Browse content similar to Frozen Solid. Check below for episodes and series from the same categories and more!
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Everything around us | 0:00:04 | 0:00:06 | |
exists somewhere on a vast scale, from cold to hot. | 0:00:06 | 0:00:12 | |
The tiniest insects, all of us, the Earth, the stars, | 0:00:13 | 0:00:18 | |
even the universe itself - everything has a temperature. | 0:00:18 | 0:00:22 | |
I'm Dr Helen Czerski. | 0:00:25 | 0:00:27 | |
In this series, I'm going to unlock temperature's deepest mysteries. | 0:00:27 | 0:00:31 | |
Across three programmes, | 0:00:35 | 0:00:37 | |
I'm going to explore the extremes of the temperature scale, | 0:00:37 | 0:00:41 | |
from some of the coldest temperatures | 0:00:41 | 0:00:44 | |
to the very hottest, | 0:00:44 | 0:00:46 | |
and everything in between. | 0:00:46 | 0:00:49 | |
I'm a physicist, so my treasure map is woven | 0:00:49 | 0:00:52 | |
from the fundamental physical laws of the universe, | 0:00:52 | 0:00:55 | |
and temperature is an essential part of that. | 0:00:55 | 0:00:58 | |
It's the hidden energy contained within matter, | 0:00:59 | 0:01:03 | |
and the way that energy endlessly shifts and flows | 0:01:03 | 0:01:08 | |
is the architect that has shaped our planet... | 0:01:08 | 0:01:11 | |
..and the universe. | 0:01:13 | 0:01:15 | |
It's not often that I get up at 5am to watch a pond, | 0:01:16 | 0:01:19 | |
but this one's worth watching. | 0:01:19 | 0:01:21 | |
In this first programme, | 0:01:25 | 0:01:27 | |
I'm going to venture to the bottom of the temperature scale. | 0:01:27 | 0:01:31 | |
I'll explore how cold has fashioned the world around us | 0:01:31 | 0:01:36 | |
and why frozen doesn't mean what you might think. | 0:01:36 | 0:01:39 | |
The salt looks like that here. | 0:01:39 | 0:01:40 | |
It would look like that if I took it into a sauna | 0:01:40 | 0:01:43 | |
because it's a frozen solid. | 0:01:43 | 0:01:45 | |
And I'll descend to the very limits of cold | 0:01:47 | 0:01:50 | |
where the everyday laws of physics break down | 0:01:50 | 0:01:53 | |
and a new world of scientific possibility begins. | 0:01:53 | 0:01:58 | |
Temperature is in every single story that nature has to tell, | 0:01:58 | 0:02:02 | |
and, in this series, I'll be exploring why, | 0:02:02 | 0:02:04 | |
what temperature means, how it works, | 0:02:04 | 0:02:06 | |
and just how deep its influence on our lives and our world really is. | 0:02:06 | 0:02:11 | |
This is Eldhraun, in the south of Iceland, | 0:02:45 | 0:02:47 | |
and it's a great place to start the story of temperature | 0:02:47 | 0:02:50 | |
because this weird landscape around me - | 0:02:50 | 0:02:52 | |
all these lumps and bumps - | 0:02:52 | 0:02:54 | |
this was sculpted by the interplay between hot and cold. | 0:02:54 | 0:02:58 | |
Just over 230 years ago, | 0:03:00 | 0:03:03 | |
a huge fissure in the ground opened up over there - 25km long - | 0:03:03 | 0:03:08 | |
and a huge amount of lava flooded out | 0:03:08 | 0:03:11 | |
in an event that lasted eight months. | 0:03:11 | 0:03:14 | |
It's thought that over 500 square kilometres | 0:03:15 | 0:03:18 | |
was covered in molten red rock. | 0:03:18 | 0:03:21 | |
When the lava came out of the ground, | 0:03:24 | 0:03:27 | |
it was at about 850 degrees Celsius, | 0:03:27 | 0:03:30 | |
but it met cool air, and heat flowed from hot to cold | 0:03:30 | 0:03:34 | |
because that's the way our universe works. | 0:03:34 | 0:03:36 | |
And, as the lava cooled, it froze, and this landscape is what you get | 0:03:36 | 0:03:41 | |
when the hot innards of the Earth meet cold | 0:03:41 | 0:03:45 | |
and are fixed in a form that will last for millennia. | 0:03:45 | 0:03:48 | |
But the mysterious ability of cold to create solid matter | 0:03:50 | 0:03:55 | |
is something we've only recently uncovered. | 0:03:55 | 0:03:58 | |
DOGS BARK | 0:03:58 | 0:04:01 | |
We've always been familiar with the experience of cold and heat, | 0:04:04 | 0:04:09 | |
but, until recently, we didn't understand what they actually were, | 0:04:09 | 0:04:13 | |
and, as the era of modern science dawned, | 0:04:13 | 0:04:16 | |
that lack of knowledge was becoming a barrier to progress. | 0:04:16 | 0:04:20 | |
I'm here at the Radcliffe Observatory in Oxford | 0:04:24 | 0:04:27 | |
and what it was built to observe is the cosmos. | 0:04:27 | 0:04:30 | |
Back in the 18th century, | 0:04:30 | 0:04:32 | |
this was one of the most foremost centres | 0:04:32 | 0:04:34 | |
of the new science of astronomy. | 0:04:34 | 0:04:36 | |
But, while looking up there, | 0:04:36 | 0:04:38 | |
they discovered they had a problem that started down here. | 0:04:38 | 0:04:42 | |
I'm meeting Amy Creese, who's a meteorological observer. | 0:04:48 | 0:04:53 | |
It's a role that was created here over 200 years ago | 0:04:53 | 0:04:57 | |
to solve a very specific problem caused by temperature. | 0:04:57 | 0:05:01 | |
Early observers made quite meticulous records | 0:05:02 | 0:05:05 | |
of the temperature | 0:05:05 | 0:05:06 | |
and that was because it was important to know | 0:05:06 | 0:05:09 | |
what the temperature was like in order to correct | 0:05:09 | 0:05:12 | |
for something called atmospheric refraction, | 0:05:12 | 0:05:14 | |
which is how much the light from a celestial object bends | 0:05:14 | 0:05:18 | |
as it comes into the Earth's atmosphere, | 0:05:18 | 0:05:20 | |
and that depends quite a lot on temperature. | 0:05:20 | 0:05:22 | |
So, in order to make very accurate measurements | 0:05:22 | 0:05:25 | |
of positions of stars, the observers found | 0:05:25 | 0:05:28 | |
that they needed to measure temperature, as well, | 0:05:28 | 0:05:30 | |
so they kept very good records of that. | 0:05:30 | 0:05:32 | |
So, even those people who were looking up at the cosmos | 0:05:32 | 0:05:35 | |
and thinking grand thoughts about the universe | 0:05:35 | 0:05:37 | |
needed to know about this quite mundane thing down here, | 0:05:37 | 0:05:39 | |
which was the temperature. | 0:05:39 | 0:05:41 | |
And you've got a book there with some of the early recordings on it. | 0:05:41 | 0:05:44 | |
I do. I have a book here from 1776. | 0:05:44 | 0:05:47 | |
It's some of the original recordings from Thomas Hornsby, | 0:05:47 | 0:05:50 | |
who founded this observatory. | 0:05:50 | 0:05:53 | |
And several times a day - he was much more keen than I am - | 0:05:53 | 0:05:56 | |
he came up here and took measurements | 0:05:56 | 0:05:59 | |
of pressure and temperature, | 0:05:59 | 0:06:01 | |
but he also made some quite funny notes in the margins. | 0:06:01 | 0:06:03 | |
For example, on the 26th of January 1776, | 0:06:03 | 0:06:07 | |
he wrote about how the wine in his study had started to freeze | 0:06:07 | 0:06:10 | |
because it had got very cold that day. | 0:06:10 | 0:06:12 | |
Which is a very important thing for a scientist to know about. | 0:06:12 | 0:06:14 | |
Yeah, and I'm glad that he wrote about it! | 0:06:14 | 0:06:17 | |
These are some of the earliest | 0:06:18 | 0:06:19 | |
regular measurements of temperature ever made, | 0:06:19 | 0:06:23 | |
and they were only possible thanks to one of the greatest | 0:06:23 | 0:06:25 | |
scientific innovations of the 18th century - | 0:06:25 | 0:06:29 | |
the modern thermometer. | 0:06:29 | 0:06:31 | |
The first thermometers were simple tubes filled with liquid. | 0:06:32 | 0:06:35 | |
If you put them in something warm, the liquid level would go up, | 0:06:35 | 0:06:38 | |
and if you put them in something cold, | 0:06:38 | 0:06:39 | |
the liquid level would go down. | 0:06:39 | 0:06:41 | |
That's not much use if you're trying to establish | 0:06:41 | 0:06:43 | |
a universal temperature scale that everyone can agree on. | 0:06:43 | 0:06:46 | |
Every inventor had their own idea of what that scale should be | 0:06:48 | 0:06:52 | |
and so no two thermometers were alike. | 0:06:52 | 0:06:56 | |
The solution that was arrived at was really clever. | 0:06:56 | 0:06:59 | |
It was to say that perhaps we can find fixed points. | 0:06:59 | 0:07:03 | |
So, perhaps there are situations | 0:07:03 | 0:07:04 | |
