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We know the universe had a beginning. | 0:00:06 | 0:00:09 | |
A moment 13.8 billion years ago when it sprang into life... | 0:00:11 | 0:00:16 | |
..creating the vast cosmos we see today. | 0:00:19 | 0:00:22 | |
Now we've discovered its origin, | 0:00:23 | 0:00:25 | |
we're faced with another equally fundamental question. | 0:00:25 | 0:00:28 | |
If the universe has a beginning, if it was born, | 0:00:29 | 0:00:32 | |
does that then mean it'll eventually die? | 0:00:32 | 0:00:35 | |
Or will it just keep on going for ever, eternal? | 0:00:35 | 0:00:38 | |
You see, for us, as all-too-mortal humans, the ultimate fate | 0:00:38 | 0:00:42 | |
of the universe is a question that's hard-wired into our psyche. | 0:00:42 | 0:00:46 | |
Trying to answer it has driven an astonishing | 0:00:46 | 0:00:49 | |
revolution in our understanding of the cosmos. | 0:00:49 | 0:00:52 | |
Yet in recent years, it's also revealed a universe | 0:00:53 | 0:00:57 | |
that's far stranger than we ever imagined. | 0:00:57 | 0:01:00 | |
And led to one of the most shocking moments in scientific history. | 0:01:02 | 0:01:06 | |
It's the latest twist in a tale stretching back over 100 years. | 0:01:09 | 0:01:14 | |
In that time, key experiments and crucial discoveries... | 0:01:17 | 0:01:21 | |
And there it is. | 0:01:21 | 0:01:23 | |
Exactly, exactly where Hoyle predicted. | 0:01:23 | 0:01:26 | |
..have brought us closer than anyone thought possible | 0:01:26 | 0:01:29 | |
to finally knowing the ultimate fate of the universe. | 0:01:29 | 0:01:33 | |
The sheer scale of the universe is truly staggering. | 0:01:46 | 0:01:50 | |
How on earth can you predict the future of something so vast... | 0:01:54 | 0:01:58 | |
..so complex... | 0:02:01 | 0:02:02 | |
..so much bigger than we are? | 0:02:05 | 0:02:07 | |
Since we first started grappling with this question, | 0:02:11 | 0:02:14 | |
the answer has hinged on one simple idea. | 0:02:14 | 0:02:17 | |
If we could chart, observe and understand how the universe has changed, | 0:02:20 | 0:02:25 | |
how it has evolved to the present moment from its very | 0:02:25 | 0:02:28 | |
ancient beginnings, then we should be able to extrapolate forward | 0:02:28 | 0:02:32 | |
and predict how it will evolve in the future. | 0:02:32 | 0:02:35 | |
Unfortunately, the slight flaw in that plan is that | 0:02:35 | 0:02:39 | |
the universe operates on timescales of millions and billions of years. | 0:02:39 | 0:02:44 | |
We don't. | 0:02:44 | 0:02:45 | |
To understand the workings of the universe, | 0:02:48 | 0:02:51 | |
we need to see beyond our limited human lifespan. | 0:02:51 | 0:02:54 | |
And in this case, it turned out the sheer scale | 0:02:58 | 0:03:01 | |
of the universe could be turned to our advantage. | 0:03:01 | 0:03:04 | |
The universe is so vast, | 0:03:24 | 0:03:26 | |
light from some of the objects we see in the night sky | 0:03:26 | 0:03:30 | |
has taken millions, even billions of years to reach the Earth. | 0:03:30 | 0:03:34 | |
When we look up, we're looking back in time at a record | 0:03:38 | 0:03:42 | |
of the deep history of the universe. | 0:03:42 | 0:03:44 | |
The problem is, we only have a snapshot, a single complex | 0:03:48 | 0:03:53 | |
and confusing picture of all this history. | 0:03:53 | 0:03:55 | |
It's like taking all the words in a novel, jumbling them up | 0:03:55 | 0:03:58 | |
and sticking them on a single page. | 0:03:58 | 0:04:01 | |
The key is to try and unpick this story, to learn how to read it, | 0:04:01 | 0:04:05 | |
to recognise and understand what's going on. | 0:04:05 | 0:04:07 | |
Astronomers realised that stars could help unlock that history. | 0:04:09 | 0:04:14 | |
If scientists could work out how stars change, | 0:04:17 | 0:04:20 | |
how they evolve in time, | 0:04:20 | 0:04:22 | |
they could begin to understand the bigger story of how the universe | 0:04:22 | 0:04:25 | |
was changing, the first clues to what the future might hold. | 0:04:25 | 0:04:29 | |
But it would take until the middle of the 20th century | 0:04:32 | 0:04:36 | |
to find the answer. | 0:04:36 | 0:04:37 | |
Unlocking the secrets of the stars would take | 0:04:39 | 0:04:42 | |
a moment of brilliance from this man, Fred Hoyle. | 0:04:42 | 0:04:46 | |
Hoyle was a brilliant mathematician and physicist, | 0:04:48 | 0:04:51 | |
one of the greatest of his day. | 0:04:51 | 0:04:53 | |
He was creative, coming up with bold theories. | 0:04:53 | 0:04:56 | |
Above all, he loved a problem, | 0:04:56 | 0:04:58 | |
some thorny issue he could make his mark by solving. | 0:04:58 | 0:05:01 | |
And in the late 1940s, he found one of the biggest. | 0:05:01 | 0:05:05 | |
Hoyle wanted to know where the elements came from. | 0:05:09 | 0:05:12 | |
The early universe was mostly just a sea of hydrogen and helium. | 0:05:15 | 0:05:20 | |
The simplest and lightest elements. | 0:05:20 | 0:05:22 | |
But we know that changed. | 0:05:25 | 0:05:28 | |
Look around us now. This is no simple world we live in. | 0:05:34 | 0:05:38 | |
We're surrounded by complexity, built from complex, heavy elements, | 0:05:38 | 0:05:44 | |
like the oxygen I breathe and the iron in our blood. | 0:05:44 | 0:05:47 | |
And of course, carbon, in the trees and in every cell in my body. | 0:05:47 | 0:05:51 | |
No-one knew how to bridge the gap, how the universe | 0:05:52 | 0:05:55 | |
went from that very simple beginning to all of this. | 0:05:55 | 0:05:59 | |
This was the problem Hoyle seized on. | 0:05:59 | 0:06:01 | |
Hoyle knew nuclear fusion must hold the answer. | 0:06:06 | 0:06:10 | |
In nuclear fusion, | 0:06:10 | 0:06:12 | |
lighter elements are fused together to make more complex ones. | 0:06:12 | 0:06:16 | |
It was already known to happen in the heart of stars, | 0:06:22 | 0:06:25 | |
where hydrogen fused together to form the more complex helium. | 0:06:25 | 0:06:29 | |
Hoyle wondered how to go further, how the helium nuclei | 0:06:32 | 0:06:36 | |
might fuse to make heavier elements. | 0:06:36 | 0:06:39 | |
It's a remarkably simple idea. Here's our helium nucleus. | 0:06:42 | 0:06:45 | |
If you could stick together two helium nuclei, | 0:06:47 | 0:06:50 | |
you'd make beryllium, a heavier, more complex nucleus. | 0:06:50 | 0:06:53 | |
Then, add a third helium nucleus and you get carbon. | 0:06:53 | 0:06:58 | |
From there, you can carry on building up heavier and heavier elements. | 0:06:58 | 0:07:02 | |
It sounds like the perfect solution. | 0:07:02 | 0:07:04 | |
But there was a very good reason why the formation of carbon - | 0:07:04 | 0:07:08 | |
hence all other elements - was still such a big mystery. | 0:07:08 | 0:07:11 | |
The problem was, that the physics of this process just didn't work. | 0:07:12 | 0:07:16 | |
Calculations showed that three helium nuclei wouldn't stick together. | 0:07:18 | 0:07:22 | |
The carbon nucleus they formed was unstable and simply fell apart. | 0:07:22 | 0:07:27 | |
If it broke down at carbon, | 0:07:28 | 0:07:30 | |
then there was no chance of making any other heavier elements. | 0:07:30 | 0:07:33 | |
It was like hitting a roadblock, every time. | 0:07:33 | 0:07:36 | |
In typical bold and bullish fashion, | 0:07:42 | 0:07:45 | |
Hoyle got around the problem by predicting a brand-new state of carbon. | 0:07:45 | 0:07:49 | |
Hoyle took an intuitive leap. | 0:08:01 | 0:08:03 | |
He decided that if three helium nuclei did come together inside a star, | 0:08:03 | 0:08:08 | |
they could form carbon with a bit more energy than normal. | 0:08:08 | 0:08:11 | |
In this special state, it could stay intact for just long enough to become stable. | 0:08:11 | 0:08:17 | |
In that way, stars could make carbon and the roadblock was removed. | 0:08:17 | 0:08:21 | |
