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Welcome back to the Deep Dive. 
We are. 

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We're doing something a little 
specialized today and frankly, I

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think it's about time we did. 
I agree. 

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We're looking at a pretty 
fundamental pivot in how well 

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how humanity invents things, how
we create new materials. 

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It's a huge topic and our source
material for this is really 

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interesting. 
We're looking at a lecture from 

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Shiki Wang, right? 
It was delivered at the 

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University of Helsinki for 
Professor Pedro Camargo's 

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course. 
And the date on the material is 

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February 13, 2026. 
So yeah, we're getting a little 

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glimpse of the very near future.
We're basically stepping into a 

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university classroom, which is a
fun change of pace for us. 

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The title is, and it's a 
mouthful. 

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Development and application of 
computational methods on 

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catalysis research. 
Right. 

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And I know as soon as you say 
catalysis, you can almost hear 

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people's eyes glazing over. 
It sounds so, so high school 

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chemistry. 
It does, but The thing is, this 

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is actually about the engine of 
the entire modern world. 

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I mean literally everything. 
The fuel in your car, the 

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medicine you take, the plastic 
in your phone case, it all 

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exists because of catalysis. 
It's the secret ingredient that 

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makes things happen. 
Exactly. 

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And the computational part of 
that title, that's the real 

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story here. 
We are witnessing the end, or 

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maybe the beginning of the end 
of the shake and bake era of 

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chemistry. 
The shake and bake era. 

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I love that. 
That's the Edisonian method, 

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right? 
Trial and error 100. 

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I have a beaker. 
I have a hunch. 

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I mix some things together and I
just, you know, I hope nothing 

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explodes. 
Precisely. 

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And for the last, what, 200 
years? 

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That's genuinely how we found 
almost everything. 

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It's incredible to think about. 
From penicillin to Teflon, it 

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was largely based on educated 
guessing, a lot of serendipity, 

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and frankly, a whole lot of. 
Luck. 

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But Shiki Wang's lecture makes 
it painfully clear that that 

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method is, well, it's hitting a 
hard wall. 

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It is. 
It's just too slow, it's way too

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expensive and honestly all the 
low hanging fruit has already 

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been picked. 
We can't rely on luck anymore 

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and the. 
Stats and the source material to

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back this up are they're wild. 
I mean, they mentioned that 

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moving from that traditional 
trial and error to what they 

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call theory guided experiments. 
So using computers to guide you.

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Exactly that simple shift cuts 
the development process by over 

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60%. 60% just stop and think 
about what that means in 

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practice. 
It's. 

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Huge. 
If it takes, say, 10 years to 

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bring a new battery material to 
market, which is pretty 

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standard, cutting that by 60% 
means you're doing it in four 

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years. 
You're getting it six years 

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earlier. 
That's the difference between 

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maybe solving a major part of 
the climate crisis and 

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completely missing the boat. 
It's a revolutionary speed up. 

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And then there's the cost 
metric, which let's be honest, 

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is probably the real clincher 
for the industry. 

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Oh, absolutely. 
It always comes down to the 

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money. 
The lecture notes state that a 

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single calculation using DfT, 
that's density functional 

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theory, and we will get deep 
into what that is. 

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It costs roughly one one 
thousandth of the equivalent 

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experimental expense. 1000 I 
mean, that's not an incremental 

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improvement. 
No, it's a phase shift. 

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It's the difference between 
buying a house and buying a cup 

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of coffee. 
It's just not on the same 

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planet. 
And that completely changes the 

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risk profile for research, 
doesn't it? 

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How so? 
Well, if I'm running a physical 

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lab, every single experiment 
burns cash. 

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You've got the chemicals, the 
waste disposal, the equipment, 

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time, the personnel. 
The energy costs, which are 

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massive. 
Right. 

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So I have to be conservative. 
I can really only afford to test

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the things I'm pretty sure are 
going to work. 

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You stick to what you know. 
You make small changes to proven

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formulas. 
Exactly. 

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But if the cost of an experiment
drops by a factor of 1000. 

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Then you can test the crazy 
ideas. 

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You can test the things that 
shouldn't work just on the off 

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chance they do. 
You can explore the entire 

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chemical universe, as they call 
it, rather than just, you know, 

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the little neighborhood you're 
already familiar with. 

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It's like going from a map of 
your town to Google Earth. 

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That's a perfect analogy, and 
that leads us right into the 

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first big theme of this lecture,
which is just the why. 

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Why are we doing all this? 
And aside from the speed and the

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money, it's about overcoming our
own human limitations. 

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The lecture highlights 
overcoming experimental limits 

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as a primary driver. 
This is so crucial. 

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There's a fundamental resolution
problem in physical chemistry. 

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You know, we talk about atoms 
like the little Legos we can 

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move around, but in a real 
experiment, you can't just you 

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can't just look at a single atom
and watch what it does. 

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No, you're always looking at 
averages. 

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Averages of trillions upon 
trillions of atoms all doing 

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something slightly different. 
Exactly. 

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But all the interesting stuff, 
the chemistry, the reason a 

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reaction works or fails, it 
happens at the margins. 

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It happens with that one weird 
atom on the corner of a 

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nanoparticle. 
And you can't see that. 

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You can't. 
The source specifically mentions

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resolving atomic scale dynamics,
and they give the example of 

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dislocation motion. 
Now for the material scientists 

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listening, you know the 
dislocation motion is 

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everything. 
It's how metals bend instead of 

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snapping. 
It's how things fail. 

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But it. 
Happens at what? 

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The speed of sound inside a 
solid block of metal at the 

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scale of a nanometer? 
You can't exactly stick a GoPro 

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in there to see what's 
happening. 

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I really, really can't. 
But in a simulation in a 

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computer model, you're 
basically. 

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You control the universe. 
You can pause time, you can 

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rewind it, you can strip away 
the outer layers of the metal 

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and justice look at the core. 
You can see the exact moment a 

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bond breaks or a new one forms. 
That kind of visibility is 

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something no physical experiment
on Earth can ever give you. 

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And the other limitation the 
lecture brings up is the 

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environment, what they call the 
dangerous factor. 

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Right, things that are too hot, 
too high pressure or too 

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radioactive to study easily. 
And the example they use is 

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predicting irradiation damage in
nuclear reactors. 

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A classic problem, and a super 
important one if you want to 

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build a fusion reactor. 
The dream of clean energy. 

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You need to design materials 
that can withstand a constant 

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bombardment of high energy 
neutrons that would basically 

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disintegrate almost anything we 
can currently. 

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Make and you can't exactly build
a test fusion reactor just to 

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see if your new wall material 
melts. 