which are absolutely always the same temperature | 0:07:04 | 0:07:08 | |
and then everyone can agree on those points on the scale, | 0:07:08 | 0:07:10 | |
and then we can all calibrate our instruments. | 0:07:10 | 0:07:13 | |
The choices that stuck were those made by Daniel Fahrenheit, | 0:07:13 | 0:07:16 | |
who was a Polish physicist, | 0:07:16 | 0:07:18 | |
and he chose three fixed points that everyone else then followed. | 0:07:18 | 0:07:22 | |
So, the first one of his fixed points was this mixture here - | 0:07:22 | 0:07:26 | |
ammonium chloride and liquid water and water ice. | 0:07:26 | 0:07:30 | |
And that is a very interesting type of mixture | 0:07:30 | 0:07:32 | |
because when you mix those three things together, | 0:07:32 | 0:07:35 | |
they will find an equilibrium at a very specific temperature, | 0:07:35 | 0:07:40 | |
and Fahrenheit choice that as his starting point. | 0:07:40 | 0:07:42 | |
So, this is at zero degrees Fahrenheit. | 0:07:42 | 0:07:46 | |
Fahrenheit's second fixed point was a mixture of water and ice, | 0:07:46 | 0:07:51 | |
which will always settle at the same temperature - | 0:07:51 | 0:07:54 | |
32 degrees Fahrenheit, | 0:07:54 | 0:07:56 | |
more familiar to us these days as zero degrees Celsius. | 0:07:56 | 0:08:01 | |
And then there was one more fixed point | 0:08:01 | 0:08:03 | |
and Fahrenheit choice the temperature of the human body. | 0:08:03 | 0:08:06 | |
So, if you put a thermometer under your arm or under your tongue, | 0:08:06 | 0:08:09 | |
Fahrenheit said that was 96 on his scale, | 0:08:09 | 0:08:13 | |
and that was the beginning of the Fahrenheit scale. | 0:08:13 | 0:08:16 | |
All of those scientists and engineers | 0:08:16 | 0:08:18 | |
could calibrate their thermometers using those same three points. | 0:08:18 | 0:08:21 | |
They could divide up the temperature scale | 0:08:21 | 0:08:23 | |
in exactly the same way, | 0:08:23 | 0:08:25 | |
and, finally, the real science of temperature could begin. | 0:08:25 | 0:08:29 | |
The thermometer opened up a whole world of possibilities | 0:08:32 | 0:08:36 | |
for astronomy, meteorology, and, of course, medicine. | 0:08:36 | 0:08:41 | |
But it also brought with it a paradox. | 0:08:41 | 0:08:44 | |
While we now had a standard scale to record temperature, | 0:08:44 | 0:08:48 | |
we still didn't have any scientific explanation | 0:08:48 | 0:08:51 | |
of what temperature really was, of what made things hot or cold. | 0:08:51 | 0:08:56 | |
Some of the earliest scientific theories propose | 0:08:58 | 0:09:00 | |
that temperature was a physical substance. | 0:09:00 | 0:09:03 | |
One idea was that heat was a weightless liquid called caloric | 0:09:10 | 0:09:14 | |
that warmed things up. | 0:09:14 | 0:09:16 | |
Another theory suggested that | 0:09:16 | 0:09:18 | |
cold consisted of frigorific particles. | 0:09:18 | 0:09:22 | |
These ideas persisted until the late 18th century | 0:09:25 | 0:09:29 | |
when they were thrown into doubt by a discovery about heat | 0:09:29 | 0:09:33 | |
that would ultimately transform our understanding of cold. | 0:09:33 | 0:09:37 | |
In the 1790s, an American-born inventor | 0:09:37 | 0:09:40 | |
working in Germany called Count Rumford | 0:09:40 | 0:09:42 | |
applied his mind to the study of heat, | 0:09:42 | 0:09:44 | |
and this is the report that he wrote on his work. | 0:09:44 | 0:09:47 | |
And I love this document because it's written in a very human way. | 0:09:47 | 0:09:50 | |
Count Rumford was overseeing the manufacture of cannons | 0:09:51 | 0:09:54 | |
by German artillerymen | 0:09:54 | 0:09:56 | |
when he noticed something very curious | 0:09:56 | 0:09:58 | |
as they bored holes into the cold metal. | 0:09:58 | 0:10:01 | |
To show you, I've got a battery-powered drill | 0:10:03 | 0:10:05 | |
and an infrared camera that will reveal | 0:10:05 | 0:10:08 | |
what happens to the temperature of the metal as I drill through it. | 0:10:08 | 0:10:11 | |
And I'm just going to drill through this piece of metal here. | 0:10:11 | 0:10:14 | |
And have a look on the infrared camera. | 0:10:16 | 0:10:18 | |
You can see the spot around where I was drilling has warmed up | 0:10:18 | 0:10:21 | |
and I can feel the heat with my finger. | 0:10:21 | 0:10:23 | |
So, even a simple drilling experiment like this | 0:10:23 | 0:10:25 | |
can generate heat. | 0:10:25 | 0:10:27 | |
And this was exactly what Count Rumford observed | 0:10:28 | 0:10:32 | |
as he watched the cannon-makers at work. | 0:10:32 | 0:10:35 | |
As they bored through the metal, the cold iron got hotter. | 0:10:35 | 0:10:39 | |
The other important thing that Count Rumford noticed | 0:10:41 | 0:10:43 | |
was that the heat didn't run out. | 0:10:43 | 0:10:46 | |
You could keep drilling and the metal just got hotter. | 0:10:46 | 0:10:49 | |
And, in his opinion, that put a very big dent | 0:10:50 | 0:10:53 | |
in the theory of caloric | 0:10:53 | 0:10:54 | |
because if heat is a fluid flowing from a hot place to a cold place, | 0:10:54 | 0:10:58 | |
at some point, that fluid is going to run out. | 0:10:58 | 0:11:00 | |
Rumford had discovered something fundamental about temperature, | 0:11:02 | 0:11:06 | |
of what makes matter hot or cold, | 0:11:06 | 0:11:09 | |
yet it would be nearly a century | 0:11:09 | 0:11:11 | |
before it was fully recognised and explained. | 0:11:11 | 0:11:14 | |
And the first step towards an explanation would come | 0:11:23 | 0:11:27 | |
from a completely different branch of science altogether. | 0:11:27 | 0:11:30 | |
In 1827, Scottish botanist Robert Brown | 0:11:36 | 0:11:39 | |
was deep into his research on flowering plants. | 0:11:39 | 0:11:42 | |
It was an exciting time in biology because of the new realisation | 0:11:42 | 0:11:45 | |
that inside the very tiny plant cell, | 0:11:45 | 0:11:48 | |
there was even tinier machinery making everything work. | 0:11:48 | 0:11:52 | |
Brown was particularly interested in pollen... | 0:11:55 | 0:11:58 | |
..so he took pollen grains back to his laboratory, | 0:11:59 | 0:12:02 | |
suspended them in drops of water | 0:12:02 | 0:12:04 | |
and looked at them under his microscope. | 0:12:04 | 0:12:06 | |
And what he saw was the pollen grains sitting in the water, | 0:12:08 | 0:12:12 | |
but, from them, there were emerging even smaller particles, | 0:12:12 | 0:12:16 | |
and when he watched those particles, | 0:12:16 | 0:12:18 | |
they were moving, they were jiggling about. | 0:12:18 | 0:12:20 | |
So, the first thing that Brown did was check whether they were alive, | 0:12:20 | 0:12:24 | |
but they weren't, and he tried with lots of different materials, | 0:12:24 | 0:12:27 | |
and what he saw was that every time there was a particle that small, | 0:12:27 | 0:12:30 | |
just on the edge of what the microscope could see, | 0:12:30 | 0:12:33 | |
it would always be just jiggling about, | 0:12:33 | 0:12:35 | |
whatever it was made of, and he had no idea why that was. | 0:12:35 | 0:12:40 | |
The answer didn't come until nearly 100 years later | 0:12:40 | 0:12:43 | |
in a paper written in 1905 by Albert Einstein, | 0:12:43 | 0:12:47 | |
and it's a really elegant paper. | 0:12:47 | 0:12:49 | |
Einstein's paper drew together two crucial ideas. | 0:12:51 | 0:12:55 | |
First, that all matter was made of atoms, | 0:13:00 | 0:13:03 | |
and, second, that these atoms were constantly moving about. | 0:13:03 | 0:13:08 | |
This finally solved the mystery of Robert Brown's jiggling particles. | 0:13:09 | 0:13:14 | |
They were being bombarded by billions | 0:13:14 | 0:13:16 | |
of smaller, invisible atoms, | 0:13:16 | 0:13:20 | |
and Einstein's explanation depended on one fundamental point - | 0:13:20 | 0:13:25 | |
that the movement of atoms was directly linked | 0:13:25 | 0:13:28 | |
to their temperature. | 0:13:28 | 0:13:30 | |
The physical existence of our universe | 0:13:30 | 0:13:33 | |
is all about the relationship between matter and energy, | 0:13:33 | 0:13:37 | |
and this paper was where that story really started. | 0:13:37 | 0:13:41 | |
Einstein understood that heat is just the energy that atoms have | 0:13:41 | 0:13:45 | |
due to their movement, | 0:13:45 | 0:13:47 | |