If he was right, then Hoyle had solved the mystery. | 0:08:24 | 0:08:29 | |
The elements were built in the heart of stars. | 0:08:29 | 0:08:31 | |
But there was more at stake than that. | 0:08:34 | 0:08:36 | |
Hoyle realised his theory could reveal how stars changed | 0:08:43 | 0:08:47 | |
through their lives. | 0:08:47 | 0:08:48 | |
And as the universe we see is built of stars, that would make it | 0:08:53 | 0:08:57 | |
a powerful tool for predicting the future of the universe. | 0:08:57 | 0:09:01 | |
Astronomers were already grouping stars based on their size, | 0:09:08 | 0:09:12 | |
colour and brightness... | 0:09:12 | 0:09:13 | |
..plotting them on a chart that was known as the Hertzsprung-Russell diagram. | 0:09:16 | 0:09:19 | |
So here we had the diagram that they created. | 0:09:25 | 0:09:27 | |
Along here is size and brightness, running from very large, | 0:09:27 | 0:09:32 | |
very bright stars, all the way down to smaller, dimmer stars. | 0:09:32 | 0:09:36 | |
And along this direction is colour and temperature. | 0:09:36 | 0:09:39 | |
Very hot blue stars, all the way down to cooler red stars. | 0:09:39 | 0:09:44 | |
Most regular-size stars fell into a long diagonal | 0:09:44 | 0:09:48 | |
through the middle of the diagram, | 0:09:48 | 0:09:51 | |
with a group of giant, bright stars above | 0:09:51 | 0:09:54 | |
and small, dwarf stars below. | 0:09:54 | 0:09:56 | |
Astronomers could see the patterns, but weren't able to unlock what they meant. | 0:09:57 | 0:10:03 | |
Until Hoyle and his theory presented | 0:10:05 | 0:10:08 | |
a radical new way of looking at the diagram. | 0:10:08 | 0:10:11 | |
One that would reveal the life cycle of a star. | 0:10:11 | 0:10:14 | |
Let's consider our own sun. | 0:10:16 | 0:10:18 | |
Now, at the moment, it's sitting here in the middle of the diagram, | 0:10:18 | 0:10:21 | |
happily burning hydrogen, turning it into helium. | 0:10:21 | 0:10:24 | |
But if Hoyle was right, when it's run out of its hydrogen, | 0:10:24 | 0:10:29 | |
it'll start fusing helium to make heavier elements. | 0:10:29 | 0:10:32 | |
Now, at this point, a dramatic transformation takes place. | 0:10:32 | 0:10:35 | |
Because rather than moving down the diagram in this direction, | 0:10:35 | 0:10:38 | |
it expands to many times its size | 0:10:38 | 0:10:41 | |
and jumps across here to live amongst the red giants. | 0:10:41 | 0:10:46 | |
At this phase, it starts burning helium to make much heavier | 0:10:46 | 0:10:49 | |
elements until it finally begins to produce carbon. | 0:10:49 | 0:10:52 | |
Now, at that point, when it's run out of its nuclear fuel, | 0:10:54 | 0:10:57 | |
it undergoes its final transformation. | 0:10:57 | 0:10:59 | |
It sheds most of its outer layer and leaves behind a tiny white cinder, | 0:10:59 | 0:11:05 | |
living here amongst the white dwarfs. | 0:11:05 | 0:11:08 | |
All stars follow their own route around the diagram. | 0:11:10 | 0:11:14 | |
Hoyle's theory provided the understanding to track each star's evolution, | 0:11:14 | 0:11:19 | |
driven by the sudden ignition of a new phase of elemental formation. | 0:11:19 | 0:11:24 | |
Here was the answer to the mystery of the heavy elements. | 0:11:28 | 0:11:33 | |
The key to the life cycle of the stars. | 0:11:33 | 0:11:36 | |
And a window onto the future of the universe. | 0:11:36 | 0:11:40 | |
All thanks to Hoyle's new state of carbon. | 0:11:40 | 0:11:43 | |
There was just one slight problem. | 0:11:44 | 0:11:47 | |
No-one had ever seen or detected Hoyle's special form of carbon, | 0:11:47 | 0:11:51 | |
not in a telltale spectra from stars, not anywhere on earth, | 0:11:51 | 0:11:55 | |
not even in a laboratory experiment. | 0:11:55 | 0:11:57 | |
As far as anyone could tell, it didn't exist. | 0:11:57 | 0:12:00 | |
And without this special form of carbon, | 0:12:00 | 0:12:02 | |
the whole theory would come crashing down. | 0:12:02 | 0:12:05 | |
What happened next is a testament to Hoyle's brilliance | 0:12:07 | 0:12:11 | |
and almost pig-headed self belief. | 0:12:11 | 0:12:14 | |
In the 1950s, Hoyle joined the California Institute of Technology - | 0:12:23 | 0:12:27 | |
Caltech - who had one of the few particle accelerators | 0:12:27 | 0:12:31 | |
in existence at the time, similar to this one. | 0:12:31 | 0:12:34 | |
Hoyle wanted to use the accelerator to try | 0:12:35 | 0:12:38 | |
and make his high-energy carbon. | 0:12:38 | 0:12:41 | |
They were not so keen. | 0:12:41 | 0:12:42 | |
Here was an unknown Brit trying to take over their new machine | 0:12:46 | 0:12:50 | |
in order to look for something he'd effectively made up. | 0:12:50 | 0:12:53 | |
Like Hoyle, I'm a theorist. | 0:13:07 | 0:13:10 | |
Experimental physics is a very different world | 0:13:10 | 0:13:12 | |
and it's a different area of expertise. | 0:13:12 | 0:13:16 | |
But Hoyle had the confidence, the daring, to stride into the lab | 0:13:16 | 0:13:21 | |
and, as the director of the facility said, | 0:13:21 | 0:13:23 | |
without a buy-or-leave, demand that they give up the research | 0:13:23 | 0:13:28 | |
they were doing in favour of carrying out a complicated experiment | 0:13:28 | 0:13:31 | |
to look for something that no-one even believed existed in the first place. | 0:13:31 | 0:13:35 | |
I'm pretty sure I wouldn't have had the guts to do that. | 0:13:35 | 0:13:39 | |
Hoyle kept at them, arguing it would be a crucial and famous discovery. | 0:13:39 | 0:13:44 | |
Finally, they gave in. | 0:13:46 | 0:13:47 | |
The search was on. | 0:13:47 | 0:13:49 | |
Today, I'm recreating their experiment. | 0:13:51 | 0:13:53 | |
The plan was to bombard a target element with a particle beam | 0:13:55 | 0:14:00 | |
to see if they could create that state of carbon. | 0:14:00 | 0:14:02 | |
Well, I have with me my own experimental colleagues, | 0:14:02 | 0:14:05 | |
Zahne and Robin, to help me out. | 0:14:05 | 0:14:07 | |
Our target will be held in the centre of this reaction chamber. | 0:14:08 | 0:14:12 | |
Now, what they were looking for was a very specific signal | 0:14:14 | 0:14:17 | |
that would show up in their detectors. | 0:14:17 | 0:14:19 | |
If that state of carbon existed, then Hoyle predicted that it would | 0:14:19 | 0:14:23 | |
show up as a spike in the energy at 7.7 million electron volts - | 0:14:23 | 0:14:28 | |
the fingerprints of this special state of carbon. | 0:14:28 | 0:14:30 | |
We'll be looking for the same spike in energy. | 0:14:32 | 0:14:35 | |
Time to seal the chamber... | 0:14:36 | 0:14:38 | |
..close the radiation doors... | 0:14:40 | 0:14:42 | |
..and see for ourselves what happened. | 0:14:43 | 0:14:46 | |
Right, this is the control panel. | 0:14:48 | 0:14:50 | |
And they've let me in - a theorist - to get it all running. | 0:14:50 | 0:14:54 | |
So the first thing I do is fire up the beam. | 0:14:54 | 0:14:56 | |
Then to aim the beam at the target. | 0:14:59 | 0:15:01 | |
Charged particles are now slamming into the target. | 0:15:03 | 0:15:07 | |
Back in the 1950s, this was Hoyle's moment of truth. | 0:15:07 | 0:15:10 | |
Now data will start coming in and the important display | 0:15:12 | 0:15:16 | |
to look at is over here. | 0:15:16 | 0:15:17 | |
Now, if Hoyle was right, they'd see his excited state of carbon at this | 0:15:19 | 0:15:23 | |
energy here. They would expect to see a spike in energy at that point. | 0:15:23 | 0:15:28 | |
And there it is. | 0:15:30 | 0:15:32 | |
Exactly - exactly - where Hoyle predicted. | 0:15:33 | 0:15:36 | |
Now, when this experiment was carried out some 60 years ago, | 0:15:36 | 0:15:40 | |
they were flabbergasted to see that Hoyle was right. | 0:15:40 | 0:15:44 | |
It's quite incredible to think that he just worked on a theoretical hunch, | 0:15:44 | 0:15:48 | |
convinced his experimental colleagues to do the experiment, | 0:15:48 | 0:15:51 | |