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Well, you can, but it costs 
billions of dollars and takes a 

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decade or more. 
Or you use computational 

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modeling. 
You build the wall inside the 

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supercomputer. 
You simulate a single neutron 

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hitting the atomic lattice. 
You calculate the energy 

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transfer. 
You watch the cascade of damage 

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as that one neutron knocks other
atoms out of place. 

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And you can fail 1000 times in 
the simulation. 

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A million times. 
And you do it without ever 

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creating a single speck of 
radioactive waste. 

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We're spending billions of 
dollars. 

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So it's safer, it sees the 
invisible, and it's 

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astronomically cheaper. 
That's a pretty compelling case.

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But then there's the 
acceleration aspect. 

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Yes, the lecture talks about 
high throughput screening. 

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This is the brute force 
approach. 

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Right. 
It is brute force, but it's 

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smart brute force. 
I mean, think about it. 

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In the old days, a PhD student 
might synthesize and 

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characterize maybe maybe one new
material a week. 

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If they were lucky and all the 
equipment was working and 

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nothing broke, right? 
And they didn't contaminate 

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their sample. 
High throughput screening is 

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more like a machine gun. 
You're not firing one bullet, 

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you're firing off thousands or 
10s of thousands of calculations

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simultaneously on a 
supercomputer cluster. 

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And the lecturer sites a 
specific MIT study that really 

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just it illustrates this 
perfectly. 

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They use this method to look for
new electrolytes for lithium ion

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batteries. 
And they didn't just find a few,

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they identified 21 promising new
candidates. 

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And these weren't just, you 
know, a 5% improvement. 

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The source says they found 
candidates that could lead to 

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100 times efficiency gains 100 
X. 

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And here's the kicker, the part 
that really matters. 

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They likely found them in parts 
of the chemical space that 

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humans were completely ignoring.
Why? 

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Because humans are biased. 
We have chemical intuition, 

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which is great, but it's also a 
blinder. 

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We tend to modify things we 
already know work. 

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We think, oh, this electrolyte 
works pretty well. 

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Let me just add a methyl group 
over here and see if it gets a 

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little better. 
You stick to your comfort zone, 

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the computer. 
The computer has no comfort 

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zone. 
It doesn't care about tradition 

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or intuition, it just 
methodically churns through all 

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the possibilities you give it. 
It looks in the weird corners of

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the periodic table that no human
would ever think to look. 

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Exactly. 
And that's where the 

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breakthroughs are hiding. 
Which leads us, I think, to the 

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biggest, most mind bending 
number in the entire fly deck. 

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The deep mind stat. 
Oh yeah, the 2.2 million 

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structure. 
It's just it's staggering. 

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Deep Mines AI, their material 
science model, predicted 2.2 

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million new stable crystal 
structures. 

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OK, put that in context for us. 
How many did we as a species 

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know about before that? 
In the entire history of 

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inorganic chemistry leading up 
to that point, humanity had 

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painstakingly identified and 
catalog maybe, maybe 50,000 

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stable inorganic crystals. 
So in one project, one AI 

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basically did what, 1000 years 
of human scientific work in an 

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afternoon? 
Essentially, yes. 

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It's a breathtaking expansion of
our knowledge. 

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Now, we have to be careful here.
Predicting a structure exists on

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a computer is not the same as 
holding in your hand. 

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There's still a lot of work to 
do to synthesize them, of 

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course, but it gives us a map 
and almost complete map of 

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what's possible. 
It turns us from explorers 

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hacking our way through the 
jungle with a machete into 

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navigators with a full blown 
GPS. 

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And this concept of inverse 
design that the lecture 

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mentions, that's the GPS, right?
That's the navigation system. 

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That's exactly traditional 
science. 

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The shake and bake method is 
direct design. 

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You have a material and you 
measure its properties to see if

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it's any good. 
Yep. 

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Does this rock conduct 
electricity? 

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No. 
OK, how about this rock? 

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No, you're just testing what you
find. 

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Inverse design completely flips 
the script. 

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It does. 
You start with the answer. 

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You go to the computer and you 
say I want a material that is 

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transparent, conducts 
electricity like a metal, is 

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flexible and cost less than $5 a
kilogram. 

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So you define the properties you
need first. 

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And the computer searches that 
massive database of 2.2 million 

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structures. 
It works backward to tell you 

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OK. 
To get those properties you need

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to make strontium, titanium and 
oxygen in this precise crystal 

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structure. 
It's the ultimate shortcut to 

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innovation. 
It's designing with intent 

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instead of by accident. 
That's the goal. 

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But let's let's get under the 
hood here, because I don't want 

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to just hype the results. 
We need to understand the tools 

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that make this possible. 
The lecture uses this wonderful 

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phrase from Newton to 
Schrodinger, which I think is a 

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great way to visualize the 
hierarchy of methods. 

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It's the scale adder, and this 
is probably the most critical 

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concept for anyone trying to get
their head around computational 

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chemistry. 
There is no single master 

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algorithm that simulates 
everything from an electron to 

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an airplane. 
It just doesn't exist. 

235
00:10:51,080 --> 00:10:54,480
Right, you can't use the same 
math to model a single electron 

236
00:10:54,480 --> 00:10:56,800
that you use to model, say, a 
bridge. 

237
00:10:56,960 --> 00:10:59,120
Exactly. 
The physics that matters changes

238
00:10:59,120 --> 00:11:01,080
depending on the size of the 
thing you're looking at and the 

239
00:11:01,080 --> 00:11:03,560
speed at which it's moving. 
The lecture breaks this down 

240
00:11:03,560 --> 00:11:06,000
into 4 main tiers. 
OK, so let's start at the 

241
00:11:06,000 --> 00:11:07,720
bottom. 
The absolute basement of 

242
00:11:07,720 --> 00:11:10,280
reality. 
Tier 1 quantum mechanical 

243
00:11:10,280 --> 00:11:12,360
methods. 
This is the electronic scale. 

244
00:11:12,480 --> 00:11:15,720
We are dealing with length 
scales of angstroms, that's .1 

245
00:11:15,720 --> 00:11:18,640
nanometers and time scales of 
femtoseconds. 

246
00:11:19,120 --> 00:11:21,600
We're talking about the behavior
of individual electrons. 

247
00:11:21,600 --> 00:11:24,600
And the boss down here, the 
governing law is Schrodinger, 

248
00:11:24,800 --> 00:11:26,440
the. 
Schrodinger equation, yeah, It's

249
00:11:26,440 --> 00:11:28,240
the fundamental equation of 
quantum mechanics. 

250
00:11:28,520 --> 00:11:30,280
It describes the wave function 
of a system. 