and the measure of that movement energy is temperature. | 0:13:47 | 0:13:51 | |
The more energy, the faster the movement | 0:13:53 | 0:13:56 | |
and the higher the temperature. | 0:13:56 | 0:13:58 | |
More than a century after Rumford had puzzled over | 0:13:58 | 0:14:01 | |
what was heating up his cannons, Einstein had explained it. | 0:14:01 | 0:14:06 | |
The very act of boring through the metal | 0:14:06 | 0:14:09 | |
was adding energy to the atoms, | 0:14:09 | 0:14:12 | |
increasing their movement and, so, making the metal hotter. | 0:14:12 | 0:14:16 | |
This definition of heat also means something profound | 0:14:17 | 0:14:21 | |
for our understanding of cold | 0:14:21 | 0:14:24 | |
because if heat is the measure of energy, | 0:14:24 | 0:14:26 | |
of the movement of atoms, | 0:14:26 | 0:14:28 | |
then cold is simply an absence of energy, | 0:14:28 | 0:14:31 | |
a lack of motion. | 0:14:31 | 0:14:32 | |
And this is vital to understanding | 0:14:42 | 0:14:44 | |
how every single solid thing in our universe came into being. | 0:14:44 | 0:14:49 | |
To show you why, I'm back in Iceland - | 0:15:01 | 0:15:04 | |
the perfect place to explore the relationship | 0:15:04 | 0:15:07 | |
between cold and matter. | 0:15:07 | 0:15:09 | |
This is Breidamerkurjokull Glacier. | 0:15:11 | 0:15:14 | |
Here, matter exists side by side in three very different forms. | 0:15:14 | 0:15:19 | |
This is made of water molecules, | 0:15:26 | 0:15:28 | |
there's water molecules dripping off the roof here, | 0:15:28 | 0:15:31 | |
and the air I'm breathing out also contains some water molecules. | 0:15:31 | 0:15:35 | |
Billions upon billions of the same type of molecule | 0:15:35 | 0:15:39 | |
all in the same place, | 0:15:39 | 0:15:41 | |
but behaving in three different ways - | 0:15:41 | 0:15:44 | |
as a solid, a liquid, and a gas. | 0:15:44 | 0:15:47 | |
Each of these three states is a consequence of temperature, | 0:15:50 | 0:15:55 | |
of how fast the molecules of water are moving... | 0:15:55 | 0:15:58 | |
..and when the water reaches its freezing point | 0:15:59 | 0:16:01 | |
and changes from a liquid to a solid, | 0:16:01 | 0:16:04 | |
something extraordinary is happening | 0:16:04 | 0:16:06 | |
in the hidden world of its molecules, | 0:16:06 | 0:16:09 | |
something we can't see by looking at ice at this massive scale. | 0:16:09 | 0:16:14 | |
To understand it, we need to look at something very much smaller, | 0:16:14 | 0:16:18 | |
something that's also frozen, even if it might not look like it. | 0:16:18 | 0:16:23 | |
This is table salt - sodium chloride. | 0:16:23 | 0:16:26 | |
About as common as you can get. | 0:16:26 | 0:16:28 | |
And, even here, you can see that the salt's a little bit sparkly. | 0:16:28 | 0:16:33 | |
If I put it under the microscope, now you can see what's going on. | 0:16:33 | 0:16:38 | |
Those tiny little grains of salt here have flat faces - | 0:16:38 | 0:16:43 | |
they're little cubes - and every single grain is the same. | 0:16:43 | 0:16:47 | |
Not a perfect cube, but they've all got a cubic shape, | 0:16:47 | 0:16:50 | |
and it's those flat faces that are reflecting the light | 0:16:50 | 0:16:52 | |
and making the salt sparkle. | 0:16:52 | 0:16:54 | |
And that's an indication of something deeper down | 0:16:54 | 0:16:57 | |
in the structure of the salt. | 0:16:57 | 0:16:59 | |
Salt is made of equal numbers of sodium and chloride ions. | 0:17:03 | 0:17:08 | |
The chloride ions are assembled in rows and columns, | 0:17:08 | 0:17:11 | |
so that they sit on a square grid. | 0:17:11 | 0:17:14 | |
The smaller sodium ions fit into the spaces in between. | 0:17:14 | 0:17:19 | |
A salt crystal is just a giant grid, like this - | 0:17:19 | 0:17:22 | |
a cube that's a million or so atoms long on each side. | 0:17:22 | 0:17:27 | |
This is the hidden structure of a crystal. | 0:17:27 | 0:17:31 | |
Its atoms are no longer free to move around each other. | 0:17:31 | 0:17:35 | |
Each one is locked in its own place on the grid. | 0:17:35 | 0:17:38 | |
So, the salt looks like that here. | 0:17:40 | 0:17:42 | |
It would look like that if I took it into a sauna because it's frozen. | 0:17:42 | 0:17:46 | |
It's a frozen solid. | 0:17:46 | 0:17:47 | |
Freezing is simply what happens when the molecules of a substance | 0:17:49 | 0:17:53 | |
no longer have enough energy to move past each other, | 0:17:53 | 0:17:57 | |
and so they become fixed in position. | 0:17:57 | 0:18:00 | |
And this doesn't always happen at a temperature | 0:18:00 | 0:18:02 | |
that we would consider cold. | 0:18:02 | 0:18:04 | |
For salt, it happens at about 800 degrees Celsius. | 0:18:04 | 0:18:09 | |
We associate freezing with water ice, | 0:18:11 | 0:18:13 | |
but that's just because water is important to us. | 0:18:13 | 0:18:17 | |
The concept of freezing is far bigger, | 0:18:17 | 0:18:19 | |
and the transition from liquid to solid | 0:18:19 | 0:18:21 | |
can happen at a huge range of temperatures, | 0:18:21 | 0:18:24 | |
depending on the substance. | 0:18:24 | 0:18:26 | |
Liquid iron freezes to become a solid metal | 0:18:28 | 0:18:31 | |
at around 1,500 degrees Celsius. | 0:18:31 | 0:18:34 | |
Liquid tungsten turns into a solid | 0:18:35 | 0:18:38 | |
at nearly 3,500 degrees Celsius. | 0:18:38 | 0:18:42 | |
It's exactly the same process | 0:18:44 | 0:18:46 | |
that transforms liquid water into solid ice | 0:18:46 | 0:18:50 | |
at zero degrees Celsius. | 0:18:50 | 0:18:52 | |
As with other liquids, the molecules in liquid water | 0:18:54 | 0:18:57 | |
have enough energy to keep moving past each other. | 0:18:57 | 0:19:00 | |
But, as they cool, the molecules slow down. | 0:19:00 | 0:19:04 | |
As water reaches its freezing point, | 0:19:04 | 0:19:06 | |
they arrange themselves in tightly fixed positions, | 0:19:06 | 0:19:10 | |
forming a hexagonal lattice - a crystalline structure. | 0:19:10 | 0:19:14 | |
The beautiful symmetry of snowflakes comes, in part, | 0:19:23 | 0:19:26 | |
from this microscopic hexagonal form. | 0:19:26 | 0:19:29 | |
Here, deep in this cave of ice, it exists on a massive scale, | 0:19:33 | 0:19:39 | |
and, in fact, the very process of cooling and freezing is key | 0:19:39 | 0:19:42 | |
to how the entire planet formed. | 0:19:42 | 0:19:45 | |
Some 4 billion years ago, | 0:19:52 | 0:19:54 | |
the Earth was covered in molten rock. | 0:19:54 | 0:19:56 | |
As we've seen in the striking landscapes of Iceland, | 0:19:58 | 0:20:01 | |
that lava eventually cooled and froze into solid rock, | 0:20:01 | 0:20:06 | |
and, sometimes, the way it cooled | 0:20:06 | 0:20:09 | |
created something truly extraordinary. | 0:20:09 | 0:20:12 | |
The hexagonal columns of basalt at Reynisfjara | 0:20:13 | 0:20:17 | |
are one of Earth's natural wonders | 0:20:17 | 0:20:20 | |
and Professor Thor Thordarson, | 0:20:20 | 0:20:22 | |
a volcanologist from the University of Iceland, | 0:20:22 | 0:20:25 | |
is going to help me understand how they formed. | 0:20:25 | 0:20:28 | |
There's lots of basalt in the world, | 0:20:30 | 0:20:32 | |
but not all of it has this amazing structure here. | 0:20:32 | 0:20:36 | |
So, here, we have these beautiful, regular columns, | 0:20:36 | 0:20:38 | |
and these extend 10m, 15m up into the cliff edge. | 0:20:38 | 0:20:41 | |
Columns like this are fairly unusual. | 0:20:41 | 0:20:44 | |
These columns tell a story | 0:20:50 | 0:20:52 | |
of how the intricacies of cooling and freezing | 0:20:52 | 0:20:56 | |
have shaped the fabric of our planet. | 0:20:56 | 0:20:58 | |
So, this column here, which is about 80cm in width here, | 0:21:01 | 0:21:05 | |
this width is actually the function of the cooling. | 0:21:05 | 0:21:08 | |
So, if you think of a lava flow, it starts cooling from the surface, | 0:21:09 | 0:21:14 | |
and it also cools fastest when it is close... | 0:21:14 | 0:21:19 | |
in contact with the atmosphere. | 0:21:19 | 0:21:21 | |
As the lava cools and freezes, it also shrinks, | 0:21:24 | 0:21:29 | |
as its molecules arrange themselves into a solid structure. | 0:21:29 | 0:21:32 | |
This happens more quickly at the surface, | 0:21:34 | 0:21:36 | |
where the lava meets the air, | 0:21:36 | 0:21:38 | |
