. And
6:04
inside of this soup, there were
6:06
quantum fluctuations from the big bang that
6:09
had been amplified by inflation in the
6:11
early universe. Right after the big bang,
6:14
about 10 seconds, the universe inflated to
6:16
be an enormous size compared to what
6:18
it was. And so the
6:20
small fluctuations that had happened right at the
6:22
quantum level after the big bang
6:25
then became huge, right? Because everything expanded
6:27
in all directions. And so those
6:29
tiny little fluctuations are now really big. And
6:32
so some of them are
6:35
troughs and dark matter can
6:37
go into those troughs. And
6:40
it forms these places that then regular matter
6:42
wants to go later. So when
6:44
the universe can cool down and then
6:46
light can finally escape from this
6:48
cosmic soup, we get the
6:51
cosmic microwave background that maybe some of
6:53
the listeners are familiar with. It's at 2.7 degrees Kelvin. But
6:57
where I was going with this is that
7:01
those fluctuations created these little nests
7:03
for regular matter to fall into
7:05
and to cool off. And that's
7:08
how we formed galaxies
7:10
and galaxy clusters. And
7:12
so these little cosmic potholes that were
7:14
really tiny at the beginning of the
7:17
universe and then grew to enormous sizes
7:19
now are the homes of lots
7:21
of regular baryonic matter, including and
7:23
also dark matter that surrounds them.
7:26
So it's like the dark matter is their
7:28
house. Yeah. Right. And then all of the
7:30
baryonic matter goes inside and then
7:32
it forms all of these structures as it cools
7:34
down, but it has to cool down because when
7:36
it's hot, stuff is moving everywhere, but as it
7:38
cools down, then it can like go to its
7:41
neighbor's house, see what's going on,
7:43
find out what's happening. It can get
7:45
together in little groups and then you
7:47
can form galaxies and then galaxies can
7:49
eventually merge and they get bigger and
7:51
that's how we think the universe works. A
7:54
nutshell. Yeah. Okay. Thank you. Just blow
7:56
my mind. Thanks very much. I
8:00
think this is a really interesting idea.
8:02
So we're saying we've got these pockets
8:04
of matter essentially, and that's where we
8:06
have our galaxies forming and clustering together.
8:08
And so are we saying like
8:11
matter can travel between these webs
8:13
from say one little cluster of
8:15
galaxies, say over here in the
8:17
left to say another one
8:19
over here on the right, you know, obviously
8:22
we're talking about astronomically massive scales, but they
8:24
are connected. They can, what
8:27
matter flows through them, is it correct to
8:29
say that? Well, it's
8:31
hard to say if it's flowing or not,
8:34
because in order to see any kind of
8:36
flow, we would have to observe it moving.
8:38
Okay. And these distances are
8:40
so vast that it's kind
8:43
of like trying to watch
8:45
a turtle go 100 kilometers and
8:48
you're wondering like, can the turtle actually travel that far?
8:50
And then if you just watch the turtle for
8:53
a second, you're like, this turtle doesn't move.
8:55
But if you give it enough time, it's
8:57
gonna move and it can go a hundred
8:59
kilometers, right? I'm Canadian. And so I tend
9:01
to use the metric system. Hey,
9:04
we're all fine with that. That's right.
9:06
Okay, good. So it's
9:08
really a time scale issue. We certainly
9:10
know that we can see the filaments,
9:13
which means that there's at least hydrogen
9:15
gas in those filaments, but
9:17
you know, which way it's flowing and if
9:19
it's flowing or if it's just there, it's
9:22
kind of hard to say. Are universes expanding?
9:24
So what does that mean for the cosmic
9:26
web? And how do we
9:28
know how that interaction plays out or
9:30
how does that interaction play out if
9:32
you've got galaxies merging as well? Right,
9:35
that's a great question. So each
9:37
one of these nodes has
9:39
galaxies in it and they're all
9:42
gravitationally bound, these galactic super clusters.
9:45
And so the force of gravity inside
9:47
of those is stronger than the acceleration
9:49
of the universe. But what
9:51
that means is that eventually we're gonna
9:53
get really far away from the other
9:55
super clusters. And so like these filaments
9:57
are gonna get thinner and thinner and...
9:59
and thinner as we move further away.