251
00:11:30,560 --> 00:11:34,480
And if you can solve it, you 
know literally everything there 

252
00:11:34,480 --> 00:11:37,840
is to know about that system, 
the energy, the position of 

253
00:11:37,840 --> 00:11:42,320
electrons, how it will react. 
Everything but, and this is a 

254
00:11:42,320 --> 00:11:44,760
big but, there's a catch. 
There's a huge catch. 

255
00:11:44,880 --> 00:11:46,280
It's called the Many Body 
Problem. 

256
00:11:46,800 --> 00:11:49,480
The Schrodinger equation is 
actually pretty easy to solve if

257
00:11:49,480 --> 00:11:52,120
you only have one electron and 
one proton, like a hydrogen 

258
00:11:52,120 --> 00:11:53,680
atom. 
But as soon as you have two 

259
00:11:53,680 --> 00:11:56,240
electrons. 
Even just two, like in a helium 

260
00:11:56,240 --> 00:11:59,160
atom, it becomes incredibly 
difficult because now you don't 

261
00:11:59,160 --> 00:12:01,680
just have the electrons 
attracted to the nucleus, you 

262
00:12:01,680 --> 00:12:03,720
have the two electrons 
propelling each other. 

263
00:12:04,120 --> 00:12:07,320
And as you add more and more 
electrons, the number of these 

264
00:12:07,320 --> 00:12:09,760
interactions just explodes in 
complexity. 

265
00:12:09,800 --> 00:12:13,480
So for a real material with 
trillions of electrons, it's 

266
00:12:13,840 --> 00:12:16,880
it's just not possible. 
It's mathematically practically 

267
00:12:16,920 --> 00:12:20,280
unsolvable in its pure form. 
So we have to cheat. 

268
00:12:20,600 --> 00:12:23,040
Or to be more polite, we 
approximate. 

269
00:12:23,200 --> 00:12:26,240
And this is where DfT comes in. 
Density functional theory. 

270
00:12:26,520 --> 00:12:28,320
It's all over these lecture 
slides for a reason. 

271
00:12:28,560 --> 00:12:31,880
It's the workhorse. 
It is the absolute workhorse of 

272
00:12:31,880 --> 00:12:34,360
modern computational chemistry 
and material science. 

273
00:12:34,640 --> 00:12:37,880
It won the Nobel Prize in 
Chemistry in 1998, and it 

274
00:12:37,880 --> 00:12:39,480
deserved. 
It So how does it cheat? 

275
00:12:39,600 --> 00:12:42,360
What's the trick? 
The trick is genius. 

276
00:12:42,760 --> 00:12:45,520
Instead of trying to track the 
position and momentum of every 

277
00:12:45,520 --> 00:12:48,600
single electron, which is a 
nightmare of complexity, Anybody

278
00:12:48,600 --> 00:12:51,920
problem, right, DfT says let's 
just look at the overall 

279
00:12:51,920 --> 00:12:54,880
electron density. 
OK, so instead of tracking every

280
00:12:54,880 --> 00:12:57,080
single car on the highway, 
you're just looking at the 

281
00:12:57,120 --> 00:12:59,760
overall flow of traffic. 
The traffic jam itself is a kind

282
00:12:59,760 --> 00:13:02,680
of fluid. 
That is a fantastic analogy. 

283
00:13:03,320 --> 00:13:06,760
By focusing on the density, a 
property that only depends on 

284
00:13:06,760 --> 00:13:11,320
three spatial coordinates XY and
Z, you reduce the complexity 

285
00:13:11,320 --> 00:13:14,160
from a three end dimensional 
problem where N is the number of

286
00:13:14,160 --> 00:13:16,400
electrons down to just three 
dimensions. 

287
00:13:16,400 --> 00:13:18,000
And that makes the impossible 
possible. 

288
00:13:18,040 --> 00:13:19,880
It makes it possible on a 
supercomputer. 

289
00:13:19,960 --> 00:13:23,600
The lecture lists the software 
heavyweights here, VISP, Quantum

290
00:13:23,600 --> 00:13:25,680
Espresso, Cast Step, and 
Gaussian. 

291
00:13:25,680 --> 00:13:27,840
Are they all just different 
flavors of the same thing? 

292
00:13:27,960 --> 00:13:30,000
Not quite. 
They're distinct tools for 

293
00:13:30,000 --> 00:13:33,160
different jobs. 
VSP, Quantum Espresso, and 

294
00:13:33,160 --> 00:13:35,560
Casket are typically used for 
solid-state physics. 

295
00:13:35,800 --> 00:13:39,280
So metals, semiconductors, 
crystals. 

296
00:13:39,280 --> 00:13:42,400
Exactly things that are periodic
that repeat in space. 

297
00:13:42,960 --> 00:13:46,080
They use something called plane 
waves to describe the electrons.

298
00:13:46,280 --> 00:13:49,280
Because in a metal the electrons
are delocalized. 

299
00:13:49,360 --> 00:13:52,040
They act like waves moving 
through the entire solid. 

300
00:13:52,320 --> 00:13:55,720
Whereas Gaussian is different. 
Gaussian is the undisputed king 

301
00:13:55,720 --> 00:13:57,520
of molecular and organic 
chemistry. 

302
00:13:57,520 --> 00:14:00,400
So if you're designing a new 
drug molecule, for example. 

303
00:14:00,400 --> 00:14:02,000
Right. 
It uses what are called 

304
00:14:02,120 --> 00:14:05,760
localized basis sets. 
It treats electrons as being 

305
00:14:05,760 --> 00:14:08,680
more or less attached to 
specific atoms, which is a much 

306
00:14:08,680 --> 00:14:10,600
better description for 
individual molecules. 

307
00:14:10,920 --> 00:14:12,760
So if you're designing a new 
pharmaceutical, you're probably 

308
00:14:12,760 --> 00:14:14,600
using Gaussian. 
If you're designing a new 

309
00:14:14,600 --> 00:14:17,040
battery cathode, you're probably
using VSP. 

310
00:14:17,280 --> 00:14:20,440
But even with the brilliant 
cheat that DfT uses, we still 

311
00:14:20,440 --> 00:14:22,720
have limits. 
The lecture notes say these 

312
00:14:22,720 --> 00:14:25,840
methods are usually limited to 
less than 1000 atoms. 

313
00:14:25,880 --> 00:14:29,000
And even 1000 atoms is pushing 
it for a routine calculation. 

314
00:14:29,560 --> 00:14:32,520
A standard DfT job might handle 
a few 100 atoms. 