and more slowly underneath, where it stays warmer. | 0:21:38 | 0:21:42 | |
And if the rate of shrinking is great enough, | 0:21:42 | 0:21:45 | |
the cooling lava at the surface is under so much stress that it cracks, | 0:21:45 | 0:21:50 | |
and often the most efficient way | 0:21:50 | 0:21:52 | |
to dissipate this huge build-up of stress | 0:21:52 | 0:21:54 | |
is to crack at an angle of 120 degrees - | 0:21:54 | 0:21:58 | |
the angle that gives us a hexagon. | 0:21:58 | 0:22:00 | |
As the rock beneath the surface also continues to cool, | 0:22:01 | 0:22:05 | |
these cracks extend downwards, | 0:22:05 | 0:22:07 | |
creating the colossal pillars we see today. | 0:22:07 | 0:22:11 | |
Can you tell from the size of these how quickly these cooled? | 0:22:12 | 0:22:15 | |
I mean, did these take a day to form, or a week, or a year? | 0:22:15 | 0:22:18 | |
Can you tell? | 0:22:18 | 0:22:20 | |
Not exactly, but I would guess between ten and 20 years. | 0:22:20 | 0:22:23 | |
This landscape was formed because lava began to cool and freeze | 0:22:27 | 0:22:31 | |
at just the right speed for the laws of physics to create a masterpiece. | 0:22:31 | 0:22:37 | |
A little faster or slower, and these columns wouldn't exist. | 0:22:37 | 0:22:41 | |
They stand as evidence that solid rock, | 0:22:43 | 0:22:46 | |
the fabric of our world, is frozen, | 0:22:46 | 0:22:50 | |
and the architect that sculpted it is temperature. | 0:22:50 | 0:22:54 | |
And as we humans have built architectural wonders of our own, | 0:23:11 | 0:23:15 | |
so we've learned to harness the potential of cooling, | 0:23:15 | 0:23:19 | |
to change the very nature of matter. | 0:23:19 | 0:23:22 | |
This is Ely Cathedral. | 0:23:27 | 0:23:30 | |
It's been here for nearly 1,000 years, | 0:23:30 | 0:23:32 | |
and, over the centuries, | 0:23:32 | 0:23:34 | |
countless craftsmen have taken local raw materials, | 0:23:34 | 0:23:37 | |
limestone and oak, | 0:23:37 | 0:23:39 | |
and transformed them into this vast and intricate structure. | 0:23:39 | 0:23:43 | |
But I'm not here because of those materials. | 0:23:48 | 0:23:51 | |
I'm here to see something else. | 0:23:51 | 0:23:54 | |
The stained glass windows here are breathtaking, | 0:23:54 | 0:23:57 | |
and they only exist thanks to the unique properties of glass | 0:23:57 | 0:24:01 | |
that emerge as it cools. | 0:24:01 | 0:24:03 | |
It's only when you're right in close like this | 0:24:08 | 0:24:11 | |
that you can really appreciate these fabulous windows. | 0:24:11 | 0:24:14 | |
Each one of these panels | 0:24:14 | 0:24:15 | |
is illuminating the cathedral with a story. | 0:24:15 | 0:24:19 | |
But the story that you can see from down there | 0:24:19 | 0:24:21 | |
is built of a thousand smaller stories | 0:24:21 | 0:24:24 | |
that you can only see up here | 0:24:24 | 0:24:25 | |
because every single one of these pieces of glass | 0:24:25 | 0:24:29 | |
is carrying its own distinctive history | 0:24:29 | 0:24:32 | |
of how cooling shaped it and locked in its properties. | 0:24:32 | 0:24:36 | |
To understand why, | 0:24:45 | 0:24:47 | |
I've come to meet someone who works with glass day in, day out. | 0:24:47 | 0:24:52 | |
This is Walter Pinches, | 0:24:52 | 0:24:54 | |
a glass-maker carrying on a tradition | 0:24:54 | 0:24:57 | |
that's changed little in 800 years. | 0:24:57 | 0:25:00 | |
-How hot is it in there? -1,250-1,300. | 0:25:02 | 0:25:05 | |
1,300 degrees C? | 0:25:05 | 0:25:06 | |
It's only 2m away! | 0:25:08 | 0:25:10 | |
SHE LAUGHS | 0:25:10 | 0:25:13 | |
Standing next to the fiery glow of the furnace, | 0:25:13 | 0:25:16 | |
it's easy to think that the key to glass-making is heat. | 0:25:16 | 0:25:20 | |
But the real key to this process is what happens | 0:25:20 | 0:25:22 | |
when the glass comes out of the furnace and begins to cool. | 0:25:22 | 0:25:25 | |
And the colour's just mixing into the liquid as you go along. | 0:25:27 | 0:25:30 | |
The colour's already twisted in. You've already got your pattern. | 0:25:30 | 0:25:33 | |
Cooling is a process that craftsmen like Walter | 0:25:34 | 0:25:37 | |
learn to control precisely. | 0:25:37 | 0:25:40 | |
When the hot glass first emerges, it's molten, | 0:25:40 | 0:25:44 | |
so, like all liquids, | 0:25:44 | 0:25:45 | |
its molecules are still free to move and slide over each other, | 0:25:45 | 0:25:50 | |
and this gives Walter a brief window of time to manipulate its shape. | 0:25:50 | 0:25:56 | |
But, with every passing second, the glass is cooling, | 0:25:56 | 0:26:00 | |
especially at the surface, where it's in contact with the air. | 0:26:00 | 0:26:03 | |
What's amazing about this is that the inside and the outside | 0:26:04 | 0:26:07 | |
are different temperatures, and right in at a molecular level, | 0:26:07 | 0:26:10 | |
everything in there is different. | 0:26:10 | 0:26:12 | |
Everywhere is behaving differently because of its temperature. | 0:26:12 | 0:26:16 | |
Starting at the surface, the glass begins to freeze. | 0:26:18 | 0:26:22 | |
Its atoms slow down and come to rest in fixed positions, | 0:26:22 | 0:26:26 | |
and they do so in a way that's unlike many other solids. | 0:26:26 | 0:26:30 | |
This is my favourite bit - when it just blows up like a balloon. | 0:26:30 | 0:26:34 | |
As we've seen, when other substances freeze, | 0:26:36 | 0:26:39 | |
like water or salt, their atoms become fixed | 0:26:39 | 0:26:42 | |
in the ordered structure of a crystal. | 0:26:42 | 0:26:45 | |
But glass is different. | 0:26:45 | 0:26:48 | |
It cools more quickly and so its atoms don't have time | 0:26:48 | 0:26:51 | |
to arrange themselves in a regular pattern. | 0:26:51 | 0:26:54 | |
Instead, they freeze in the disordered, | 0:26:55 | 0:26:58 | |
chaotic arrangement of a liquid, | 0:26:58 | 0:27:01 | |
and this gives glass one of its most valuable properties. | 0:27:01 | 0:27:06 | |
Unconstrained by a rigid, crystalline structure, | 0:27:06 | 0:27:10 | |
it can be worked and manipulated into an infinite number of forms. | 0:27:10 | 0:27:15 | |
This is the clever bit - | 0:27:20 | 0:27:22 | |
hot molecules at the bottom flowing quickly, | 0:27:22 | 0:27:24 | |
cooler ones at the top flowing more slowly. | 0:27:24 | 0:27:27 | |
By precisely controlling the heating and cooling of glass, | 0:27:34 | 0:27:38 | |
craftsmen like Walter can create shapes and forms | 0:27:38 | 0:27:42 | |
that are truly unique. | 0:27:42 | 0:27:44 | |
Liquids are at their most beautiful when they're flowing freely, | 0:27:47 | 0:27:50 | |
but they change so quickly | 0:27:50 | 0:27:52 | |
that we almost never get to appreciate the details. | 0:27:52 | 0:27:55 | |
But glass-blowing is this fabulous process | 0:27:55 | 0:27:58 | |
of sculpting a moment in time | 0:27:58 | 0:28:00 | |
and then catching it by cooling it for us all to admire. | 0:28:00 | 0:28:04 | |
The modern world is built of solids like glass | 0:28:12 | 0:28:15 | |
that we created by controlling the process of cooling and freezing. | 0:28:15 | 0:28:19 | |
But that change from liquid to solid isn't the end of the story. | 0:28:32 | 0:28:37 | |
As a solid becomes colder, it may outwardly look the same, | 0:28:40 | 0:28:44 | |
but, in the hidden world of atoms and molecules, | 0:28:44 | 0:28:48 | |
it can still be changing | 0:28:48 | 0:28:50 | |
in ways that utterly transform how it behaves. | 0:28:50 | 0:28:55 | |
And, occasionally, when we fail to understand these changes, | 0:28:55 | 0:28:59 | |
our pursuit of progress has ended in catastrophe. | 0:28:59 | 0:29:04 | |
Some events in history are so unexpected, so shocking | 0:29:04 | 0:29:08 | |
that the mentality of an entire society is divided | 0:29:08 | 0:29:11 | |
into before and after. | 0:29:11 | 0:29:14 | |
And, for our nation's maritime history, | 0:29:14 | 0:29:16 | |
that cusp came on the 15th of April 1912, | 0:29:16 | 0:29:20 | |
when news filtered out from London and New York | 0:29:20 | 0:29:24 | |
that the gigantic Titanic, that unsinkable symbol of luxury, | 0:29:24 | 0:29:29 | |
had struck an iceberg and had sunk. | 0:29:29 | 0:29:31 | |
There were 2,200 people on that ship, | 0:29:32 | 0:29:36 | |
