0:00

Let's say I've got, uh, an atom in a liquid, and it has some freedom. It can move around, but, you know, it's very closely packed in with all of its neighboring atoms.

0:10

Let's say that it occupies some spherical volume with a radius R. Well, we can say that that R is the uncertainty in its position.

0:21

So the uncertainty in the momentum is gonna look like H-bar, Planck's constant, over R. But if it's got an uncertainty in momentum, it means it must be jiggling around inside that sphere.

0:35

We know if it's jiggling, we can say it's got an energy.

0:38

Well, we know what its momentum is. It's Planck's constant over, over R. So how do we get the energy? Well, it's easy.

0:46

We say it's the momentum squared over twice the mass.

0:50

Now, helium, being such a light atom, that mass term is very small.

0:56

So that means that the energy that it has, because it's confined, is very, very large.

1:03

Now, this is what we call the zero-point energy.

1:05

This is the energy it cannot get rid of.

1:07

It's nothing to do with thermal energy. It's not because there's a temperature in the liquid.

1:12

In fact, when you're in the liquid state, that zero-point energy accounts for more than 98% of the total energy in the fluid.

1:21

Wait, what? It is, it is enormous. That is crazy. I had no clue.

1:26

This zero-point energy is too large for the atoms ever to lock down in place, so helium never freezes just by cooling it down.

1:36

So when you're thinking of this kind of ladder of states, this kind of BEC picture, like, you know, everything's macroscopically occupying this bottom state, we think, we-- the, the intuition is to think of it as like a ladder,

1:48

where each rung is nice and evenly spaced.

1:51

But the way to think of it in terms of this zero-point energy is that that first rung is 10 stories off the floor.

End of transcript · 337 words

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