315
00:14:33,360 --> 00:14:36,400
The problem is that the 
computational cost still scales 

316
00:14:36,400 --> 00:14:40,280
badly, usually with the cube or 
even the 4th power of the number

317
00:14:40,280 --> 00:14:42,800
of electrons. 
So if you double the size of 

318
00:14:42,800 --> 00:14:45,280
your system. 
The calculation takes 8 or 16 

319
00:14:45,280 --> 00:14:48,360
times longer to run. 
It gets expensive very, very 

320
00:14:48,360 --> 00:14:50,560
fast. 
So you can model a very accurate

321
00:14:50,560 --> 00:14:54,160
picture of the, say, the active 
site of a catalyst. 

322
00:14:54,160 --> 00:14:56,560
The most important part, Yes. 
But you can't model the whole 

323
00:14:56,560 --> 00:14:59,480
nanoparticle it sits on, let 
alone the whole reactor. 

324
00:14:59,760 --> 00:15:02,520
Not with this method. 
For that you have to climb up 

325
00:15:02,520 --> 00:15:05,240
the ladder to Tier 2 atomistic 
simulation. 

326
00:15:05,360 --> 00:15:07,680
And this is where we say goodbye
to Schrodinger and quantum 

327
00:15:07,680 --> 00:15:10,040
mechanics, and we say hello to 
good old Isaac Newton. 

328
00:15:10,680 --> 00:15:12,320
We do. 
We're in the world of classical 

329
00:15:12,320 --> 00:15:15,120
mechanics now. 
The main tool here is molecular 

330
00:15:15,120 --> 00:15:17,680
dynamics or MD. 
OK, so what's the big 

331
00:15:17,680 --> 00:15:19,120
simplification we're making 
here? 

332
00:15:19,120 --> 00:15:22,680
The big simplification is that 
we completely stop caring about 

333
00:15:22,680 --> 00:15:24,720
individual electrons. 
We just ignore them. 

334
00:15:24,720 --> 00:15:29,560
We treat the atom as a single 
hard sphere, a little ball like 

335
00:15:29,560 --> 00:15:31,640
a billiard ball. 
We're essentially dumbing the 

336
00:15:31,640 --> 00:15:33,600
system down. 
So how did the balls know how to

337
00:15:33,600 --> 00:15:36,160
interact with each other? 
We tell them we use what's 

338
00:15:36,160 --> 00:15:39,400
called a force field. 
It's basically a set a simple 

339
00:15:39,600 --> 00:15:41,200
mathematical rules. 
Like what? 

340
00:15:41,360 --> 00:15:45,280
Like if ball A and ball B get 
too close, push them apart with 

341
00:15:45,280 --> 00:15:47,280
this much force. 
If they're connected by a 

342
00:15:47,280 --> 00:15:50,080
chemical bond, treat that bond 
like a spring and pull them 

343
00:15:50,080 --> 00:15:53,080
together. 
It's all just simple springs and

344
00:15:53,080 --> 00:15:55,280
repulsions. 
And because we're not solving 

345
00:15:55,280 --> 00:15:58,600
these incredibly complex quantum
equations anymore, this must be 

346
00:15:58,600 --> 00:16:01,840
way, way faster. 
Orders of magnitude faster. 

347
00:16:01,960 --> 00:16:03,960
It's not even a comparison with 
MD. 

348
00:16:03,960 --> 00:16:07,280
You can simulate systems with 
millions or even billions of 

349
00:16:07,280 --> 00:16:09,640
atoms. 
You can watch proteins fold in 

350
00:16:09,640 --> 00:16:11,720
water. 
You can watch polymers entangled

351
00:16:11,720 --> 00:16:13,880
to form plastics. 
The lecture lists the big 

352
00:16:13,880 --> 00:16:17,480
software names here to LAMP, PS,
Gromax, Amber. 

353
00:16:17,560 --> 00:16:19,160
Right, and again, they have 
their specialties. 

354
00:16:19,480 --> 00:16:23,480
Gromax and Amber are very famous
in the biochemistry world for 

355
00:16:23,480 --> 00:16:26,840
simulating proteins in DNA. 
LAMP PS is more of a general 

356
00:16:26,840 --> 00:16:29,280
purpose tool, very powerful for 
material science. 

357
00:16:29,440 --> 00:16:30,960
There has to be a huge trade 
off. 

358
00:16:31,160 --> 00:16:34,000
If we're ignoring electrons, how
can we possibly do chemistry? 

359
00:16:34,000 --> 00:16:36,920
Chemical reactions are electrons
moving around, bonds breaking 

360
00:16:36,920 --> 00:16:38,480
and forming. 
If I just have little balls 

361
00:16:38,480 --> 00:16:40,440
connected by springs, I can't 
break the spring. 

362
00:16:40,440 --> 00:16:43,280
And that is the classic 
fundamental limitation of 

363
00:16:43,280 --> 00:16:46,520
standard classical MD. 
It is non reactive so. 

364
00:16:46,520 --> 00:16:47,960
It's great for physical 
processes. 

365
00:16:47,960 --> 00:16:51,040
Fantastic melting, boiling, 
diffusion. 

366
00:16:51,400 --> 00:16:53,720
How a material responds to being
stretched. 

367
00:16:54,400 --> 00:16:57,680
All physical things, but it's 
terrible for modeling chemical 

368
00:16:57,680 --> 00:16:59,840
reactions. 
So it can't model a fire. 

369
00:16:59,880 --> 00:17:03,680
No, but the lecture mentions a 
bridge, a clever way to get 

370
00:17:03,680 --> 00:17:06,400
around this called Reax FF. 
Reactive force fields. 

371
00:17:06,400 --> 00:17:08,560
This is a really brilliant 
hybrid method. 

372
00:17:08,800 --> 00:17:10,760
It's still a classical method at
its core. 

373
00:17:10,760 --> 00:17:14,000
It's not solving Schrodinger's 
equation, but the force field 

374
00:17:14,000 --> 00:17:16,680
itself. 
The rules for the springs is 

375
00:17:16,680 --> 00:17:19,920
much more sophisticated. 
It's been trained on a vast 

376
00:17:19,920 --> 00:17:22,560
amount of quantum data from DfT 
calculations. 

377
00:17:22,560 --> 00:17:25,160
So it learns how bonds should 
behave. 

378
00:17:25,160 --> 00:17:27,200
Exactly. 
It has a concept of bond order. 

379
00:17:27,200 --> 00:17:30,120
It knows that if you pull 2 
atoms apart, the bond between 

380
00:17:30,120 --> 00:17:32,640
them gets weaker and weaker 
until at a certain point it 

381
00:17:32,640 --> 00:17:35,360
snaps and it knows how to form 
new bonds. 

382
00:17:35,600 --> 00:17:38,080
O with Rex FF you can simulate a
fire. 