and he was right. | 0:15:51 | 0:15:52 | |
He was also right about the fame. | 0:15:55 | 0:15:58 | |
The director of the laboratory went on to receive | 0:15:58 | 0:16:01 | |
the Nobel Prize for the discovery. | 0:16:01 | 0:16:03 | |
Hoyle, however, received nothing. | 0:16:04 | 0:16:07 | |
They published their findings in one of the most famous | 0:16:10 | 0:16:12 | |
and heavily referenced papers in science. | 0:16:12 | 0:16:16 | |
On the front cover of the paper, | 0:16:16 | 0:16:17 | |
the authors put a very apt quote from Shakespeare's King Lear. | 0:16:17 | 0:16:22 | |
"It is the stars, the stars above us, govern our conditions." | 0:16:22 | 0:16:25 | |
It was the confirmation of this excited state of carbon that | 0:16:27 | 0:16:30 | |
proved that it's inside stars that all the elements that make | 0:16:30 | 0:16:34 | |
up the world around us, including ourselves, are actually forged. | 0:16:34 | 0:16:38 | |
And with that discovery, we gained real insight into the life cycle of stars. | 0:16:38 | 0:16:43 | |
We could begin to understand how the universe changed over time, | 0:16:43 | 0:16:47 | |
both now and into the future. | 0:16:47 | 0:16:49 | |
Here was the foundation for extrapolating into the future. | 0:16:53 | 0:16:57 | |
And it made one clear prediction for the end of the universe. | 0:16:59 | 0:17:03 | |
It was hydrogen and helium that first formed stars, | 0:17:06 | 0:17:10 | |
and it was these two elements that were consumed in stars | 0:17:10 | 0:17:13 | |
as they aged, creating all the heavier elements in the process. | 0:17:13 | 0:17:17 | |
The logical conclusion was disturbing. | 0:17:17 | 0:17:20 | |
After an almost unimaginable length of time, | 0:17:20 | 0:17:22 | |
stars would use up all the hydrogen and helium in existence. | 0:17:22 | 0:17:27 | |
No new stars could form, | 0:17:27 | 0:17:29 | |
and existing stars would eventually run out of their fuel and die. | 0:17:29 | 0:17:33 | |
The universe would go dark. | 0:17:34 | 0:17:36 | |
For everything that's important to you and me, the light and life | 0:17:38 | 0:17:44 | |
created by the stars, the universe would eventually come to an end. | 0:17:44 | 0:17:50 | |
But there was another option. | 0:17:55 | 0:17:57 | |
One that promised a very different fate... | 0:17:57 | 0:17:59 | |
..and would play out long before the stars ran out of fuel. | 0:18:00 | 0:18:04 | |
A fate that involved a fundamental force of the universe. | 0:18:05 | 0:18:09 | |
Gravity. | 0:18:11 | 0:18:13 | |
The potential for gravity to define the ultimate fate | 0:18:16 | 0:18:20 | |
of the universe was first spotted by one of science's unsung heroes. | 0:18:20 | 0:18:25 | |
Vesto Slipher. | 0:18:25 | 0:18:27 | |
Little-known, his pioneering expert measurements | 0:18:27 | 0:18:30 | |
would transform our understanding of the universe. | 0:18:30 | 0:18:33 | |
In the early 1900s, astronomy was entering its golden age, | 0:18:35 | 0:18:40 | |
with evermore powerful telescopes trained on the skies. | 0:18:40 | 0:18:43 | |
One of the biggest targets of the time was the nebulae. | 0:18:45 | 0:18:48 | |
Nebulae were patches and swirls of light | 0:18:54 | 0:18:57 | |
that could be seen in between the stars, | 0:18:57 | 0:18:59 | |
and not much was known about these mysterious objects, | 0:18:59 | 0:19:03 | |
so astronomers were scrambling to find out as much about them as possible. | 0:19:03 | 0:19:07 | |
Slipher was interested in one particular aspect of the nebulae - | 0:19:07 | 0:19:11 | |
their motion. | 0:19:11 | 0:19:12 | |
And for his target, he chose the most famous one of all, Andromeda. | 0:19:12 | 0:19:17 | |
Slipher wanted to be the first to measure how quickly a nebula was moving. | 0:19:22 | 0:19:27 | |
The problem was, his was not the best telescope out there. | 0:19:29 | 0:19:33 | |
Not by a long chalk. | 0:19:33 | 0:19:34 | |
But Slipher did have one big advantage over his competitors. | 0:19:36 | 0:19:39 | |
He was a superb astronomer. | 0:19:42 | 0:19:44 | |
This telescope is actually the same size as Slipher's. | 0:19:47 | 0:19:51 | |
It has a 24-inch mirror. | 0:19:51 | 0:19:53 | |
But Slipher would have loved to have got his hands on something like this. | 0:19:54 | 0:19:58 | |
You see, what he needed was to get a spectrum. | 0:19:58 | 0:20:01 | |
Now, that involves splitting the light from the nebulae | 0:20:01 | 0:20:05 | |
into its different wavelengths, the different colours that it's made of. | 0:20:05 | 0:20:09 | |
Now, he'd have used something like this - it's a diffraction grating. | 0:20:09 | 0:20:12 | |
I can see it reflects this light and gives me | 0:20:12 | 0:20:16 | |
all the different colours of the rainbow. | 0:20:16 | 0:20:19 | |
What worried Slipher was that he needed to collect as much light as possible | 0:20:19 | 0:20:24 | |
to give him a usable spectrum, and nebulae are exceptionally faint. | 0:20:24 | 0:20:29 | |
He feared that getting enough light from his telescope would | 0:20:30 | 0:20:35 | |
prove to be impossible. | 0:20:35 | 0:20:36 | |
It may be the same size, | 0:20:40 | 0:20:43 | |
but this modern telescope can capture the spectrum | 0:20:43 | 0:20:46 | |
of Andromeda in a matter of minutes. | 0:20:46 | 0:20:48 | |
With his telescope, Slipher needed 14 hours to produce one spectrum. | 0:20:52 | 0:20:57 | |
Two days of backbreaking efforts. | 0:20:57 | 0:21:00 | |
Seven hours each night, | 0:21:02 | 0:21:04 | |
constantly adjusting the telescope to keep it fixed on Andromeda. | 0:21:04 | 0:21:07 | |
Slipher wanted to know how Andromeda was moving, | 0:21:11 | 0:21:15 | |
and for that he didn't just need the spectrum of light on Andromeda, | 0:21:15 | 0:21:18 | |
he needed to have the absorption lines. | 0:21:18 | 0:21:21 | |
Now, these are discreet gaps in the spectrum, like this. | 0:21:21 | 0:21:25 | |
Now, these absorption lines should always be in the same place | 0:21:25 | 0:21:29 | |
if the source isn't moving. | 0:21:29 | 0:21:31 | |
If they've shifted to the right, towards the red end of the spectrum, | 0:21:31 | 0:21:35 | |
that means that the source is moving away from us. | 0:21:35 | 0:21:38 | |
If they've shifted to the left, towards the blue end of the spectrum, | 0:21:38 | 0:21:42 | |
that means the source is moving towards us - a blue shift. | 0:21:42 | 0:21:46 | |
Now, after two days of observing, Slipher was ready to develop his photograph. | 0:21:46 | 0:21:52 | |
And he didn't get something as beautiful and clean as this. | 0:21:52 | 0:21:56 | |
He got this image. | 0:21:58 | 0:21:59 | |
Now this is in fact blown up. | 0:21:59 | 0:22:01 | |
In fact, what he got was a much smaller image than this. | 0:22:01 | 0:22:04 | |
And it's not even these lines, at the top and bottom. | 0:22:04 | 0:22:07 | |
In fact, what he got was this dirty smudge in the middle. | 0:22:07 | 0:22:12 | |
That was the spectrum from Andromeda. | 0:22:12 | 0:22:14 | |
Now, you might think he'd failed, | 0:22:15 | 0:22:17 | |
that you couldn't get anything meaningful from this. | 0:22:17 | 0:22:20 | |
In fact, not only was he able to get a meaningful measurement, | 0:22:20 | 0:22:23 | |
he could work out that Andromeda showed a very clear blue shift, | 0:22:23 | 0:22:28 | |
that it was moving towards us. | 0:22:28 | 0:22:30 | |
In fact, he worked out it was moving towards us at a speed of 300km per second, | 0:22:30 | 0:22:36 | |
which actually matches modern-day estimates. | 0:22:36 | 0:22:39 | |
Slipher had done it. | 0:22:40 | 0:22:42 | |
The first ever measure of the speed of a nebula. | 0:22:42 | 0:22:45 | |
His skill and tenacity overcoming the limits of his telescope. | 0:22:45 | 0:22:49 | |
When Slipher presented his findings at an astronomy meeting in 1914, | 0:22:52 | 0:22:57 | |
he received a standing ovation. | 0:22:57 | 0:22:59 | |