and 70% of them died that day. | 0:29:36 | 0:29:38 | |
Titanic was built from state-of-the-art steel. | 0:29:46 | 0:29:50 | |
As with glass, we'd learned over centuries | 0:29:50 | 0:29:53 | |
to make steel incredibly strong | 0:29:53 | 0:29:56 | |
through precisely honed processes of heating and cooling. | 0:29:56 | 0:30:00 | |
Nobody doubted she was strong enough | 0:30:00 | 0:30:03 | |
to stand up to the extreme cold of the Arctic. | 0:30:03 | 0:30:07 | |
To understand what went wrong, | 0:30:08 | 0:30:10 | |
I've come to the Cammell Laird shipyard in Merseyside | 0:30:10 | 0:30:14 | |
where marine engineers are working on their latest project. | 0:30:14 | 0:30:18 | |
I've been on a lot of ships, | 0:30:21 | 0:30:23 | |
but I haven't ever been quite this excited | 0:30:23 | 0:30:25 | |
to be on the back deck of a ship | 0:30:25 | 0:30:27 | |
because this is the Royal Research Ship | 0:30:27 | 0:30:29 | |
Sir David Attenborough in the process of being built. | 0:30:29 | 0:30:33 | |
We're surrounded by the innards of a ship, | 0:30:33 | 0:30:35 | |
all these individual pieces that will build the final structure. | 0:30:35 | 0:30:40 | |
And what's brilliant about it is that the oceans are raw | 0:30:40 | 0:30:42 | |
and the structures you need to sail on them are raw, | 0:30:42 | 0:30:45 | |
and this is what's going on - | 0:30:45 | 0:30:47 | |
steel being welded to build one of the most modern | 0:30:47 | 0:30:51 | |
polar research ships in the world. | 0:30:51 | 0:30:53 | |
Joining me on board the Sir David Attenborough | 0:30:57 | 0:30:59 | |
is Captain Ralph Stevens. | 0:30:59 | 0:31:01 | |
It will be his responsibility to navigate this huge vessel | 0:31:01 | 0:31:06 | |
through icy polar waters. | 0:31:06 | 0:31:08 | |
It's astonishing to me that we're still building ships of steel. | 0:31:09 | 0:31:12 | |
You know, we associate steel with the Industrial Revolution | 0:31:12 | 0:31:15 | |
150 years ago, and, yet, we are still building ships from steel. | 0:31:15 | 0:31:18 | |
Why is it so good? | 0:31:18 | 0:31:19 | |
Well, for us, it's quite a revolutionary material | 0:31:19 | 0:31:23 | |
in that it allows us to take impacts. | 0:31:23 | 0:31:26 | |
It's quite common for us to say some of the ice is as hard as steel. | 0:31:26 | 0:31:30 | |
And some of the glacial ice, it's rock-hard | 0:31:30 | 0:31:33 | |
and it's noticeably different. | 0:31:33 | 0:31:34 | |
When you hit a piece, you'll hear a big clang throughout the ship. | 0:31:34 | 0:31:37 | |
LOUD CLANG | 0:31:37 | 0:31:40 | |
And so we want the hull to be able to take all of these forces | 0:31:40 | 0:31:43 | |
that it's exposed to without cracking. | 0:31:43 | 0:31:46 | |
And steel can do that job? | 0:31:46 | 0:31:47 | |
Steel can do that. The right steel can do that. | 0:31:47 | 0:31:49 | |
But, ironically, steel may actually have been Titanic's Achilles heel... | 0:31:51 | 0:31:56 | |
..because what the engineers of the day didn't fully understand | 0:31:58 | 0:32:01 | |
is that, under certain conditions, | 0:32:01 | 0:32:04 | |
the behaviour of steel can fundamentally change. | 0:32:04 | 0:32:07 | |
And the key to this change was cold. | 0:32:09 | 0:32:12 | |
Steel, like many metals, is ductile. | 0:32:16 | 0:32:19 | |
That means it can stretch when put under stress - | 0:32:19 | 0:32:22 | |
a property that's useful in a huge structure like a ship. | 0:32:22 | 0:32:27 | |
Few had imagined that, in the cold, this crucial property might change. | 0:32:27 | 0:32:32 | |
Got a sample of shipbuilding steel here | 0:32:33 | 0:32:35 | |
with a little notch in the bottom, | 0:32:35 | 0:32:37 | |
and I'm going to do this experiment twice - | 0:32:37 | 0:32:39 | |
once with this one, which is at room temperature, | 0:32:39 | 0:32:42 | |
and once with an identical sample, | 0:32:42 | 0:32:44 | |
which has been in the dry ice here at minus 80 Celsius. | 0:32:44 | 0:32:47 | |
Very, very cold. The difference will be very obvious. | 0:32:47 | 0:32:50 | |
So, here we go. | 0:32:50 | 0:32:52 | |
First, the steel at room temperature. | 0:32:52 | 0:32:54 | |
So, here's the cold one, down at minus 80 Celsius. | 0:33:07 | 0:33:11 | |
This is the sample at room temperature, | 0:33:22 | 0:33:24 | |
and you can see that it bent, absorbed the energy, | 0:33:24 | 0:33:27 | |
absorbed the energy, but it didn't snap, | 0:33:27 | 0:33:29 | |
whereas this one - this is the cold temperature one - | 0:33:29 | 0:33:32 | |
and the surface looks really different. | 0:33:32 | 0:33:34 | |
There's all this speckled pattern and that's a snap. | 0:33:34 | 0:33:37 | |
This was brittle fracture. You don't want your ship doing this. | 0:33:37 | 0:33:41 | |
Cold has changed the nature of the steel, | 0:33:43 | 0:33:46 | |
making it more brittle. | 0:33:46 | 0:33:48 | |
And it's this that some experts now think | 0:33:50 | 0:33:52 | |
could have played a significant role in the Titanic disaster. | 0:33:52 | 0:33:56 | |
Analysis of metal taken from the wreckage | 0:33:58 | 0:34:01 | |
suggests that, rather than flexing on collision with the iceberg, | 0:34:01 | 0:34:05 | |
the hull and rivets had become brittle and they fractured. | 0:34:05 | 0:34:10 | |
With this in mind, modern shipbuilders are able | 0:34:19 | 0:34:22 | |
to avoid the mistakes of their predecessors. | 0:34:22 | 0:34:25 | |
We did some calculations. | 0:34:27 | 0:34:29 | |
We went through the last ten years of temperatures | 0:34:29 | 0:34:32 | |
our ships have been exposed to. | 0:34:32 | 0:34:34 | |
We came to 25 degrees and then reduced it down to minus 35. | 0:34:34 | 0:34:38 | |
So, the game is that you want the steel to give a little bit, | 0:34:38 | 0:34:41 | |
-but not snap. -That's it. | 0:34:41 | 0:34:43 | |
We don't... We can't afford to have it fracture, | 0:34:43 | 0:34:45 | |
and if the worst came to the worst, | 0:34:45 | 0:34:47 | |
you want that steel to deform rather than crack. | 0:34:47 | 0:34:50 | |
The tragic irony of Titanic is that she was constructed from metals | 0:34:53 | 0:34:58 | |
that we've been using for centuries. | 0:34:58 | 0:35:00 | |
We thought we understood them... | 0:35:03 | 0:35:05 | |
..but cold altered them in ways that no-one expected. | 0:35:07 | 0:35:12 | |
Since then, we've been much more aware | 0:35:19 | 0:35:22 | |
of the hidden changes that can occur within materials | 0:35:22 | 0:35:25 | |
when they're cooled far below their freezing point. | 0:35:25 | 0:35:30 | |
And, by pushing temperatures lower and lower, | 0:35:30 | 0:35:33 | |
we're beginning to unlock some strange and exciting | 0:35:33 | 0:35:36 | |
new properties of matter. | 0:35:36 | 0:35:38 | |
This is a material with a very long name. | 0:35:42 | 0:35:44 | |
It's yttrium barium copper oxide, and it doesn't look like very much. | 0:35:44 | 0:35:49 | |
There's very strong magnets here and it's not responding to them. | 0:35:49 | 0:35:53 | |
It doesn't conduct electricity. | 0:35:53 | 0:35:55 | |
Doesn't seem very interesting, | 0:35:55 | 0:35:56 | |
but, when you cool it down, it changes completely. | 0:35:56 | 0:35:59 | |
Using liquid nitrogen, I'm reducing the temperature of the disc | 0:36:00 | 0:36:04 | |
to minus 196 degrees Celsius. | 0:36:04 | 0:36:08 | |
And, now, when I bring it close to the magnets, | 0:36:08 | 0:36:12 | |
something unexpected happens. | 0:36:12 | 0:36:14 | |
It's levitating. | 0:36:19 | 0:36:21 | |
And it will scoot around on the little track here for quite a while. | 0:36:23 | 0:36:27 | |
So, something's changed. We've cooled it down. | 0:36:27 | 0:36:29 | |
The behaviour changed completely. | 0:36:29 | 0:36:30 | |
And that's because cold has altered the material at the atomic scale. | 0:36:33 | 0:36:38 | |
Materials conduct electricity when electrons travel through them, | 0:36:40 | 0:36:45 | |
but the atoms in a conductor are an obstacle to the flow of electrons | 0:36:45 | 0:36:49 | |
because, as electrons bump into them, they lose energy. | 0:36:49 | 0:36:53 | |
At extremely low temperatures, | 0:36:53 | 0:36:56 | |
the electrons can team up into pairs | 0:36:56 | 0:36:59 | |