383
00:17:38,160 --> 00:17:40,320
You can. 
You can simulate combustion, or 

384
00:17:40,320 --> 00:17:43,840
an explosion, or a battery 
material degrading overtime, all

385
00:17:43,840 --> 00:17:47,000
these complex chemical events 
involving millions of atoms 

386
00:17:47,440 --> 00:17:50,080
which you could never ever hope 
to do with pure DfT. 

387
00:17:50,080 --> 00:17:52,800
It sits right in that sweet spot
between the two tiers. 

388
00:17:53,000 --> 00:17:55,840
It's an incredibly powerful tool
for bridging that gap. 

389
00:17:56,040 --> 00:17:58,400
OK, let's keep climbing. 
We're moving up the ladder to 

390
00:17:58,400 --> 00:18:01,320
Tier 3, the mesoscale. 
This is the middle ground, 

391
00:18:01,320 --> 00:18:03,320
right? 
We're zooming out again, and 

392
00:18:03,320 --> 00:18:06,320
here we start to blur the atoms 
together. 

393
00:18:06,760 --> 00:18:09,000
The main technique is called 
coarse graining. 

394
00:18:09,160 --> 00:18:11,360
It sounds like pixelating an 
image. 

395
00:18:11,640 --> 00:18:13,120
That's a great way to think 
about it. 

396
00:18:13,480 --> 00:18:17,440
Imagine you're trying to model a
cell membrane which is made of 

397
00:18:17,640 --> 00:18:21,840
millions of lipid molecules. 
You don't need to know the exact

398
00:18:21,840 --> 00:18:25,280
position of every single 
hydrogen atom on every lipid 

399
00:18:25,280 --> 00:18:27,200
tail. 
It's just too much detail, you'd

400
00:18:27,200 --> 00:18:29,720
never be able to simulate it for
long enough to see anything 

401
00:18:29,720 --> 00:18:30,920
interesting. 
Exactly. 

402
00:18:31,120 --> 00:18:34,400
So with coarse graining, you 
might say, OK, let's treat the 

403
00:18:34,400 --> 00:18:38,000
head group of a lipid as one big
bead, and we'll treat the tail 

404
00:18:38,000 --> 00:18:40,240
as two or three other beads 
connected by a string. 

405
00:18:40,640 --> 00:18:42,600
You're simplifying the 
representation. 

406
00:18:42,640 --> 00:18:44,600
Drastically. 
And by doing that you can 

407
00:18:44,600 --> 00:18:48,280
suddenly simulate much larger 
systems for much longer times. 

408
00:18:48,920 --> 00:18:51,800
Instead of nanoseconds, you can 
watch things happen over 

409
00:18:51,800 --> 00:18:53,960
microseconds or even 
milliseconds. 

410
00:18:54,480 --> 00:18:57,080
This is how people study things 
like protein folding or how 

411
00:18:57,080 --> 00:18:59,760
polymers self assemble. 
And the lecture also mentions 

412
00:18:59,760 --> 00:19:02,320
the phase field method here. 
That sounds a bit different. 

413
00:19:02,320 --> 00:19:04,280
It is. 
This is huge for metallurgy and 

414
00:19:04,280 --> 00:19:07,920
material science. 
Imagine a pool of molten metal 

415
00:19:08,000 --> 00:19:10,080
that's cooling down and starting
to solidify. 

416
00:19:10,080 --> 00:19:13,160
Crystals begin to form. 
Right, little crystals, what we 

417
00:19:13,160 --> 00:19:16,800
call grains, start to grow. 
They bump into each other and 

418
00:19:16,800 --> 00:19:19,360
form boundaries. 
The Hase field method is a 

419
00:19:19,360 --> 00:19:22,760
mathematical way to track the 
evolution of those boundaries an

420
00:19:22,760 --> 00:19:24,520
the shapes of those grains 
overtime O. 

421
00:19:24,680 --> 00:19:26,920
It's not tracking atoms at all 
anymore. 

422
00:19:27,080 --> 00:19:29,480
Not at all. 
It's tracking a continuous field

423
00:19:29,480 --> 00:19:33,360
that just tells you this region 
is solid crystal A, this region 

424
00:19:33,360 --> 00:19:36,480
is solid crystal B, and this 
region is still liquid. 

425
00:19:36,480 --> 00:19:39,000
It's another level of 
abstraction up. 

426
00:19:39,280 --> 00:19:42,520
And that leads us to the top of 
the ladder, Tier 4, the macro 

427
00:19:42,520 --> 00:19:45,480
scale or continuum methods. 
This is the world we actually 

428
00:19:45,480 --> 00:19:47,160
see and live in. 
This is engineering. 

429
00:19:47,160 --> 00:19:50,440
This is where the material 
becomes just a solid uniform 

430
00:19:50,440 --> 00:19:53,160
block with certain properties 
like strength and conductivity. 

431
00:19:53,640 --> 00:19:56,920
We use tools like the Finite 
Element Method or FEM, or 

432
00:19:56,920 --> 00:19:59,080
Computational Fluid Dynamics 
CFD. 

433
00:19:59,080 --> 00:20:02,120
This is what an aerospace 
company uses to design A wing. 

434
00:20:02,360 --> 00:20:04,760
Exactly. 
They are not simulating the 

435
00:20:04,760 --> 00:20:07,400
individual iron and aluminum 
atoms in the wing. 

436
00:20:07,600 --> 00:20:09,400
They've smeared all that detail 
out. 

437
00:20:09,720 --> 00:20:13,160
They're solving equations for 
stress, strain, heat, flow and 

438
00:20:13,160 --> 00:20:15,880
things like that. 
And for CFD it's airflow. 

439
00:20:16,160 --> 00:20:19,080
Right, they're solving the 
Navier Stokes equations for how 

440
00:20:19,080 --> 00:20:21,920
air flows over the wing. 
The software here are giants 

441
00:20:21,920 --> 00:20:25,160
like COMSOL and NSYS. 
So the ultimate goal, and I 

442
00:20:25,160 --> 00:20:28,200
think the lecture is really 
emphatic about this point, is to

443
00:20:28,200 --> 00:20:30,240
link all of these tiers 
together. 

444
00:20:30,280 --> 00:20:33,000
Yes, that's the dream. 
To take the quantum data about 

445
00:20:33,000 --> 00:20:37,040
how 2 atoms bond, feed that 
information into the force field

446
00:20:37,040 --> 00:20:40,160
for your molecular model. 
Use the results of the molecular

447
00:20:40,160 --> 00:20:43,680
model to parameterize your 
mesoscale model, and finally use

448
00:20:43,680 --> 00:20:46,360
that to tell the engineer what 
the bulk properties of the 

449
00:20:46,360 --> 00:20:48,560
bridge will be. 
That whole process is called 

450
00:20:48,560 --> 00:20:51,360
multi scale modeling. 
It is the Holy Grail of this 

451
00:20:51,360 --> 00:20:54,360
entire field. 
It's incredibly difficult to do 

452
00:20:54,360 --> 00:20:57,760
seamlessly to pass information 
between the scales without 

453
00:20:57,760 --> 00:21:00,480
losing accuracy, but it's where 
everything is headed. 