It's often easy to forget how important people like Slipher are. | 0:22:59 | 0:23:03 | |
The major breakthroughs in science aren't always about | 0:23:04 | 0:23:07 | |
the big idea or the beautiful theory. | 0:23:07 | 0:23:10 | |
They're often simply reliant on people who are exceptionally | 0:23:10 | 0:23:14 | |
skilled at observing and measuring the natural world. | 0:23:14 | 0:23:18 | |
We now know that the Andromeda nebula is actually a galaxy | 0:23:22 | 0:23:26 | |
like our own, the Milky Way. | 0:23:26 | 0:23:28 | |
And it's Andromeda's movement that reveals how gravity can shape | 0:23:30 | 0:23:34 | |
the fate of the universe. | 0:23:34 | 0:23:36 | |
Since it was first born in the Big Bang, | 0:23:42 | 0:23:45 | |
the universe has been expanding outwards. | 0:23:45 | 0:23:48 | |
As a result, most galaxies are actually | 0:23:48 | 0:23:51 | |
heading away from each other. | 0:23:51 | 0:23:52 | |
When they first formed, the same would have been true | 0:23:54 | 0:23:56 | |
of Andromeda and the Milky Way. | 0:23:56 | 0:23:59 | |
Until gravity got to work and began to overwhelm that expansion. | 0:23:59 | 0:24:03 | |
It's gravity that's dragging Andromeda | 0:24:07 | 0:24:09 | |
and our own Milky Way galaxy inexorably together. | 0:24:09 | 0:24:13 | |
The question is, if it can pull off this trick in our own little corner of the cosmos, | 0:24:13 | 0:24:17 | |
can it do the same over the entire expanse of the universe? | 0:24:17 | 0:24:22 | |
If gravity could overwhelm the expansion, | 0:24:36 | 0:24:39 | |
then long before the stars are burnt out, | 0:24:39 | 0:24:42 | |
our vast universe would inevitably, inescapably collapse in on itself. | 0:24:42 | 0:24:48 | |
The universe would end with a big crunch. | 0:24:50 | 0:24:53 | |
If gravity failed, the universe would simply continue to expand, | 0:24:57 | 0:25:01 | |
far beyond even the time when the last star had died. | 0:25:01 | 0:25:05 | |
Everything hinged on one factor, | 0:25:12 | 0:25:15 | |
predicted by Einstein's general theory of relativity. | 0:25:15 | 0:25:19 | |
Using general relativity | 0:25:23 | 0:25:25 | |
revealed that there were two very different futures to the universe. | 0:25:25 | 0:25:29 | |
What's more, they were able to calculate a specific figure | 0:25:29 | 0:25:33 | |
that marked the boundary between these two different scenarios. | 0:25:33 | 0:25:36 | |
It became known as the critical density. | 0:25:36 | 0:25:39 | |
The critical density was effectively a threshold | 0:25:44 | 0:25:48 | |
based on how much matter and energy - how much stuff - | 0:25:48 | 0:25:52 | |
there was in the entire universe. | 0:25:52 | 0:25:55 | |
If that total was above the critical density, | 0:25:58 | 0:26:01 | |
then gravity would drag the entire universe back together | 0:26:01 | 0:26:05 | |
into the Big Crunch. | 0:26:05 | 0:26:06 | |
If the total was below the critical density, | 0:26:10 | 0:26:13 | |
then the expansion of the universe will continue for ever. | 0:26:13 | 0:26:17 | |
The fate of the entire universe came down to a simple question - | 0:26:20 | 0:26:24 | |
what universe do we live in? | 0:26:24 | 0:26:26 | |
One that is above the critical density, or one that is below? | 0:26:26 | 0:26:30 | |
One way to tell was to look at the expansion of the universe. | 0:26:35 | 0:26:39 | |
If the universe was above the critical density and heading for | 0:26:40 | 0:26:44 | |
collapse, then the rate of expansion would already be slowing down. | 0:26:44 | 0:26:49 | |
So, astronomers began working on a way to measure | 0:26:50 | 0:26:53 | |
how the expansion of the universe was changing. | 0:26:53 | 0:26:56 | |
They were confident until a precocious PhD student | 0:26:59 | 0:27:03 | |
called Beatrice Tinsley spotted a fatal flaw in the plan. | 0:27:03 | 0:27:08 | |
Tinsley, know as "little beetle" to her family and friends, | 0:27:11 | 0:27:14 | |
was an extremely talented musician. | 0:27:14 | 0:27:17 | |
She could have turned professional. | 0:27:17 | 0:27:19 | |
But instead she decided to focus on her other great passion, | 0:27:19 | 0:27:22 | |
which was astrophysics. | 0:27:22 | 0:27:24 | |
Here, too, she excelled. | 0:27:24 | 0:27:26 | |
But an academic career in the 1960s, if you are woman, wasn't easy, | 0:27:26 | 0:27:30 | |
and her institution, the University of Texas, | 0:27:30 | 0:27:33 | |
seemed determined to ignore this brilliant scientist in their midst. | 0:27:33 | 0:27:37 | |
Despite that, she completed her PhD | 0:27:37 | 0:27:40 | |
in less than half the time it would normally take. | 0:27:40 | 0:27:43 | |
And that PhD spelled trouble for the expansion rate measurements. | 0:27:44 | 0:27:48 | |
The plan was to measure how galaxies were moving | 0:27:51 | 0:27:54 | |
at different distances from Earth | 0:27:54 | 0:27:56 | |
and therefore at different times in the past. | 0:27:56 | 0:28:00 | |
How their movement changed | 0:28:02 | 0:28:04 | |
would reveal how the expansion of the universe was changing. | 0:28:04 | 0:28:08 | |
Measuring the movement was relatively straightforward. | 0:28:09 | 0:28:13 | |
It was measuring the distance where the problem lay. | 0:28:13 | 0:28:16 | |
In our everyday world, we're surrounded by visual clues | 0:28:18 | 0:28:21 | |
that give us a good sense of scale, and therefore of distance. | 0:28:21 | 0:28:25 | |
But in the vastness of the universe, this is much more difficult, | 0:28:25 | 0:28:28 | |
so astronomers turned to something that might seem unusual. | 0:28:28 | 0:28:32 | |
Light itself. | 0:28:32 | 0:28:33 | |
Light is not perhaps an obvious tape measure, | 0:28:37 | 0:28:40 | |
but in this case it seemed ideal. | 0:28:40 | 0:28:43 | |
Now, this relies on a very simple principle. | 0:28:43 | 0:28:45 | |
How bright the light appears to me is dependant on how close I am to it | 0:28:45 | 0:28:50 | |
so when I'm very close, a lot of light enters my eyes | 0:28:50 | 0:28:53 | |
and it seems bright. | 0:28:53 | 0:28:55 | |
But as I move away, the light has had more chance to spread out | 0:28:55 | 0:28:59 | |
and less of it enters my eyes, so it appears dimmer. | 0:28:59 | 0:29:02 | |
Crucially, this change in the level of brightness | 0:29:02 | 0:29:06 | |
follows a very precise mathematical relationship. | 0:29:06 | 0:29:09 | |
And I can use this relationship to calculate distance. | 0:29:12 | 0:29:16 | |
'If I measure the difference in brightness | 0:29:18 | 0:29:21 | |
'between a light next to me...' | 0:29:21 | 0:29:23 | |
220. | 0:29:23 | 0:29:24 | |
'..and one further away...' | 0:29:25 | 0:29:27 | |
About 1.5. | 0:29:27 | 0:29:29 | |
I don't know if you can see that. It's quite dark. | 0:29:29 | 0:29:32 | |
'..I can work out how far away the light is.' | 0:29:32 | 0:29:35 | |
And so now I have to divide these two numbers. | 0:29:37 | 0:29:41 | |
Well, it's roughly 150. | 0:29:41 | 0:29:45 | |
Now I have to take the square root. | 0:29:46 | 0:29:48 | |
The square root of 150... | 0:29:48 | 0:29:51 | |
Well, it's about 12. | 0:29:51 | 0:29:53 | |
It's just over 12. | 0:29:53 | 0:29:55 | |
About 12.2 metres. | 0:29:55 | 0:29:58 | |
Right. | 0:29:59 | 0:30:01 | |
Now to check my working. | 0:30:02 | 0:30:04 | |
It's this principle that astronomers were using | 0:30:07 | 0:30:09 | |
to measure the distance to galaxies. | 0:30:09 | 0:30:12 | |
So, what I have here... | 0:30:15 | 0:30:18 | |
is 11.5 metres. | 0:30:18 | 0:30:20 | |
It's a bit less than the 12 metres I calculated, but close enough. | 0:30:20 | 0:30:24 | |
I'm pretty happy with that. | 0:30:24 | 0:30:26 | |
But this technique only works | 0:30:28 | 0:30:30 | |
if you know how bright the distance object should be, | 0:30:30 | 0:30:34 | |
so you can measure how much that brightness has changed. | 0:30:34 | 0:30:38 | |