10:02
So imagine a piece of toffee
10:04
getting thinner and thinner and thinner as
10:07
it goes. And eventually, there won't be
10:09
anything left. We can already
10:11
see some of these superclusters accelerating away from
10:13
us. And so in
10:15
the future, if we as a species
10:18
can survive another 100 million billion years,
10:21
what we see today is going to be
10:23
completely different from what our descendants will see. We
10:26
might be very much alone in a little
10:29
island in our little supercluster, because the other
10:31
ones will have accelerated away. So
10:33
does this mean that as our universe
10:36
expands, the formations
10:38
of galaxies, does that slow down? They're
10:40
not going to have that, I
10:43
want to say, swap of hydrogen
10:45
to help continue to build
10:47
them. Is that what we're talking about here?
10:50
Well, so what we're talking about is
10:53
competing forces. So we know, for
10:55
example, the universe is expanding right
10:57
now. But we're humans,
10:59
and we're here, because the forces
11:02
that keeps ourselves together is stronger
11:04
than the force of gravity that's
11:06
expanding everywhere. And so
11:08
similarly, in our supercluster right now,
11:11
the force of gravity and all of the
11:13
dark matter that's holding us together is stronger
11:15
than the expansion of the universe. It's making
11:17
everything else fly out. But
11:20
eventually, what will happen is something called
11:22
the heat death of the
11:24
universe. And that means
11:26
that eventually, the galaxies will all
11:28
merge, they're supermassive, black holes will
11:30
merge, all of the stars will
11:33
eventually burn out, and we'll have
11:35
just a black hole universe, where everything is
11:37
in some sort of black hole. And
11:39
then the black holes start to evaporate. And
11:41
that takes a really long time. They
11:44
emit something called Hawking radiation. But
11:47
all that means is that they eventually lose all
11:49
of their mass to radiation. And
11:51
the universe just becomes this cold, dead
11:53
place. OK.
11:56
I mean, it sounds lovely. Doesn't it?
11:58
Yes. Yes. Exactly. How
12:02
much can we actually know
12:04
about, because obviously
12:07
a big part of this is dark
12:09
matter. So can
12:11
we study it or does that depend
12:14
on being able to detect dark matter,
12:17
which in itself is a whole other
12:19
podcast episode? Yeah,
12:21
we can study it in different ways.
12:23
We can study the cosmic web by
12:26
looking at large surveys of
12:28
galaxies. We have really big
12:30
telescopes that look at the sky and
12:33
then we can map the sky and
12:35
we can see these filamentary structures emerging
12:37
so we can actually see the cosmic
12:39
web. We can also
12:42
make large computer simulations like
12:44
Illustris. And if you
12:46
look up Illustris on the internet, you can
12:48
find lots of beautiful animations that show you
12:50
where the dark matter has to be, where
12:52
the regular matter is. And
12:54
then what's really amazing is that you
12:57
can match the two, that
12:59
these simulations have to match what we
13:01
actually see with our telescopes in order
13:03
to be credible. So
13:06
one of the fun things you can do with the simulations
13:08
is that you can turn off dark matter. And
13:11
then what you see is that you can't make a universe.
13:13
There's no scaffolding. There's no skeleton for
13:16
the matter to clump on and cool
13:18
down on. There's no little house that
13:20
all the baryons can go into and
13:22
chill out. Right? Like they're just kind
13:24
of floating everywhere. And
13:26
it's really difficult to create any kind of
13:28
large scale structure, as we call it, which
13:31
is this cosmic web. Oh,
13:35
I really enjoyed speaking with Kiara. Yeah, she's great.
13:37
Yeah, yeah. It's so good. We've got part two
13:39
of an interview with her coming up in just
13:41
a moment because there was literally too much to
13:43
cover. Turns
13:45
out covering the biggest thing in the
13:47
entire universe. It's quite difficult. It's quite
13:49
difficult. Yeah. So
13:52
Becky, some follow up questions to that.
13:54
How important is dark matter for
13:57
this web light structure? I
14:00
mean, it literally wouldn't exist without it.