454
00:21:00,480 --> 00:21:03,240
OK, so we have the toolkit. 
We understand the latter of 

455
00:21:03,240 --> 00:21:04,960
complexity. 
Now let's apply it. 

456
00:21:05,240 --> 00:21:07,600
The lecture focuses very 
specifically on the field of 

457
00:21:07,600 --> 00:21:09,840
catalysis. 
The absolute heart of the 

458
00:21:09,840 --> 00:21:13,440
chemical industry, something 
like 90% of all chemical 

459
00:21:13,440 --> 00:21:16,640
products have seen a catalyst at
some point in their production. 

460
00:21:16,640 --> 00:21:20,400
So if you can improve catalysts,
you improve, well, everything 

461
00:21:20,440 --> 00:21:22,280
pretty much. 
And the core question the 

462
00:21:22,280 --> 00:21:26,480
lecture poses is what can 
computational methods do for 

463
00:21:26,480 --> 00:21:29,560
catalysis? 
And from what I can see, it 

464
00:21:29,560 --> 00:21:32,680
seems to boil down to 
understanding and improving 3 

465
00:21:32,680 --> 00:21:36,680
key pillars, Activity, Kinetics 
and Selectivity. 

466
00:21:36,920 --> 00:21:39,240
Right, let's break those down 
because this is where the theory

467
00:21:39,240 --> 00:21:41,080
meets the real world. 
This is where the money is made.

468
00:21:41,080 --> 00:21:42,040
Let's. 
Start with the first one 

469
00:21:42,160 --> 00:21:44,880
Activity. 
The slides say this is all about

470
00:21:44,880 --> 00:21:48,320
the active site structure. 
The active site is the specific 

471
00:21:48,320 --> 00:21:51,920
special arrangement of atoms on 
the catalyst surface where the 

472
00:21:51,920 --> 00:21:53,760
chemical reaction actually 
happens. 

473
00:21:54,280 --> 00:21:56,720
You can think of it as a 
perfectly shaped parking spot 

474
00:21:56,720 --> 00:21:59,560
for a molecule. 
If the molecule parks there, the

475
00:21:59,560 --> 00:22:01,720
reaction happens. 
If it parks anywhere else, 

476
00:22:01,720 --> 00:22:03,960
nothing happens. 
So a more active catalyst has 

477
00:22:03,960 --> 00:22:06,360
more of these special parking 
spots or better ones. 

478
00:22:06,360 --> 00:22:08,520
Exactly, and computation lets us
design them. 

479
00:22:08,880 --> 00:22:11,520
The lecture mentions heteroatom 
doping is 1 strategy. 

480
00:22:11,520 --> 00:22:14,400
OK, what is that? 
So imagine you have a surface of

481
00:22:14,400 --> 00:22:16,240
pure carbon, like a sheet of 
graphene. 

482
00:22:16,880 --> 00:22:19,840
It's pretty inert. 
The carbon atoms are all happy. 

483
00:22:19,840 --> 00:22:21,440
They don't really want to react 
with much. 

484
00:22:22,080 --> 00:22:25,480
But what if you use a computer 
to simulate kicking out one of 

485
00:22:25,480 --> 00:22:28,760
those carbon atoms and replacing
it with a nitrogen atom? 

486
00:22:29,520 --> 00:22:32,200
That's heteroatom doping. 
You're introducing an impurity 

487
00:22:32,200 --> 00:22:34,000
on. 
Purpose a strategic impurity, 

488
00:22:34,520 --> 00:22:36,960
and you've completely changed 
the electronic landscape right 

489
00:22:36,960 --> 00:22:39,040
at that spot. 
Nitrogen has a different number 

490
00:22:39,040 --> 00:22:41,360
of electrons than carbon. 
It creates a little hot spot on 

491
00:22:41,360 --> 00:22:44,240
the surface. 
Suddenly, that one spot becomes 

492
00:22:44,240 --> 00:22:48,000
incredibly attractive to, say, 
an oxygen molecule in the air. 

493
00:22:48,000 --> 00:22:49,760
It activates it it. 
Activates it. 

494
00:22:50,120 --> 00:22:53,160
The reaction can now happen at 
that site, and with computation 

495
00:22:53,280 --> 00:22:55,800
we can screen the entire 
periodic table to predict 

496
00:22:55,800 --> 00:22:58,960
exactly which element to dope 
with and precisely where to put 

497
00:22:58,960 --> 00:23:01,280
it to get the maximum possible 
activity. 

498
00:23:01,640 --> 00:23:04,000
The lecture also mentions defect
engineering. 

499
00:23:04,360 --> 00:23:07,600
I love this concept because in 
most parts of life, defects are 

500
00:23:07,600 --> 00:23:10,240
bad. 
You want a perfect diamond, a 

501
00:23:10,240 --> 00:23:13,800
flawless crystal. 
But in catalysis, perfection is 

502
00:23:13,800 --> 00:23:16,000
actually failure. 
It's so true. 

503
00:23:16,360 --> 00:23:20,240
A perfectly flat, perfectly 
ordered crystal surface is often

504
00:23:20,240 --> 00:23:23,240
a terrible catalyst. 
The atoms are all happy and 

505
00:23:23,240 --> 00:23:25,160
comfortable and have the right 
number of neighbors. 

506
00:23:25,400 --> 00:23:27,360
They are low energy. 
They don't want to bond with 

507
00:23:27,360 --> 00:23:28,920
anything else. 
So you need to break the 

508
00:23:28,920 --> 00:23:30,440
surface. 
You need to introduce 

509
00:23:30,440 --> 00:23:32,640
imperfection. 
You need to rough it up, but in 

510
00:23:32,640 --> 00:23:36,560
a very controlled way. 
You need to create steps, edges,

511
00:23:36,560 --> 00:23:39,480
corners and vacancies where 
you've plucked an atom out. 

512
00:23:39,600 --> 00:23:41,320
And why are those spots so 
active? 

513
00:23:41,840 --> 00:23:45,640
It's because the atoms at those 
defect sites have missing 

514
00:23:45,640 --> 00:23:47,600
neighbors. 
We call them low coordination 

515
00:23:47,600 --> 00:23:50,720
sites, and because they're 
missing neighbors, their 

516
00:23:50,720 --> 00:23:55,120
remaining electrons are sort of 
dangling, unsatisfied. 