and then the attraction between the electron pairs | 0:36:59 | 0:37:02 | |
helps them navigate through the atoms far more easily. | 0:37:02 | 0:37:05 | |
So, when I bring the disc close to the magnetic track, | 0:37:07 | 0:37:10 | |
a strong electric current begins to flow in the disc. | 0:37:10 | 0:37:15 | |
This, in turn, generates its own magnetic field. | 0:37:15 | 0:37:19 | |
The magnets in the track and the disc repel each other, | 0:37:19 | 0:37:22 | |
and so the disc levitates. | 0:37:22 | 0:37:24 | |
This is an example of superconductivity. | 0:37:24 | 0:37:27 | |
Once it's cooled down below the critical temperature, | 0:37:27 | 0:37:30 | |
the properties of the material change. | 0:37:30 | 0:37:32 | |
It becomes able to conduct electrical currents | 0:37:32 | 0:37:35 | |
without any resistance. | 0:37:35 | 0:37:36 | |
And it also changes how it responds to magnets. | 0:37:36 | 0:37:41 | |
The peculiar electromagnetic properties | 0:37:43 | 0:37:45 | |
of supercooled materials | 0:37:45 | 0:37:47 | |
have given us a powerful new tool in engineering and medicine. | 0:37:47 | 0:37:51 | |
Some countries already use a super-sized version | 0:37:55 | 0:37:58 | |
of this magnetic levitation effect in their high-speed rail systems. | 0:37:58 | 0:38:03 | |
Having no contact with the track, | 0:38:03 | 0:38:06 | |
trains run faster and more smoothly and efficiently. | 0:38:06 | 0:38:09 | |
And, inside MRI scanners, | 0:38:11 | 0:38:13 | |
liquid helium supercools massive coils of copper wire | 0:38:13 | 0:38:18 | |
to a temperature of minus 269 degrees Celsius. | 0:38:18 | 0:38:23 | |
At this extreme cold, | 0:38:23 | 0:38:25 | |
an electric current can flow with almost zero resistance, | 0:38:25 | 0:38:29 | |
which helps generate the powerful and stable magnetic field | 0:38:29 | 0:38:33 | |
that the MRI machine needs. | 0:38:33 | 0:38:35 | |
The extraordinary discoveries we've made | 0:38:38 | 0:38:40 | |
at extremely low temperatures are now driving | 0:38:40 | 0:38:43 | |
one of the biggest scientific quests of the modern age. | 0:38:43 | 0:38:48 | |
How cold is it possible to go? | 0:38:48 | 0:38:51 | |
How do we get there? | 0:38:51 | 0:38:53 | |
And what new properties of matter might we uncover? | 0:38:53 | 0:38:57 | |
The first step on that journey is to understand how things cool down. | 0:39:02 | 0:39:06 | |
Take this humble cup of tea. | 0:39:11 | 0:39:14 | |
I always drink my tea far too quickly | 0:39:16 | 0:39:18 | |
because the experience of a lifetime tells me that, if I don't, | 0:39:18 | 0:39:21 | |
it will cool down. | 0:39:21 | 0:39:23 | |
Heat will flow out of the tea, which is warm, | 0:39:23 | 0:39:25 | |
into its surroundings, which are cooler. | 0:39:25 | 0:39:28 | |
If I look at this glass of iced water here, | 0:39:28 | 0:39:30 | |
this is cooler than the surroundings, | 0:39:30 | 0:39:32 | |
and, if I leave that alone, it will heat up | 0:39:32 | 0:39:34 | |
until it matches the temperature of everything around it. | 0:39:34 | 0:39:37 | |
This is a demonstration of a fundamental principle of physics - | 0:39:41 | 0:39:45 | |
the second law of thermodynamics. | 0:39:45 | 0:39:48 | |
Heat flows from hot to cold until equilibrium is reached. | 0:39:48 | 0:39:55 | |
We can see this in action through the thermal imaging camera. | 0:39:55 | 0:39:58 | |
The hot tea is cooling and the chilled water is warming | 0:39:58 | 0:40:03 | |
until both are the same temperature as their surroundings. | 0:40:03 | 0:40:07 | |
It's a law that can't be broken, but it also raises a question. | 0:40:07 | 0:40:13 | |
How can you ever make something colder than its surroundings, | 0:40:13 | 0:40:17 | |
like an ice cube? | 0:40:17 | 0:40:19 | |
Here's the problem. | 0:40:20 | 0:40:21 | |
At some point, this ice was liquid water, | 0:40:21 | 0:40:24 | |
and, to cool it down, to freeze it, | 0:40:24 | 0:40:26 | |
heat had to flow out of it to make it colder, | 0:40:26 | 0:40:30 | |
but that seems to go against this fundamental law. | 0:40:30 | 0:40:33 | |
So, how is this possible? | 0:40:33 | 0:40:35 | |
The answer to that question can be found here. | 0:40:39 | 0:40:42 | |
This 33,000-square-metre | 0:40:45 | 0:40:48 | |
food distribution centre in Warwickshire | 0:40:48 | 0:40:50 | |
handles almost 200,000 home grocery deliveries every day, | 0:40:50 | 0:40:56 | |
and much of it is chilled well below ambient temperature. | 0:40:56 | 0:41:01 | |
The invention of refrigeration | 0:41:01 | 0:41:03 | |
made an enormous difference to our society | 0:41:03 | 0:41:05 | |
because it allowed us to control our food supply. | 0:41:05 | 0:41:09 | |
So, something like this - frozen carrots - | 0:41:09 | 0:41:12 | |
was probably frozen just after it left the field, and, since then, | 0:41:12 | 0:41:16 | |
it's passed through an unbroken chain of cold - | 0:41:16 | 0:41:19 | |
refrigerated lorries, refrigerated warehouses, | 0:41:19 | 0:41:21 | |
all the way to us, | 0:41:21 | 0:41:23 | |
and places like this gigantic freezer are part of that. | 0:41:23 | 0:41:27 | |
And, after being in here, | 0:41:27 | 0:41:29 | |
I will never take frozen food for granted ever again | 0:41:29 | 0:41:32 | |
because it's so cold. It's minus 22! | 0:41:32 | 0:41:35 | |
And when you stop to think about that, it's strange. | 0:41:40 | 0:41:44 | |
How DO you make this building so much colder | 0:41:44 | 0:41:47 | |
than the ambient temperature here in balmy Warwickshire? | 0:41:47 | 0:41:51 | |
The secret to this place is the same as the hidden workings | 0:41:52 | 0:41:55 | |
of the fridge-freezer in your kitchen... | 0:41:55 | 0:41:57 | |
..and it begins with something counterintuitive. | 0:41:58 | 0:42:01 | |
The odd thing about the process of making something cold | 0:42:03 | 0:42:06 | |
is that it starts with a huge input of energy, | 0:42:06 | 0:42:09 | |
and that happens here. | 0:42:09 | 0:42:11 | |
These are compressors. | 0:42:11 | 0:42:13 | |
They're taking ammonia gas, and all the energy is being used | 0:42:13 | 0:42:17 | |
to squeeze the gas to a high pressure. | 0:42:17 | 0:42:20 | |
And, at the same time, that heats it up, | 0:42:20 | 0:42:23 | |
so what leaves here is both at high pressure and high temperature. | 0:42:23 | 0:42:28 | |
Next, this pressurised ammonia needs to be cooled down. | 0:42:32 | 0:42:36 | |
Ammonia gas comes out of the plant room downstairs | 0:42:38 | 0:42:41 | |
at 100 degrees C, and this is where it's cooled down. | 0:42:41 | 0:42:46 | |
It's flowing through all these pipes in the inside of here. | 0:42:46 | 0:42:49 | |
And the water falling down is cooling it down | 0:42:49 | 0:42:53 | |
much closer to room temperature. | 0:42:53 | 0:42:55 | |
This is where the energy is lost | 0:42:55 | 0:42:57 | |
from the refrigerant fluid - the ammonia. | 0:42:57 | 0:43:00 | |
By the time it leaves here, it's much cooler and it's a liquid. | 0:43:00 | 0:43:04 | |
Crucially, even though the ammonia is now cooler, | 0:43:07 | 0:43:10 | |
it's still under pressure. | 0:43:10 | 0:43:12 | |
Releasing this pressure is the secret | 0:43:14 | 0:43:16 | |
of how this vast warehouse space is cooled, | 0:43:16 | 0:43:19 | |
and I can show you how using something very familiar. | 0:43:19 | 0:43:22 | |
What happens is the same as when you have an aerosol spray | 0:43:24 | 0:43:28 | |
and you spray it and you can see it. I've got a thermometer here. | 0:43:28 | 0:43:31 | |
If I spray the bottom of the thermometer, | 0:43:32 | 0:43:33 | |
the temperature goes right down. | 0:43:33 | 0:43:36 | |
This process is called adiabatic cooling. | 0:43:36 | 0:43:40 | |
As the high-pressure gas leaves the can, | 0:43:40 | 0:43:43 | |
it pushes outwards on the air around it and expands. | 0:43:43 | 0:43:47 | |
But that push uses energy that can only come | 0:43:47 | 0:43:51 | |
from the movement of the atoms, | 0:43:51 | 0:43:53 | |
and so the expanding gas cools down. | 0:43:53 | 0:43:56 | |
The exact same process happens | 0:43:58 | 0:44:00 | |
as liquid ammonia is pumped into the warehouse. | 0:44:00 | 0:44:03 | |
The high-pressure liquid passes through a valve, | 0:44:03 | 0:44:06 | |