And that would turn out to be the astronomers' Achilles heel. | 0:30:38 | 0:30:42 | |
They were measuring galaxies at different distances, | 0:30:44 | 0:30:47 | |
so at different times during the life of the universe. | 0:30:47 | 0:30:50 | |
This meant that the galaxies differed in age by millions | 0:30:50 | 0:30:54 | |
or billions of years. | 0:30:54 | 0:30:55 | |
You see, for the distance measurements to work, | 0:30:55 | 0:30:58 | |
they had to assume that all these galaxies of different ages | 0:30:58 | 0:31:01 | |
were shining with the same brightness. | 0:31:01 | 0:31:04 | |
In other words, | 0:31:04 | 0:31:05 | |
a galaxy's brightness doesn't change over time. | 0:31:05 | 0:31:08 | |
But for Beatrice Tinsley, | 0:31:08 | 0:31:10 | |
there was a fatal flaw at the heart of this assumption. | 0:31:10 | 0:31:13 | |
Tinsley was fascinated by the life cycle of the stars - | 0:31:16 | 0:31:20 | |
how they changed through their lives. | 0:31:20 | 0:31:23 | |
Her PhD looked at what effect that would have | 0:31:24 | 0:31:28 | |
on the brightness of galaxies. | 0:31:28 | 0:31:30 | |
For Tinsley, it was clear that if stars have a life cycle | 0:31:33 | 0:31:37 | |
during which their appearance and brightness change, | 0:31:37 | 0:31:40 | |
then because galaxies are fundamentally made of stars, | 0:31:40 | 0:31:44 | |
so too would their brightness change over time. | 0:31:44 | 0:31:48 | |
Tinsley's findings sent shockwaves through the field. | 0:31:50 | 0:31:54 | |
"A palpable sense of panic", as one astronomer of the time described it. | 0:31:54 | 0:31:59 | |
And they were immediately challenged. | 0:31:59 | 0:32:02 | |
You see, a huge amount of time, effort and money | 0:32:02 | 0:32:04 | |
had been invested in these expansion measurements | 0:32:04 | 0:32:07 | |
and yet here was this unknown young PhD student - a woman, no less - | 0:32:07 | 0:32:11 | |
who was questioning it all. | 0:32:11 | 0:32:13 | |
And yet there was no arguing the logic of Tinsley's work | 0:32:13 | 0:32:17 | |
and, after four years, it was eventually accepted. | 0:32:17 | 0:32:20 | |
With that, it was back to the drawing board. | 0:32:23 | 0:32:26 | |
A new way was needed to test how close the universe was | 0:32:29 | 0:32:32 | |
to the critical density | 0:32:32 | 0:32:34 | |
to see if it would collapse or continue to expand. | 0:32:34 | 0:32:37 | |
There was another option. | 0:32:44 | 0:32:46 | |
A more direct approach. | 0:32:46 | 0:32:48 | |
One obvious way to see how close the universe is | 0:32:52 | 0:32:55 | |
to the critical density | 0:32:55 | 0:32:57 | |
is just to count how much stuff there is out there. | 0:32:57 | 0:33:00 | |
It's a simple enough idea, but rather difficult to pull off. | 0:33:00 | 0:33:04 | |
After all, in something as almost unimaginably vast as the universe, | 0:33:04 | 0:33:08 | |
how do you count every galaxy, every star, | 0:33:08 | 0:33:11 | |
every speck of interstellar gas? | 0:33:11 | 0:33:14 | |
It's almost impossible. | 0:33:14 | 0:33:16 | |
So, instead, astronomers cut the universe down to size. | 0:33:18 | 0:33:22 | |
They took an average count of just one small part | 0:33:23 | 0:33:26 | |
and then multiplied it up from there. | 0:33:26 | 0:33:29 | |
They could do this thanks to one unique characteristic | 0:33:29 | 0:33:33 | |
of the universe. | 0:33:33 | 0:33:34 | |
As far as we can tell, the universe is, on the largest scales, | 0:33:36 | 0:33:39 | |
the same in whatever direction we look. | 0:33:39 | 0:33:42 | |
So an astronomer sitting on Earth looking out into space | 0:33:42 | 0:33:45 | |
will get pretty much the same view as an alien astronomer | 0:33:45 | 0:33:49 | |
on a planet thousands of light years away | 0:33:49 | 0:33:51 | |
looking out in a completely different direction. | 0:33:51 | 0:33:54 | |
And that's why measuring how much stuff there is | 0:33:54 | 0:33:57 | |
in one small part of the universe | 0:33:57 | 0:33:59 | |
gives us a pretty accurate measure of how much there is overall. | 0:33:59 | 0:34:03 | |
They took their averages and came up with a total amount of mass | 0:34:05 | 0:34:09 | |
and energy in the universe. | 0:34:09 | 0:34:11 | |
The results took everyone by surprise. | 0:34:12 | 0:34:15 | |
All of them suggested the universe was well below the critical density. | 0:34:15 | 0:34:20 | |
In fact, the best estimate suggested the universe had so little mass | 0:34:20 | 0:34:23 | |
that its density was only a tiny fraction of the critical value. | 0:34:23 | 0:34:28 | |
Obviously, if right, | 0:34:29 | 0:34:31 | |
there was no way that the universe was going to collapse. | 0:34:31 | 0:34:35 | |
But there was a problem with this first estimate | 0:34:51 | 0:34:54 | |
of how close the universe was to the critical density. | 0:34:54 | 0:34:58 | |
The results were so low, they just didn't make any sense. | 0:34:58 | 0:35:02 | |
A flat white coffee, please. | 0:35:04 | 0:35:06 | |
Ours is so clearly a universe of matter, mass and energy. | 0:35:08 | 0:35:12 | |
They dominate our world. | 0:35:12 | 0:35:14 | |
They ARE our world. | 0:35:14 | 0:35:16 | |
These findings painted a picture of a universe | 0:35:16 | 0:35:19 | |
so alien to our everyday experience that it is perhaps understandable | 0:35:19 | 0:35:23 | |
it was such a difficult concept to embrace. | 0:35:23 | 0:35:26 | |
What's more, the estimates seemed to be at odds with the universe itself. | 0:35:27 | 0:35:32 | |
The scale of the mismatch was revealed | 0:35:34 | 0:35:37 | |
when the universe was mapped on an unprecedented scale | 0:35:37 | 0:35:41 | |
by Margaret Geller at Harvard University. | 0:35:41 | 0:35:44 | |
What Geller and her team did was first take a slice of the universe | 0:35:51 | 0:35:55 | |
some 500 million light-years long, 300 million light-years wide, | 0:35:55 | 0:36:01 | |
but still a thin wedge of the visible universe. | 0:36:01 | 0:36:04 | |
They observed as many galaxies as they could | 0:36:04 | 0:36:07 | |
and plotted them against distance. | 0:36:07 | 0:36:09 | |
So, every one of these dots is an individual galaxy. | 0:36:09 | 0:36:13 | |
There's over a thousand of them. | 0:36:13 | 0:36:15 | |
What took everyone by surprise was this pattern that they saw - | 0:36:15 | 0:36:19 | |
these bubbles, or almost a honeycomb structure. | 0:36:19 | 0:36:22 | |
You see, everyone had assumed that the galaxies would be | 0:36:22 | 0:36:25 | |
scattered randomly throughout the universe. | 0:36:25 | 0:36:28 | |
Here, for the first time, was evidence that - far from random - | 0:36:28 | 0:36:32 | |
the universe actually had structure. | 0:36:32 | 0:36:35 | |
And at the heart of this newly-discovered structure | 0:36:36 | 0:36:40 | |
was the pull of gravity. | 0:36:40 | 0:36:42 | |
Since almost the beginning of the universe, | 0:36:44 | 0:36:47 | |
gravity has been drawing matter together. | 0:36:47 | 0:36:50 | |
First into clouds of gas, which then clumped together to form galaxies. | 0:36:51 | 0:36:56 | |
These galaxies come together to form clusters of galaxies | 0:36:59 | 0:37:03 | |
and the clusters into superclusters. | 0:37:03 | 0:37:05 | |
It looks like a work of art. | 0:37:08 | 0:37:10 | |
These superclusters of galaxies are all joined together | 0:37:18 | 0:37:22 | |
by filaments of dust and gas, | 0:37:22 | 0:37:26 | |
all acting under the same irresistible pull. | 0:37:26 | 0:37:30 | |
My universe has just collapsed. | 0:37:33 | 0:37:36 | |
Argh! | 0:37:36 | 0:37:38 | |
Here we clearly see gravity acting as an architect, | 0:37:41 | 0:37:45 | |
shaping and influencing the structure of the entire universe | 0:37:45 | 0:37:49 | |
on a truly cosmic scale. | 0:37:49 | 0:37:52 | |
No, I think I can do better. | 0:37:54 | 0:37:57 | |
'The problem was, the estimates of matter in the universe | 0:37:57 | 0:38:00 | |