517
00:23:55,320 --> 00:23:58,320
They are desperate to bond with 
something to become stable. 

518
00:23:58,440 --> 00:24:00,680
So they'll grab on to passing 
molecules. 

519
00:24:00,680 --> 00:24:02,440
You'll grab on tight and help 
them react. 

520
00:24:02,480 --> 00:24:05,280
Computers can tell us if you 
create a step edge with this 

521
00:24:05,280 --> 00:24:08,440
specific geometry and your 
nanoparticle, your reaction rate

522
00:24:08,440 --> 00:24:11,800
will increase by 1000%. 
We can design the defects. 

523
00:24:11,880 --> 00:24:14,600
OK, that's activity. 
The second pillar is kinetics. 

524
00:24:14,600 --> 00:24:16,920
This is about movement, about 
speed, right? 

525
00:24:17,320 --> 00:24:19,560
The lecture frames this as 
support architecture. 

526
00:24:20,520 --> 00:24:22,720
It doesn't matter how amazing 
your active site is if the 

527
00:24:22,720 --> 00:24:25,640
reactive molecules can't get to 
it and the product molecules 

528
00:24:25,640 --> 00:24:28,320
can't get away. 
This is a mass transport 

529
00:24:28,320 --> 00:24:30,800
problem, a diffusion problem. 
And the lecture talks about 

530
00:24:30,800 --> 00:24:34,520
designing hierarchical pores. 
This is a beautiful concept 

531
00:24:34,600 --> 00:24:36,840
borrowed from nature. 
Think about a city's road 

532
00:24:36,840 --> 00:24:39,160
network. 
You need huge highways. 

533
00:24:39,160 --> 00:24:42,920
Those are the large pores to get
a massive amount of traffic into

534
00:24:42,920 --> 00:24:45,600
the city center quickly. 
But you can't park on a highway.

535
00:24:45,600 --> 00:24:47,520
Exactly. 
So then you need the main 

536
00:24:47,520 --> 00:24:50,840
streets, the medium sized pores 
to distribute that traffic 

537
00:24:50,840 --> 00:24:54,000
throughout the neighborhoods. 
And finally, you need the little

538
00:24:54,000 --> 00:24:57,360
driveways, the small pores to 
get to the individual houses 

539
00:24:57,440 --> 00:25:00,440
which are the active sites. 
If you only had tiny driveways 

540
00:25:00,440 --> 00:25:03,000
from the countryside, you'd have
a permanent traffic jam. 

541
00:25:03,360 --> 00:25:05,400
If you only had highways, you 
could never stop. 

542
00:25:05,600 --> 00:25:07,960
Precisely. 
You need all three scales 

543
00:25:07,960 --> 00:25:10,320
working together. 
Nature does this brilliantly. 

544
00:25:10,320 --> 00:25:13,400
Look at the structure of your 
lungs or the veins in a leaf. 

545
00:25:14,200 --> 00:25:17,200
We use computations, 
specifically methods like CFD, 

546
00:25:17,560 --> 00:25:20,680
to design these hierarchical 
pore structures in catalyst 

547
00:25:20,680 --> 00:25:23,920
supports to maximize the flow of
molecules in and out. 

548
00:25:24,200 --> 00:25:27,360
So you're engineering the 
Catalyst's plumbing system? 

549
00:25:27,360 --> 00:25:28,880
You're being a civil engineer, 
yes. 

550
00:25:29,040 --> 00:25:32,160
And that brings us to the third 
pillar, selectivity. 

551
00:25:32,720 --> 00:25:35,440
This is the really subtle one, 
the one that prevents waste. 

552
00:25:36,240 --> 00:25:38,560
This is arguably the most 
important one for green 

553
00:25:38,560 --> 00:25:40,960
chemistry. 
In many complex chemical 

554
00:25:40,960 --> 00:25:44,840
reactions, you have a choice. 
Your reactive molecule A could 

555
00:25:44,840 --> 00:25:47,400
turn into product B, which is 
the valuable pharmaceutical you 

556
00:25:47,400 --> 00:25:50,920
want, or could turn into product
C, which is a useless toxic 

557
00:25:50,920 --> 00:25:52,680
sludge. 
And traditionally you just get a

558
00:25:52,680 --> 00:25:55,280
mix of both and then have to 
spend a ton of energy and money 

559
00:25:55,280 --> 00:25:57,920
separating the good stuff from 
the bad stuff later on. 

560
00:25:58,000 --> 00:26:01,320
Right Computational catalysis 
allows us to tune the reaction 

561
00:26:01,320 --> 00:26:04,280
to be more selective, to force 
it down the path we want. 

562
00:26:04,720 --> 00:26:07,280
The lecture mentions field 
effects as a powerful way to do 

563
00:26:07,280 --> 00:26:09,800
this. 
Strain electric fields, Magnetic

564
00:26:09,800 --> 00:26:11,840
fields. 
Take strain for example. 

565
00:26:12,200 --> 00:26:14,320
If you take your catalyst 
surface and you simulate 

566
00:26:14,320 --> 00:26:17,760
stretching it, literally pulling
the atoms apart by just a few 

567
00:26:17,760 --> 00:26:21,520
percent, you change the exact 
distance between the binding 

568
00:26:21,520 --> 00:26:24,840
sites on the surface. 
So maybe the molecule that leads

569
00:26:24,840 --> 00:26:28,400
to the good product, product B 
fits perfectly on that stretch 

570
00:26:28,400 --> 00:26:31,440
surface now, but the one that 
leads to the bad product, 

571
00:26:31,480 --> 00:26:34,960
product C doesn't fit anymore. 
That's exactly the idea. 

572
00:26:35,160 --> 00:26:38,240
You are physically tuning the 
lock so that only the right key 

573
00:26:38,240 --> 00:26:40,160
will fit. 
It's an incredible level of 

574
00:26:40,160 --> 00:26:42,680
control. 
Or you could apply an external 

575
00:26:42,680 --> 00:26:45,640
electric field, and the 
simulation can show you how that

576
00:26:45,640 --> 00:26:49,760
field stabilizes the transition 
state for the reaction you want,

577
00:26:49,920 --> 00:26:52,320
making it happen much faster 
than the one you don't want. 

578
00:26:52,560 --> 00:26:55,600
And the lecture also mentions 
using light photocatalysis. 

579
00:26:55,680 --> 00:26:58,280
This is a huge area, especially 
for green energy. 

580
00:26:58,560 --> 00:27:02,040
Think about splitting water into
clean hydrogen fuel using only 

581
00:27:02,040 --> 00:27:04,640
sunlight. 
The simulation can track what 

582
00:27:04,640 --> 00:27:07,200
happens when a photon of light 
hits an electron in the 

583
00:27:07,200 --> 00:27:09,600
catalyst. 
It enters an excited state. 