14:02
So dark matter, I think it's often
14:04
referred to as like the scaffold of
14:06
the cosmic web, right? It holds galaxies
14:08
together and it holds together clusters of
14:10
galaxies as well. And therefore,
14:12
if you keep going on that, it holds
14:14
together the whole structure of the web. So
14:16
without it, in just a
14:18
few billion years, those structures would completely disperse,
14:20
right? And it just wouldn't be held together
14:23
anymore. And that's because gravity just wouldn't be
14:25
strong enough to hold it together against all
14:27
the random motions that these galaxies have in
14:29
different directions, right? Like we talk about sort
14:31
of like redshift when we look out into
14:33
the universe, right? And all the galaxies appear
14:36
to be moving away from us, but that's
14:38
like an overall global thing that's going on
14:40
or universal thing that's going on. But like
14:42
think about how Andromeda is actually coming towards
14:44
us, towards the Milky Way, because in our
14:46
little local group, everything's got random motions
14:49
with respect to each other. Yeah. And
14:51
so it's the dark matter that sort
14:54
of pervades this entire structure and sort
14:56
of connects galaxies along these
14:58
filaments that holds everything together. And it's just
15:00
without it, it'd be like a whole house
15:02
of cards that falls apart. This is one
15:05
of the actual like big
15:07
pieces of evidence we have for dark matter
15:09
is that we can't get the
15:11
universe to exist and to look like
15:13
it does without it. Yeah, absolutely. And
15:15
so is there a repeatable pattern within
15:17
the web itself? Like, can we see
15:19
that or is it just random? We
15:22
don't think it repeats, no. So
15:24
there are recurring like similar structures,
15:27
like filaments, walls, voids, that Robert
15:29
was talking about before, they show
15:31
up everywhere and in every direction
15:33
we look, but we don't
15:35
see like the same patterns of those
15:37
structures repeating. No, it's not like some
15:39
sort of weird fractal or anything like
15:41
that. So when we go out to
15:43
large enough scales beyond around 300 million
15:45
light years across, the universe starts to
15:47
look what we call homogeneous. So it
15:49
looks the same in all directions on
15:51
a large scale. But like, if
15:53
you zoom into those smaller scales, it's still very
15:56
different in terms of like a
15:58
pattern. Yeah, okay. covered
28:00
and I think we can all agree that the
28:02
answer to that part is yes. So the second
28:04
half of David's question is, if that
28:06
is the case, is it possible
28:09
to calculate how long the process will
28:11
take, very best wishes to you all
28:13
and keep up the excellent podcast. Hi
28:16
David, first of all, great, great question.
28:18
Now, as we know, and as Kiara
28:20
said, yes, okay, this is going to
28:22
happen. The cosmic web will gradually thin
28:24
out and disappear due to the expansion
28:26
of the universe. Now we know the
28:29
rate of expansion of the universe. We
28:31
know the rate is accelerating at, but
28:33
extrapolating forward is a little bit difficult
28:35
because, you know, there are different models
28:37
for what the expansion is going to
28:39
do. So that does affect things slightly.
28:41
However, the timescales involved
28:44
are really, really quite long.
28:46
So I think in the grand scheme of
28:48
things, I can give you like an earmark
28:50
figure for what would happen. We
28:52
think in around about a hundred billion
28:54
years because of the accelerated expansion and bear in
28:57
mind, you know, the universe currently has 13.7 billion
28:59
years. This is far in the future in terms of its
29:01
sort of history. That any
29:03
galaxy that's not bound to our local group,
29:05
so in the way and Andromeda, they'll
29:08
have moved so far away that we actually
29:10
won't be able to see them beyond the
29:12
observable universe. So the structure will still
29:14
exist, but it'll be so thin that we won't even be
29:16
able to see it. It's only
29:18
in a trillion years time
29:20
that structures like within clusters and
29:22
the web itself will actually begin
29:25
to be affected, right? So it
29:27
will be stretched out.
29:30
And then over trillions to tens of
29:33
trillions, hundreds of trillions of years, we
29:35
think is when eventually that gravitationally bound
29:37
sort of nature of clusters will
29:40
actually be overtaken by the universe's expansion.
29:42
And I think that just puts it
29:44
into perspective, like, okay, yes, the universe
29:46
is expanding at an incredible rate, but
29:49
you know, gravity does its job pretty well in
29:51
holding things together. And thanks to, you know, dark
29:54
matter, as we talked about before, you know,
29:56
and this is why, you know, when people ask why
29:59
isn't the space between stars. expanding in the
30:01
Milky Way, it's because well gravity is stronger
30:03
on those smaller scales to hold everything together.
30:05
So like, you know, the space between stars
30:07
isn't getting bigger in the Milky Way because
30:10
everything's bound by gravity. And so
30:12
over a much larger scale is when
30:15
the acceleration of the universe starts to
30:17
take hold, but still gravity locally is
30:19
the strongest thing until trillions to tens
30:21
of trillions of years time, when eventually
30:23
that is overcome, at least, we
30:26
think, based on our current models of what's happening
30:28
in terms of the expansion rate of the universe.