'were so small...' | 0:38:00 | 0:38:02 | |
Open that up. | 0:38:02 | 0:38:03 | |
'..they put the universe so far below the critical density, | 0:38:03 | 0:38:07 | |
'that such grand structures simply could not form.' | 0:38:07 | 0:38:10 | |
I don't like that. | 0:38:10 | 0:38:12 | |
'According to the numbers, | 0:38:12 | 0:38:14 | |
'the universe as we know it couldn't exist.' | 0:38:14 | 0:38:17 | |
This is a rubbish universe. | 0:38:17 | 0:38:19 | |
There had to be something missing from the counts. | 0:38:28 | 0:38:32 | |
But what was it? | 0:38:32 | 0:38:33 | |
And what would it mean for the critical density | 0:38:33 | 0:38:37 | |
and the fate of the universe? | 0:38:37 | 0:38:39 | |
One of the most colourful and controversial scientists | 0:38:40 | 0:38:44 | |
of the 20th century found the first clue. | 0:38:44 | 0:38:47 | |
Fritz Zwicky. | 0:38:48 | 0:38:50 | |
Zwicky was an eccentric, abrasive and brilliant scientist, | 0:38:51 | 0:38:56 | |
known occasionally to refer to the rest of his profession | 0:38:56 | 0:38:59 | |
as "spherical bastards", which is basically anyone who's a bastard, | 0:38:59 | 0:39:03 | |
whichever way you look at him. | 0:39:03 | 0:39:05 | |
But even those who disliked him | 0:39:05 | 0:39:07 | |
had to admit that he was capable of brilliant work. | 0:39:07 | 0:39:10 | |
Zwicky was also looking at galaxy clusters | 0:39:14 | 0:39:18 | |
and they would lead him to discover something extraordinary. | 0:39:18 | 0:39:22 | |
This picture here is just such a galaxy cluster. | 0:39:25 | 0:39:29 | |
It's called Abell 1689. | 0:39:29 | 0:39:31 | |
Each one of these yellow dots is part of the cluster. | 0:39:31 | 0:39:35 | |
It's quite incredible to think that each one of them | 0:39:35 | 0:39:38 | |
is an entire galaxy in itself. | 0:39:38 | 0:39:40 | |
It sort of gives you an impression of the sheer scale of these things. | 0:39:40 | 0:39:44 | |
Zwicky was fascinated by what held the clusters together. | 0:39:45 | 0:39:49 | |
The answer, of course, has to be gravity. | 0:39:50 | 0:39:53 | |
Imagine these marbles are all each individual galaxies, | 0:39:53 | 0:39:56 | |
moving in chaotic orbits around the centre of the cluster, | 0:39:56 | 0:40:00 | |
but none of them moves fast enough to be able to break free | 0:40:00 | 0:40:04 | |
and escape from the cluster. | 0:40:04 | 0:40:06 | |
Because of that, Zwicky could use how fast they were travelling | 0:40:07 | 0:40:11 | |
to measure the strength of gravity holding them in place. | 0:40:11 | 0:40:15 | |
And the strength of gravity would tell him how much matter - | 0:40:15 | 0:40:19 | |
how much stuff - there was within the cluster. | 0:40:19 | 0:40:22 | |
That is where things got very strange, | 0:40:23 | 0:40:26 | |
because the galaxies were moving at tremendous speeds. | 0:40:26 | 0:40:30 | |
The strength of gravity needed to hold all these speeding galaxies | 0:40:32 | 0:40:36 | |
within the cluster required far more mass than he could see. | 0:40:36 | 0:40:40 | |
And it wasn't just a small difference. | 0:40:40 | 0:40:43 | |
In fact, he needed something like a hundred times more mass | 0:40:43 | 0:40:46 | |
than could be detected. | 0:40:46 | 0:40:48 | |
Zwicky called this mysterious mass Dunkle Materie. | 0:40:51 | 0:40:55 | |
Dark matter. | 0:40:55 | 0:40:57 | |
Here was a strong candidate for the missing mass of the universe. | 0:40:58 | 0:41:03 | |
But to know if it took the universe above or below the critical density, | 0:41:04 | 0:41:09 | |
they had to solve one major problem. | 0:41:09 | 0:41:12 | |
How to study something when there is no known way of detecting it. | 0:41:12 | 0:41:17 | |
The answer would come thanks to a discovery made here | 0:41:24 | 0:41:28 | |
at the Jodrell Bank Observatory. | 0:41:28 | 0:41:30 | |
This giant dish is the Bernard Lovell Radio Telescope | 0:41:30 | 0:41:34 | |
and, in 1973, it spotted something no-one had ever seen before. | 0:41:34 | 0:41:39 | |
At the time, it was carrying out a survey of some very distant, | 0:41:45 | 0:41:49 | |
very bright objects - | 0:41:49 | 0:41:51 | |
quasars. | 0:41:51 | 0:41:53 | |
Part way through the survey, they detected something very unusual. | 0:41:58 | 0:42:02 | |
I've come here today to take another look at what they saw, | 0:42:03 | 0:42:07 | |
this time using not just the telescopes here at Jodrell, | 0:42:07 | 0:42:10 | |
but radio telescopes across the country. | 0:42:10 | 0:42:13 | |
Right, here we are - the control room at Jodrell Bank. | 0:42:22 | 0:42:25 | |
A lovely view there of the Lovell Telescope. | 0:42:25 | 0:42:27 | |
Now, over here, on these screens, | 0:42:27 | 0:42:30 | |
we see live data coming in from various telescopes. | 0:42:30 | 0:42:33 | |
One of them, the Mark II, is a radio telescope at Jodrell Bank, | 0:42:33 | 0:42:37 | |
but the rest are scattered around the country, all linked together | 0:42:37 | 0:42:41 | |
through optical fibres feeding into the central computer here. | 0:42:41 | 0:42:45 | |
The point is, the longer you observe an object, the better-quality image | 0:42:46 | 0:42:50 | |
you get, and after 50 hours of observation, here's what they see. | 0:42:50 | 0:42:54 | |
This is the same image as was seen 40 years ago, | 0:42:54 | 0:42:58 | |
showing these two bright dots - | 0:42:58 | 0:43:01 | |
two quasars. | 0:43:01 | 0:43:03 | |
This wasn't the first time quasars had been seen | 0:43:03 | 0:43:06 | |
but certainly the first time they had been spotted so close together, | 0:43:06 | 0:43:10 | |
as though they were a pair. | 0:43:10 | 0:43:12 | |
A pair was something new. | 0:43:14 | 0:43:16 | |
They began to gather as much information about them as possible, | 0:43:17 | 0:43:20 | |
including measuring their spectra - | 0:43:20 | 0:43:23 | |
the unique fingerprint contained within their light. | 0:43:23 | 0:43:27 | |
Here are the spectra from the two quasars. | 0:43:30 | 0:43:33 | |
Now, even at first glance, I can tell they look quite similar. | 0:43:33 | 0:43:37 | |
In fact, they are much more than just quite similar. | 0:43:37 | 0:43:40 | |
When they first measured them, | 0:43:40 | 0:43:42 | |
they saw that they were both red-shifted - | 0:43:42 | 0:43:44 | |
so longer wavelengths - by exactly the same amount. | 0:43:44 | 0:43:47 | |
And have a look at these emission peaks. | 0:43:47 | 0:43:50 | |
They both fall at exactly the same wavelength. | 0:43:50 | 0:43:53 | |
In fact, the spectra was so similar | 0:43:53 | 0:43:56 | |
they thought they had made a mistake - | 0:43:56 | 0:43:58 | |
that they had looked at the same object twice. | 0:43:58 | 0:44:01 | |
But they hadn't. | 0:44:01 | 0:44:02 | |
And that left just one possibility. | 0:44:02 | 0:44:05 | |
What they thought were two separate quasars | 0:44:05 | 0:44:07 | |
were in fact just one single quasar | 0:44:07 | 0:44:10 | |
that had somehow been split into two images. | 0:44:10 | 0:44:13 | |
A case of astronomical double vision. | 0:44:13 | 0:44:16 | |
There was a theory that could explain this - | 0:44:19 | 0:44:22 | |
a strange effect predicted by Albert Einstein - | 0:44:22 | 0:44:26 | |
gravitational lensing. | 0:44:26 | 0:44:28 | |
If you look through this lens, | 0:44:33 | 0:44:35 | |
you see that everything behind it is warped into strange shapes. | 0:44:35 | 0:44:40 | |
This bizarre effect is because, | 0:44:40 | 0:44:43 | |
as light passes through different thicknesses of the glass, | 0:44:43 | 0:44:46 | |
it bends, giving rise to a warped image. | 0:44:46 | 0:44:50 | |
Now, Einstein said that matter - stuff - also warped space, | 0:44:50 | 0:44:55 | |
changing the very shape of the fabric of the universe, | 0:44:55 | 0:44:59 | |
and so, as light passes through regions of space | 0:44:59 | 0:45:03 | |
with high concentrations of matter, it will bend, | 0:45:03 | 0:45:06 | |