and, still contained within the pipes, | 0:44:06 | 0:44:08 | |
it rapidly expands into a gas | 0:44:08 | 0:44:11 | |
causing its temperature to instantly drop. | 0:44:11 | 0:44:14 | |
Heat then flows from the warm air inside the warehouse | 0:44:15 | 0:44:18 | |
to the much colder ammonia until they reach equilibrium, | 0:44:18 | 0:44:23 | |
just as the second law of thermodynamics | 0:44:23 | 0:44:26 | |
dictate they should. | 0:44:26 | 0:44:28 | |
And, since the equilibrium temperature | 0:44:28 | 0:44:30 | |
is far colder than that at which the air began, | 0:44:30 | 0:44:33 | |
this vast space cools down. | 0:44:33 | 0:44:37 | |
Refrigeration works because you keep moving the goalposts, | 0:44:37 | 0:44:41 | |
so that heat only ever flows from hot to cold. | 0:44:41 | 0:44:44 | |
No laws of physics are broken. | 0:44:44 | 0:44:46 | |
As long as you keep pumping a bit of energy in at the compressors, | 0:44:46 | 0:44:50 | |
the refrigerators will keep working. | 0:44:50 | 0:44:52 | |
As we saw, the process of lowering temperature requires energy... | 0:44:57 | 0:45:02 | |
..and this raises an interesting question. | 0:45:03 | 0:45:06 | |
How much colder is it possible to go? | 0:45:06 | 0:45:09 | |
We know that, as you cool materials down, | 0:45:13 | 0:45:15 | |
they tend to turn to liquid and then solids, but, actually, | 0:45:15 | 0:45:18 | |
the question of how cold you could make something | 0:45:18 | 0:45:21 | |
started with gases, | 0:45:21 | 0:45:23 | |
and this was the kind of experiment that was used. | 0:45:23 | 0:45:25 | |
What I've got here are four beakers, | 0:45:25 | 0:45:28 | |
each of which is at a different temperature. | 0:45:28 | 0:45:30 | |
They range from minus five to 50 degrees Celsius. | 0:45:32 | 0:45:36 | |
Into each, I'm placing a syringe | 0:45:36 | 0:45:39 | |
containing 15ml of air at room temperature. | 0:45:39 | 0:45:43 | |
This air will heat up or cool down | 0:45:43 | 0:45:46 | |
until it's at the same temperature as what's in the beaker. | 0:45:46 | 0:45:49 | |
So much science is about waiting, | 0:45:51 | 0:45:53 | |
and this is one of those experiments. | 0:45:53 | 0:45:55 | |
But it's not the change in temperature I'm interested in here. | 0:45:57 | 0:46:00 | |
It's something else. | 0:46:00 | 0:46:02 | |
After five minutes, the air that's heated to 50 degrees | 0:46:04 | 0:46:07 | |
has expanded from 15ml to 16ml, | 0:46:07 | 0:46:11 | |
while the air that's cooled to minus five | 0:46:11 | 0:46:14 | |
has reduced to 14ml. | 0:46:14 | 0:46:17 | |
In other words, there's a direct relationship | 0:46:17 | 0:46:20 | |
between the temperature of a gas and its volume. | 0:46:20 | 0:46:23 | |
So, the first scientists who saw this kind of relationship | 0:46:24 | 0:46:27 | |
did something very straightforward - | 0:46:27 | 0:46:29 | |
they plotted a graph that showed temperature against volume. | 0:46:29 | 0:46:33 | |
And, at the higher temperatures, the volume was higher, | 0:46:33 | 0:46:35 | |
and, as you go down to the lower and lower and lower temperatures, | 0:46:35 | 0:46:39 | |
the volume decreases. | 0:46:39 | 0:46:40 | |
And then there's a question because, at some point, | 0:46:40 | 0:46:43 | |
even though they couldn't see it, if that line kept going, | 0:46:43 | 0:46:48 | |
it was going to pass through zero volume, | 0:46:48 | 0:46:51 | |
and at that point and past that point, | 0:46:51 | 0:46:53 | |
what happens to the temperature? What does it mean? | 0:46:53 | 0:46:56 | |
And that was the first hint that there might be a limit | 0:46:56 | 0:46:59 | |
on just how cold you can go. | 0:46:59 | 0:47:01 | |
This observation led to a concept known as absolute zero - | 0:47:03 | 0:47:08 | |
the theoretical limit of cold. | 0:47:08 | 0:47:11 | |
And now we know exactly what it is. | 0:47:14 | 0:47:16 | |
On the Celsius scale, it's minus 273.15 - | 0:47:16 | 0:47:20 | |
a fantastically low temperature. | 0:47:20 | 0:47:23 | |
But, below that, there's nowhere to go. | 0:47:23 | 0:47:25 | |
That's the coldest you can get. | 0:47:25 | 0:47:26 | |
And it remains a theoretical point on the temperature scale. | 0:47:30 | 0:47:34 | |
The Boomerang Nebula 5,000 light years away from Earth | 0:47:36 | 0:47:40 | |
is the coldest place we know of in nature. | 0:47:40 | 0:47:44 | |
It's a star in the late stages of its life | 0:47:45 | 0:47:49 | |
that's shedding huge plumes of gas. | 0:47:49 | 0:47:51 | |
As this gas expands rapidly into the void of interstellar space, | 0:47:51 | 0:47:56 | |
it loses energy quickly, | 0:47:56 | 0:47:58 | |
resulting in its unusually low temperature | 0:47:58 | 0:48:01 | |
of minus 272 degrees Celsius. | 0:48:01 | 0:48:06 | |
But even this is one whole degree warmer | 0:48:06 | 0:48:09 | |
than absolute zero. | 0:48:09 | 0:48:11 | |
Though we've yet to find absolute zero | 0:48:19 | 0:48:21 | |
in the far reaches of the universe, | 0:48:21 | 0:48:24 | |
we're trying to create it ourselves much closer to home. | 0:48:24 | 0:48:28 | |
At Imperial College London, Professor Ed Hinds and his team | 0:48:28 | 0:48:32 | |
are working at the very limits of the ultracold, | 0:48:32 | 0:48:35 | |
within fractions of a degree of absolute zero. | 0:48:35 | 0:48:39 | |
It promises to open up a whole new world of physics, | 0:48:42 | 0:48:45 | |
which could revolutionise our future. | 0:48:45 | 0:48:48 | |
The stuff they're cooling here is tiny clouds of molecules. | 0:48:50 | 0:48:55 | |
Chilling them to absolute zero requires two phases of cooling. | 0:48:55 | 0:48:59 | |
First, using liquid helium, | 0:49:00 | 0:49:03 | |
they take them down to within four degrees of absolute zero. | 0:49:03 | 0:49:07 | |
But it's these last few degrees that pose the problem. | 0:49:07 | 0:49:11 | |
There are ways to make helium a bit colder, | 0:49:13 | 0:49:15 | |
but to get to the millionths of a degree, | 0:49:15 | 0:49:18 | |
there is no fluid that you can use, | 0:49:18 | 0:49:21 | |
so, instead, we use light. | 0:49:21 | 0:49:24 | |
By scattering the light, the molecules will get colder. | 0:49:26 | 0:49:31 | |
Even at this temperature, | 0:49:36 | 0:49:39 | |
the molecules still have some movement. | 0:49:39 | 0:49:43 | |
Photons in the laser light collide with the slowly moving molecules, | 0:49:43 | 0:49:48 | |
and, in that instant, | 0:49:48 | 0:49:49 | |
what little momentum they have is transferred to the photons. | 0:49:49 | 0:49:54 | |
The photons are scattered, | 0:49:54 | 0:49:57 | |
but the molecules slow down and so get even colder. | 0:49:57 | 0:50:01 | |
By using an array of different colours of laser light | 0:50:08 | 0:50:11 | |
in just the right order, | 0:50:11 | 0:50:13 | |
Ed and his team can reach temperatures | 0:50:13 | 0:50:15 | |
within a few millionths of a degree of absolute zero. | 0:50:15 | 0:50:19 | |
At these incredibly low temperatures, | 0:50:20 | 0:50:23 | |
materials begin to behave differently | 0:50:23 | 0:50:26 | |
at the subatomic or quantum level. | 0:50:26 | 0:50:28 | |
In this quantum state, they exhibit strange properties, | 0:50:28 | 0:50:33 | |
which might lead to a new type of computer. | 0:50:33 | 0:50:36 | |
A normal computer bit can only represent a zero or a one, | 0:50:36 | 0:50:41 | |
but these quantum materials can be zero and one at the same time. | 0:50:41 | 0:50:46 | |
Link these multitasking bits together, | 0:50:47 | 0:50:50 | |
and they can do vast numbers of calculations simultaneously | 0:50:50 | 0:50:54 | |
far faster than any conventional computer chip. | 0:50:54 | 0:50:58 | |
This opens up the possibility of quantum computing, | 0:51:04 | 0:51:07 | |
quantum sensing, quantum cryptography. | 0:51:07 | 0:51:10 | |
These are all ways of doing useful things, | 0:51:10 | 0:51:13 | |
but much better than can be done with conventional techniques. | 0:51:13 | 0:51:18 | |
The world of absolute zero is a strange new realm of physics | 0:51:23 | 0:51:27 | |
and one that we're only just beginning to get to grips with. | 0:51:27 | 0:51:31 | |
But there is something ironic about the vast effort required | 0:51:31 | 0:51:35 | |
to push things extremely close to absolute zero. | 0:51:35 | 0:51:39 | |