30:31
Okay, thanks Becky. I hope that answers
30:33
your question, David. And Robert
30:35
Adrian111 asks, can
30:38
Euclid help with mapping the cosmic
30:40
web? Will it make a dark
30:42
matter and dark energy map? So
30:44
Euclid is this telescope that we've
30:46
all been talking about recently. I'm
30:48
so excited. Yeah, it's great. So
30:50
stay released next year. So excited.
30:52
Okay, good stuff. But back to
30:54
Adrian's question. Yeah, it's good stuff.
30:56
Adrian111, it's a good question to
30:58
ask. The answer is yes, because Euclid is designed
31:00
to map galaxies out 10 billion light
31:02
years away across a third of the sky. So looking back
31:04
a long way into the past in the universe as well.
31:06
So it'll definitely help us make a map of the web
31:09
because the whole objective is to make a 3D map of
31:11
a chunk of the universe. So not the whole universe that
31:13
we can see by any means, but quite a big bit
31:15
of it. And when you look
31:17
at things like phenomena like gravitational lensing and
31:19
the bending of light by gravity, that's a
31:21
way of mapping dark matter and understanding exactly
31:24
where it is because you see this lensing.
31:26
And you know, if you don't associate it
31:28
with visible matter or even implied visible matter,
31:30
normal matter as it's called, then you know
31:32
there's dark matter there. Now, dark
31:34
energy is sort of more pervasive and
31:36
uniform and we have really,
31:39
it's fair to say, not a good idea of what
31:41
it is still, even compared with dark matter where they
31:43
release more candidates. So mapping it is a bit
31:46
of a challenge. But by
31:48
getting the spectra of the galaxy, so looking when
31:50
I talk about a spectrum, you think about a
31:52
rainbow, think about the light being dispersed across colors
31:54
and then think about that happening in radio and
31:56
x-ray as well. But for this, in
31:58
this case optical. And infrared. And
32:01
infrared. So I'm sorry, infrared. We can
32:03
use that to make... Don't get infrared, please. Yeah,
32:05
no, no, I do need to be corrected. Mostly
32:07
infrared, the infrared. But we can work out how
32:09
fast galaxies are moving through redshift, basically by seeing
32:11
how the lines in the spectrum are shifted, and
32:14
then understand the expansion of the universe, and
32:16
then we can deduce how much of an
32:18
effect dark energy is having. We have a
32:20
good idea overall, but just verifying that, thinking
32:22
about all that stuff. So Euclid is making
32:24
a big contribution to that too. So the
32:26
answer to your question is, yeah, we'll get
32:28
better maps as a result, including dark matter.
32:30
Yeah, the dark energy one's so exciting as
32:32
well. The idea that we can trace the
32:34
expansion rate of the universe by looking back
32:36
in further weather distances is just
32:39
so cool. I'm so excited for it. And someday we'll
32:41
know what it is, right? Well, fingers crossed, you know?
32:43
Come on, guys, I'm out of this. Come on, Becky, you
32:46
need to change field. You need
32:48
a Nobel Prize, surely. No
32:50
pressure. Yeah, no pressure. Okay,
32:52
and Becky, there's not a name on
32:54
this one. But they've asked, how sure
32:57
are we about the structure of the
32:59
cosmic web? How precise can we be,
33:01
especially in far areas? Yeah, that's
33:03
a pretty good question. So I mean, we're
33:06
pretty sure about the structure because many surveys
33:08
have looked at this and all seen the
33:10
same thing. And obviously with newer telescopes, new
33:12
observatories, we're pushing to higher redshifts or greater
33:14
distances away from us all the time, like
33:16
with Euclid, as we just talked about. But
33:19
as we do that, obviously we're only seeing
33:21
the brightest of galaxies. We're not seeing the
33:23
faintest of galaxies when we go to those
33:25
huge distances. Even with something
33:27
like James Webb, right? You're still
33:29
not going to see the faintest of
33:31
things, even though it's got this incredible
33:33
sensitivity and light-collecting power. We know there's
33:36
some that we're still missing. However,
33:38
the brightest galaxies still do trace that
33:40
overall structure, right? And as I said
33:43
before, 300 million light
33:45
years is when things start to look homogeneous
33:47
and the same in all directions and have
33:49
that overarching structure of the filaments and the
33:51
clusters and the voids and the knots. So
33:54
we know that it's sort of the same everywhere
33:56
else we look. Now, to put context on that
33:58
number of 300 million.
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