just like it does going through the glass of this lens, | 0:45:06 | 0:45:09 | |
and so giving rise to similar visual tricks. | 0:45:09 | 0:45:12 | |
How much the light is bent | 0:45:14 | 0:45:16 | |
is dependent on how much the space is being warped, | 0:45:16 | 0:45:20 | |
and that depends on how much mass there is. | 0:45:20 | 0:45:24 | |
Between the quasar and the telescopes, | 0:45:24 | 0:45:26 | |
there had to be a huge amount of mass, | 0:45:26 | 0:45:29 | |
bending the light so much that the image is split, | 0:45:29 | 0:45:33 | |
making the single quasar appear as two. | 0:45:33 | 0:45:36 | |
Here's our culprit, or at least part of it. | 0:45:38 | 0:45:41 | |
This smudge here is just one galaxy within a cluster of galaxies | 0:45:41 | 0:45:45 | |
that sit between us and the distant quasar. | 0:45:45 | 0:45:48 | |
So it's not just a little bit of mass, | 0:45:48 | 0:45:50 | |
but hundreds of galaxies, each with billions of stars. | 0:45:50 | 0:45:54 | |
Combined, they bend the light from the quasar, | 0:45:54 | 0:45:58 | |
giving us the double image. | 0:45:58 | 0:46:00 | |
And the double image was crucial to the study of dark matter. | 0:46:02 | 0:46:06 | |
Even with all the mass and matter contained in the galaxy cluster, | 0:46:09 | 0:46:13 | |
there wasn't enough to bend the light that much. | 0:46:13 | 0:46:17 | |
For that, you needed Zwicky's mysterious and invisible | 0:46:18 | 0:46:22 | |
dark matter. | 0:46:22 | 0:46:23 | |
And carefully analysing exactly how much the light was distorted | 0:46:23 | 0:46:28 | |
could reveal where that dark matter was. | 0:46:28 | 0:46:31 | |
This is what you get - a map. | 0:46:32 | 0:46:35 | |
In the centre is the normal matter of the galaxy cluster itself, | 0:46:35 | 0:46:39 | |
but, surrounding it, stretching out much further, coloured here in red, | 0:46:39 | 0:46:43 | |
is the dark matter. | 0:46:43 | 0:46:44 | |
Look how far out it spreads. | 0:46:44 | 0:46:46 | |
It completely dwarfs the normal matter of the galaxy cluster. | 0:46:46 | 0:46:50 | |
Zwicky's mysterious and invisible matter | 0:46:50 | 0:46:53 | |
revealed by a cosmic optical illusion. | 0:46:53 | 0:46:56 | |
It couldn't reveal what dark matter was, | 0:46:58 | 0:47:01 | |
but mapping like this, as Jodrell is still doing to this day, | 0:47:01 | 0:47:05 | |
did give an idea of how much there was out there, | 0:47:05 | 0:47:09 | |
and it seemed to far outweigh normal matter, | 0:47:09 | 0:47:13 | |
but was it enough to take the universe over the critical density? | 0:47:13 | 0:47:18 | |
Even though there appeared to be far more dark matter than normal matter, | 0:47:20 | 0:47:24 | |
that still seemed to leave the universe | 0:47:24 | 0:47:26 | |
way below the critical density - | 0:47:26 | 0:47:29 | |
but this was still far from the end of the story. | 0:47:29 | 0:47:31 | |
The discovery of dark matter | 0:47:31 | 0:47:33 | |
had taken the scientific community completely by surprise. | 0:47:33 | 0:47:37 | |
Trying to work out how close the universe was to the critical density | 0:47:37 | 0:47:42 | |
was just throwing up more mysteries than answers. | 0:47:42 | 0:47:45 | |
A shocking new discovery that initially promised | 0:47:50 | 0:47:53 | |
to finally reveal the fate of the universe | 0:47:53 | 0:47:56 | |
instead threw physics into crisis. | 0:47:56 | 0:47:59 | |
In the 1990s, these telescopes were part of an international project | 0:48:11 | 0:48:15 | |
looking to finally reveal the fate of the universe. | 0:48:15 | 0:48:19 | |
They were using a new technique to once again | 0:48:23 | 0:48:27 | |
look at how the expansion of the universe had changed over time. | 0:48:27 | 0:48:31 | |
I've come to use this telescope - the GTC - | 0:48:40 | 0:48:44 | |
to observe the object that was at the heart of those studies. | 0:48:44 | 0:48:48 | |
This huge telescope - you can see the vast mirror behind it - | 0:48:54 | 0:48:59 | |
is going to take a close look at a supernova, | 0:48:59 | 0:49:02 | |
the explosive death of a star. | 0:49:02 | 0:49:04 | |
The light reaching us from these distant epic events would be key | 0:49:04 | 0:49:09 | |
to unlocking how the universe expanded in the past | 0:49:09 | 0:49:12 | |
and, in turn, would reveal what would happen to it in the future. | 0:49:12 | 0:49:16 | |
To measure the expansion, | 0:49:21 | 0:49:23 | |
researchers were interested in a particular type of supernova. | 0:49:23 | 0:49:26 | |
Our target tonight is the same class of supernovae | 0:49:39 | 0:49:42 | |
that they were searching for - a type Ia. | 0:49:42 | 0:49:45 | |
Now, what made type Ia supernovae so useful | 0:49:45 | 0:49:49 | |
is that, when they went off, | 0:49:49 | 0:49:50 | |
they created an incredibly bright spike of light. | 0:49:50 | 0:49:54 | |
Briefly, the star would shine brighter than its entire galaxy. | 0:49:54 | 0:49:57 | |
Not only that, but they always gave off | 0:49:57 | 0:50:00 | |
almost exactly the same level of brightness. | 0:50:00 | 0:50:03 | |
This meant that not only could they see them | 0:50:03 | 0:50:05 | |
over vast distances and remote galaxies, | 0:50:05 | 0:50:08 | |
but they could also work out exactly how far away they were. | 0:50:08 | 0:50:12 | |
So, if they could find enough of them, | 0:50:12 | 0:50:14 | |
they could sample conditions in the universe | 0:50:14 | 0:50:16 | |
over a wide range of distances and times. | 0:50:16 | 0:50:20 | |
Tonight, astronomer David Alvarez has been homing in | 0:50:22 | 0:50:26 | |
on a recently discovered type Ia supernova. | 0:50:26 | 0:50:29 | |
Right, David, this is very exciting. Do you have the supernova? | 0:50:32 | 0:50:36 | |
This is the image of the supernova. | 0:50:36 | 0:50:39 | |
-That thing there? -That thing there. | 0:50:39 | 0:50:41 | |
-Can you zoom in at all on it? -Yeah, we can zoom in here. | 0:50:41 | 0:50:44 | |
You can see the bright dot. | 0:50:44 | 0:50:47 | |
And the rest of it is the galaxy? | 0:50:47 | 0:50:49 | |
The rest of the light you can see there | 0:50:49 | 0:50:51 | |
is the host galaxy of the supernova. | 0:50:51 | 0:50:54 | |
I mean, that's incredible. | 0:50:54 | 0:50:55 | |
Here's a galaxy with hundreds of billions of stars, | 0:50:55 | 0:50:58 | |
but this one exploding star - this one supernova - | 0:50:58 | 0:51:01 | |
is shining brighter than the whole of the rest the galaxy. | 0:51:01 | 0:51:05 | |
And you know how far away this supernova is? | 0:51:05 | 0:51:08 | |
You've measured the distance? | 0:51:08 | 0:51:10 | |
-Yeah, the supernova is about eight billion light years away. -Wow. | 0:51:10 | 0:51:14 | |
As well as the distance, | 0:51:17 | 0:51:18 | |
the spectrum of the supernova is also crucial. | 0:51:18 | 0:51:21 | |
The astronomers needed the spectrum of the light | 0:51:23 | 0:51:26 | |
because it gave them the redshift. | 0:51:26 | 0:51:28 | |
You see, as the light travels from the distant supernova to Earth, | 0:51:28 | 0:51:31 | |
the universe is expanding, | 0:51:31 | 0:51:34 | |
the space the light is travelling through is stretching, | 0:51:34 | 0:51:37 | |
and so the light itself is also stretching. | 0:51:37 | 0:51:40 | |
Its wavelength is getting longer. | 0:51:40 | 0:51:42 | |
If it leaves the supernova | 0:51:42 | 0:51:44 | |
at a particular wavelength, a particular colour, | 0:51:44 | 0:51:46 | |
when it arrives in our telescopes, it's at a longer wavelength - | 0:51:46 | 0:51:50 | |
it's shifted towards the red end of the spectrum, | 0:51:50 | 0:51:52 | |
hence a redshift. | 0:51:52 | 0:51:54 | |
So knowing the redshift of the light | 0:51:54 | 0:51:56 | |
tells us how much space has expanded in that time. | 0:51:56 | 0:52:00 | |
In a sense, it gives us a measure of how big the universe has become. | 0:52:00 | 0:52:05 | |