Because wait long enough - billions of years - | 0:51:41 | 0:51:45 | |
and everything will get there. | 0:51:45 | 0:51:47 | |
The universe itself is cold and it's getting colder. | 0:51:47 | 0:51:51 | |
Humans have always looked up at the sky | 0:52:10 | 0:52:12 | |
and asked questions about the stars and the structure of galaxies - | 0:52:12 | 0:52:15 | |
everything they could see. | 0:52:15 | 0:52:16 | |
But in the 1940s and '50s, a new type of question emerged | 0:52:16 | 0:52:21 | |
about what was between the stars and about what dark really was, | 0:52:21 | 0:52:25 | |
and this question opened the door on the nature of the universe. | 0:52:25 | 0:52:30 | |
And, then, in 1964, it was answered by accident. | 0:52:30 | 0:52:34 | |
In a small laboratory in New Jersey, | 0:52:37 | 0:52:39 | |
astrophysicists Robert Wilson and Arno Penzias | 0:52:39 | 0:52:43 | |
stumbled on a discovery | 0:52:43 | 0:52:45 | |
that changed our understanding of the universe forever, | 0:52:45 | 0:52:48 | |
revealing something profound about its temperature. | 0:52:48 | 0:52:51 | |
I'm meeting Professor Tim O'Brien, | 0:52:55 | 0:52:58 | |
an astrophysicist at the University of Manchester | 0:52:58 | 0:53:01 | |
and director of the Jodrell Bank Observatory. | 0:53:01 | 0:53:04 | |
So, at some point during every undergraduate physicist's degree, | 0:53:06 | 0:53:09 | |
they hear the names Penzias and Wilson. | 0:53:09 | 0:53:11 | |
Tell me what they did. | 0:53:11 | 0:53:13 | |
So, these were these two great characters | 0:53:13 | 0:53:15 | |
that were working in the USA in the 1960s, | 0:53:15 | 0:53:19 | |
and they built themselves a remarkable telescope. | 0:53:19 | 0:53:22 | |
It was incredibly well-built | 0:53:22 | 0:53:24 | |
to try and study the outer regions of the Milky Way, | 0:53:24 | 0:53:27 | |
and they were measuring very weak signals coming from space. | 0:53:27 | 0:53:31 | |
But there was this last bit of noise | 0:53:31 | 0:53:33 | |
that they had no idea where it came from. | 0:53:33 | 0:53:35 | |
They could not get rid of it. | 0:53:35 | 0:53:38 | |
It was a faint hiss, | 0:53:38 | 0:53:39 | |
and that faint hiss came from everywhere on the sky. | 0:53:39 | 0:53:42 | |
It had the same sort of strength, the same brightness | 0:53:42 | 0:53:45 | |
of the radio signal everywhere on the sky. | 0:53:45 | 0:53:46 | |
And they tried everything. | 0:53:46 | 0:53:48 | |
They tried all kinds of things, didn't they? | 0:53:48 | 0:53:49 | |
They did try everything. At one point, | 0:53:49 | 0:53:51 | |
they thought it might be coming from pigeon droppings in the telescope. | 0:53:51 | 0:53:54 | |
So, big telescope that the pigeons were sitting in. | 0:53:54 | 0:53:57 | |
Washed it all out - no, this stuff was still there. | 0:53:57 | 0:54:00 | |
There remained only one possible explanation for this noise, | 0:54:02 | 0:54:06 | |
and it had enormous implications for our view of the universe. | 0:54:06 | 0:54:10 | |
The strange hissing was coming from beyond our own galaxy. | 0:54:12 | 0:54:18 | |
It's what we now know and they didn't know at the time... | 0:54:18 | 0:54:20 | |
It's what we call the cosmic microwave background - | 0:54:20 | 0:54:22 | |
the fading glow of the Big Bang. | 0:54:22 | 0:54:24 | |
-Where was this coming from? -It's coming from the whole sky. So, it's coming from everywhere. | 0:54:24 | 0:54:28 | |
And it's actually the light that was emitted by the universe | 0:54:28 | 0:54:31 | |
about 380,000 years after the Big Bang. | 0:54:31 | 0:54:34 | |
The cosmic microwave background radiation | 0:54:39 | 0:54:42 | |
is invisible to the naked eye, but it fills the universe. | 0:54:42 | 0:54:46 | |
If we could see it, the entire sky would glow | 0:54:49 | 0:54:52 | |
with a brightness that's astonishingly uniform | 0:54:52 | 0:54:54 | |
in every direction. | 0:54:54 | 0:54:56 | |
What's remarkable is that these microwaves carry information. | 0:54:58 | 0:55:02 | |
They allow us to take an accurate temperature | 0:55:02 | 0:55:05 | |
of the entire universe without the use of a thermometer. | 0:55:05 | 0:55:09 | |
A thermometer has a fundamental limitation, | 0:55:11 | 0:55:13 | |
which is that it has to be touching the thing that it's measuring. | 0:55:13 | 0:55:16 | |
And that's not much use if you're looking at the rest of the world | 0:55:16 | 0:55:19 | |
or even the rest of the universe. | 0:55:19 | 0:55:21 | |
But the laws of physics themselves offer another route | 0:55:21 | 0:55:24 | |
because every single object in the universe with a temperature | 0:55:24 | 0:55:28 | |
is radiating some of that energy away as light, | 0:55:28 | 0:55:30 | |
and every single object has a temperature. | 0:55:30 | 0:55:33 | |
The reason you can see me now on the infrared camera | 0:55:33 | 0:55:36 | |
is that I have a temperature, and so I'm glowing in the infrared - | 0:55:36 | 0:55:39 | |
effectively, a human infrared light bulb. | 0:55:39 | 0:55:41 | |
The temperature of an object determines the exact wavelengths | 0:55:44 | 0:55:48 | |
of the light that it radiates, | 0:55:48 | 0:55:50 | |
and this means that there's a precise relationship | 0:55:50 | 0:55:53 | |
between temperature and colour. | 0:55:53 | 0:55:56 | |
So, when an astronomer sees the star of a certain colour, | 0:55:56 | 0:55:59 | |
they know it has a certain temperature. | 0:55:59 | 0:56:02 | |
The reddest star visible to the naked eye is Mu Cephei. | 0:56:04 | 0:56:08 | |
The wavelength of red light that it radiates | 0:56:08 | 0:56:11 | |
tells us that this star has a temperature | 0:56:11 | 0:56:13 | |
of around 3,200 degrees Celsius. | 0:56:13 | 0:56:17 | |
And this is Spica, | 0:56:18 | 0:56:20 | |
a star that glows a brilliant blueish-white. | 0:56:20 | 0:56:24 | |
The shorter wavelength light is indicative of a young, hot star | 0:56:24 | 0:56:28 | |
that's burning at a temperature of around 22,000 degrees Celsius. | 0:56:28 | 0:56:33 | |
And then you can go back the other way - | 0:56:35 | 0:56:37 | |
cooling down through all those very hot temperatures, | 0:56:37 | 0:56:40 | |
down through our everyday temperatures, | 0:56:40 | 0:56:42 | |
and keep going and keep going. | 0:56:42 | 0:56:44 | |
The wavelengths get longer and longer. | 0:56:44 | 0:56:46 | |
Eventually, you reach the very long wavelengths | 0:56:50 | 0:56:53 | |
of the cosmic microwave background. | 0:56:53 | 0:56:56 | |
They're not part of the visible spectrum, | 0:56:56 | 0:56:58 | |
but the wavelengths of these microwaves | 0:56:58 | 0:57:01 | |
reveal its temperature, | 0:57:01 | 0:57:03 | |
and that temperature is cold. | 0:57:03 | 0:57:06 | |
Today, the cosmic microwave | 0:57:08 | 0:57:10 | |
background radiation glows | 0:57:10 | 0:57:11 | |
at a temperature of minus 270 degrees Celsius - | 0:57:11 | 0:57:17 | |
only 2.7 degrees warmer than absolute zero. | 0:57:17 | 0:57:22 | |
We live in a nice, warm bubble on planet Earth, | 0:57:22 | 0:57:25 | |
but out there in the universe, it isn't just very empty. | 0:57:25 | 0:57:29 | |
It's very, very cold. | 0:57:29 | 0:57:32 | |
But that's not the end of our story of temperature... | 0:57:34 | 0:57:38 | |
..because amidst the vast swathes of cold and nothingness, | 0:57:40 | 0:57:45 | |
we're starting to find other bubbles of warmth | 0:57:45 | 0:57:48 | |
out there in the universe - | 0:57:48 | 0:57:50 | |
planets with a temperature similar to our own, | 0:57:50 | 0:57:53 | |
which means they may have the right conditions | 0:57:53 | 0:57:56 | |
for liquid water and complex chemistry. | 0:57:56 | 0:57:59 | |
These discoveries are causing huge excitement among scientists | 0:57:59 | 0:58:04 | |
because they offer up the tantalising possibility | 0:58:04 | 0:58:07 | |
that maybe - just maybe - | 0:58:07 | 0:58:10 | |
we might not be alone in this vast universe. | 0:58:10 | 0:58:14 | |
Next time, the temperatures of life. | 0:58:15 | 0:58:18 | |
This is an awesome force of nature. | 0:58:18 | 0:58:21 | |
I'll discover how the slenderest knife-edge of temperature | 0:58:21 | 0:58:25 | |
here on Earth provided the catalyst for life to flourish. | 0:58:25 | 0:58:30 |