Because of this, measuring redshifts at greater distances - | 0:52:07 | 0:52:10 | |
in effect, further back in time - | 0:52:10 | 0:52:13 | |
could create a potted history | 0:52:13 | 0:52:15 | |
of how the expansion of the universe was changing. | 0:52:15 | 0:52:18 | |
Astronomers were convinced that gravity must have, | 0:52:21 | 0:52:25 | |
at the very least, been slowing down the expansion. | 0:52:25 | 0:52:28 | |
The question was - by how much? | 0:52:28 | 0:52:32 | |
By plotting distance | 0:52:32 | 0:52:35 | |
against the redshift's measure of expansion, | 0:52:35 | 0:52:37 | |
they could finally answer that question. | 0:52:37 | 0:52:40 | |
Now, if you imagine the universe has been expanding at the same rate - | 0:52:42 | 0:52:45 | |
the rate that it is now - for its entire history, | 0:52:45 | 0:52:48 | |
I'd get a very simple line. | 0:52:48 | 0:52:51 | |
But astronomers knew this couldn't be correct | 0:52:51 | 0:52:54 | |
because, of course, gravity is putting the brakes on the expansion, | 0:52:54 | 0:52:57 | |
so the expansion of the universe should be slowing down | 0:52:57 | 0:53:00 | |
and, if it's expanding more slowly now, | 0:53:00 | 0:53:03 | |
it should've been expanding more quickly in the past. | 0:53:03 | 0:53:06 | |
Space stretching more would mean a bigger redshift. | 0:53:06 | 0:53:10 | |
Now, what does this mean for our supernova? | 0:53:10 | 0:53:12 | |
Well, we know it was eight billion light years away. | 0:53:12 | 0:53:15 | |
So we know it wouldn't fall exactly on this line, | 0:53:16 | 0:53:19 | |
which corresponds to a redshift of about 0.49. | 0:53:19 | 0:53:23 | |
It should sit maybe somewhere over here. | 0:53:23 | 0:53:25 | |
Maybe at a redshift greater than 0.5. | 0:53:25 | 0:53:28 | |
That means this line should really be curving down like that. | 0:53:28 | 0:53:33 | |
But, of course, the exact shape of this line would tell them | 0:53:33 | 0:53:36 | |
how much gravity is slowing down the expansion of the universe | 0:53:36 | 0:53:40 | |
and that would tell them the fate of the universe. | 0:53:40 | 0:53:44 | |
OK, so, David, you have the spectrum ready now. | 0:53:44 | 0:53:47 | |
We have it. | 0:53:47 | 0:53:49 | |
Yes, bring it up. | 0:53:49 | 0:53:51 | |
And that gives you a measure of the redshift. | 0:53:51 | 0:53:53 | |
So what did you measure that to be here? | 0:53:53 | 0:53:55 | |
For this case, we measured 0.47. | 0:53:55 | 0:53:58 | |
0.47! Well, that puts it on this side of the line. | 0:53:58 | 0:54:01 | |
That means it's not a larger redshift, but a smaller redshift. | 0:54:01 | 0:54:05 | |
This is fascinating because it's exactly what they saw. | 0:54:07 | 0:54:10 | |
Not redshifts that were larger, but redshifts that were smaller. | 0:54:10 | 0:54:14 | |
And they saw this time and time again | 0:54:14 | 0:54:16 | |
and it could only have one explanation - | 0:54:16 | 0:54:18 | |
smaller redshifts meant that the universe must have been expanding | 0:54:18 | 0:54:22 | |
more slowly in the past than it is today. | 0:54:22 | 0:54:25 | |
In other words, rather than slowing down, | 0:54:25 | 0:54:28 | |
the rate of expansion of the universe is accelerating. | 0:54:28 | 0:54:31 | |
As more and more supernovae were plotted, | 0:54:34 | 0:54:37 | |
the picture became clearer. | 0:54:37 | 0:54:39 | |
For the first few billion years after the Big Bang, | 0:54:42 | 0:54:45 | |
it looked as if the expansion rates had been slowing as expected... | 0:54:45 | 0:54:49 | |
..but then that changed | 0:54:51 | 0:54:53 | |
and the expansion started to accelerate. | 0:54:53 | 0:54:57 | |
It's hard to stress how much of a shock this was. | 0:54:59 | 0:55:03 | |
Back then, everyone knew that the expansion of the universe | 0:55:03 | 0:55:06 | |
had to be slowing down. | 0:55:06 | 0:55:07 | |
Now, whether it would slow down enough to stop and then recollapse, | 0:55:07 | 0:55:11 | |
that wasn't clear, but it had to be slowing down. | 0:55:11 | 0:55:14 | |
After all, gravity had to be doing its job of putting the brakes on, | 0:55:14 | 0:55:18 | |
but it wasn't. | 0:55:18 | 0:55:19 | |
About six billion years ago, | 0:55:19 | 0:55:21 | |
the expansion started to speed up. | 0:55:21 | 0:55:24 | |
Clearly, there was some new and unexpected thing | 0:55:24 | 0:55:27 | |
going on in the universe - | 0:55:27 | 0:55:28 | |
something that science didn't have an answer for, | 0:55:28 | 0:55:30 | |
something that was pushing the expansion of the universe | 0:55:30 | 0:55:34 | |
at an accelerating rate. | 0:55:34 | 0:55:36 | |
It became known, for want of another term, as dark energy. | 0:55:36 | 0:55:40 | |
The best estimates suggest that dark energy | 0:55:44 | 0:55:47 | |
makes up 70% of the universe. | 0:55:47 | 0:55:50 | |
And that means the universe will not collapse and end in a big crunch. | 0:55:52 | 0:55:56 | |
Instead, dark energy, not gravity, | 0:55:56 | 0:56:00 | |
will define the ultimate fate of the universe. | 0:56:00 | 0:56:03 | |
Dark energy pushes the universe apart. | 0:56:06 | 0:56:09 | |
It won't carry on expanding steadily for ever. | 0:56:09 | 0:56:12 | |
Instead, dark energy forces the universe to fly apart | 0:56:12 | 0:56:16 | |
at an ever-increasing rate. | 0:56:16 | 0:56:18 | |
Galaxies will become so far apart | 0:56:18 | 0:56:20 | |
that light wouldn't be able to travel between them. | 0:56:20 | 0:56:23 | |
Each one will end up as an individual island of stars | 0:56:23 | 0:56:26 | |
alone in the cosmos. | 0:56:26 | 0:56:28 | |
It may even become so extreme | 0:56:28 | 0:56:30 | |
that galaxies themselves will be ripped apart, | 0:56:30 | 0:56:33 | |
leaving individual stars all alone in the black emptiness. | 0:56:33 | 0:56:37 | |
Then again, maybe not. | 0:56:40 | 0:56:43 | |
After all, the effect of dark energy | 0:56:44 | 0:56:47 | |
seemed to suddenly appear between six and seven billion years ago. | 0:56:47 | 0:56:51 | |
Who's to say how it'll behave in the future? | 0:56:51 | 0:56:54 | |
That may sound bizarre | 0:56:56 | 0:56:58 | |
but, with the discovery of dark energy, all bets are off. | 0:56:58 | 0:57:02 | |
It's hard to stress how little we know about dark energy. | 0:57:04 | 0:57:07 | |
It has a name, but that's about it. | 0:57:07 | 0:57:10 | |
We don't know what it's made of, | 0:57:10 | 0:57:11 | |
why it's driving the universe apart | 0:57:11 | 0:57:14 | |
and, crucially, how it'll behave in the future. | 0:57:14 | 0:57:17 | |
And that leaves a big hole in our understanding of the universe | 0:57:17 | 0:57:20 | |
and its ultimate fate. | 0:57:20 | 0:57:22 | |
Dark energy may simply be part of the universe, | 0:57:24 | 0:57:28 | |
built into the way it works... | 0:57:28 | 0:57:30 | |
..or it could point to a fundamental problem | 0:57:33 | 0:57:37 | |
with the most important and trusted scientific theories we have... | 0:57:37 | 0:57:41 | |
..ones that are at the very heart of our understanding | 0:57:43 | 0:57:46 | |
of how the world works. | 0:57:46 | 0:57:47 | |
How the universe will end started as astronomy's great challenge, | 0:57:52 | 0:57:56 | |
but the fate of the universe has become | 0:57:56 | 0:57:58 | |
much more than just an academic question. | 0:57:58 | 0:58:01 | |
Through the discovery of this strange, enigmatic energy - | 0:58:01 | 0:58:05 | |
if, indeed, that's what it is - one that defies current understanding, | 0:58:05 | 0:58:08 | |
it's spread to the heart of fundamental physics. | 0:58:08 | 0:58:12 | |
Finding the answer to how the universe will end | 0:58:12 | 0:58:15 | |
could have profound implications on how we understand our world. | 0:58:15 | 0:58:20 | |
If you want to find out more about the universe and the end of time, | 0:58:24 | 0:58:28 | |
go to the address below and follow the links to the Open University. | 0:58:28 | 0:58:32 |