584
00:27:09,600 --> 00:27:11,800
And you need that excited 
electron to go to the right 

585
00:27:11,800 --> 00:27:12,960
place. 
You do. 

586
00:27:13,120 --> 00:27:16,280
Does it jump to the right place 
on the surface to drive the 

587
00:27:16,280 --> 00:27:19,400
water splitting reaction or does
it just fall back down and waste

588
00:27:19,400 --> 00:27:22,440
that energy as heat? 
We can use quantum mechanics, 

589
00:27:22,760 --> 00:27:26,600
specifically time dependent DfT,
to design materials that Channel

590
00:27:26,600 --> 00:27:29,440
that light energy exactly where 
we need it to go. 

591
00:27:29,760 --> 00:27:32,760
O We're designing the activity, 
the plumbing, and the final 

592
00:27:32,760 --> 00:27:34,320
outcome. 
It's total control. 

593
00:27:34,480 --> 00:27:38,200
In theory, yes, that's the goal.
OK, section five of our 

594
00:27:38,200 --> 00:27:41,160
discussion here brings us to 
what the lecture calls the 

595
00:27:41,160 --> 00:27:44,080
Trinity diagram. 
It's a flow chart that connects 

596
00:27:44,080 --> 00:27:47,280
insights, computations and 
guidelines specifically for the 

597
00:27:47,280 --> 00:27:49,720
task of Electro catalyst 
discovery. 

598
00:27:50,000 --> 00:27:51,640
This is basically the modern 
workflow. 

599
00:27:51,920 --> 00:27:54,680
It shows how a computational 
chemistry lab actually operates 

600
00:27:54,680 --> 00:27:56,520
day-to-day. 
It starts with insights on the 

601
00:27:56,520 --> 00:28:00,080
left, things like understanding 
the activity origin, reaction 

602
00:28:00,080 --> 00:28:04,520
mechanisms and active sites. 
So this is the human part, the 

603
00:28:04,520 --> 00:28:06,920
scientists intuition and 
existing knowledge. 

604
00:28:07,160 --> 00:28:09,320
What do we think is making this 
catalyst work? 

605
00:28:09,560 --> 00:28:12,360
Then that feeds into the middle 
box computations. 

606
00:28:12,800 --> 00:28:15,080
This is the engine this. 
Is the supercomputer doing the 

607
00:28:15,080 --> 00:28:16,600
heavy lifting? 
We've been talking about renting

608
00:28:16,600 --> 00:28:20,280
the DfT, the MD, all of it. 
And that produces the output on 

609
00:28:20,280 --> 00:28:23,640
the right guidelines for the 
experimentalist and there are 

610
00:28:23,640 --> 00:28:27,000
three types listed, rational 
design, high throughput 

611
00:28:27,000 --> 00:28:30,800
screening and machine learning. 
Right, so rational design is the

612
00:28:30,800 --> 00:28:33,680
classic approach. 
The computer tells you the 

613
00:28:33,680 --> 00:28:36,200
binding strength of oxygen is 
too strong. 

614
00:28:36,520 --> 00:28:39,680
Try adding a little bit of gold 
to your platinum catalyst to 

615
00:28:39,680 --> 00:28:42,280
weaken it. 
It's a specific logical 

616
00:28:42,280 --> 00:28:44,320
suggestion. 
High throughput screening is 

617
00:28:44,320 --> 00:28:47,320
what we talked about before, 
testing thousands of options 

618
00:28:47,320 --> 00:28:49,480
virtually to find the top 
candidates. 

619
00:28:49,480 --> 00:28:53,000
And machine learning is the new 
frontier, using AI and neural 

620
00:28:53,000 --> 00:28:56,320
networks to find patterns in the
data that a human might miss. 

621
00:28:56,680 --> 00:28:59,240
I want to focus on the battery 
application here because the 

622
00:28:59,240 --> 00:29:02,360
lecture notes mention 
computational material science 

623
00:29:02,360 --> 00:29:05,280
in the context of anodes, 
cathodes, and electrolytes. 

624
00:29:06,000 --> 00:29:09,280
Everyone listening has a lithium
ion battery in their pocket or 

625
00:29:09,280 --> 00:29:12,240
on their desk right now. 
What is the computer actually 

626
00:29:12,240 --> 00:29:14,920
calculating inside that battery?
One of the most important 

627
00:29:14,920 --> 00:29:17,320
properties it's calculating is 
the migration barrier. 

628
00:29:17,360 --> 00:29:21,600
OK, unpack that term for us. 
A battery works by moving ions, 

629
00:29:21,680 --> 00:29:24,720
in this case lithium ions, from 
one electrode to the other. 

630
00:29:25,160 --> 00:29:28,560
To do that, a lithium ion has to
hop from one empty spot in the 

631
00:29:28,560 --> 00:29:31,720
crystal lattice of the electrode
material to the next available 

632
00:29:31,720 --> 00:29:33,840
spot. 
And that hop isn't free. 

633
00:29:33,960 --> 00:29:35,680
It's not free. 
It cost a certain amount of 

634
00:29:35,680 --> 00:29:37,360
energy to squeeze through the 
other atoms. 

635
00:29:37,600 --> 00:29:39,960
That energy cost is a migration 
barrier. 

636
00:29:40,080 --> 00:29:43,800
And if that barrier, that energy
cost is too high? 

637
00:29:43,920 --> 00:29:46,920
The lithium ion moves very 
slowly, it struggles to make the

638
00:29:46,920 --> 00:29:50,160
hop and that means your battery 
takes forever to charge and 

639
00:29:50,160 --> 00:29:51,720
can't deliver power very 
quickly. 

640
00:29:51,760 --> 00:29:54,640
But if the barrier is very low. 
You get fast charging, 

641
00:29:55,040 --> 00:29:57,520
supercharging. 
The lithium ions can just glide 

642
00:29:57,520 --> 00:29:58,240
through. 
The material. 

643
00:29:58,480 --> 00:30:01,480
Computation allows us to map out
the entire energy landscape 

644
00:30:01,640 --> 00:30:04,880
inside a crystal and find the 
pathways of least resistance. 

645
00:30:04,880 --> 00:30:07,880
Yeah, we can design materials 
where the lithium just zips 

646
00:30:07,880 --> 00:30:09,400
through like it's on a slip and 
slide. 

647
00:30:09,400 --> 00:30:11,520
Amazing. 
The other term listed is 

648
00:30:11,520 --> 00:30:14,600
absorption energy. 
That's basically how sticky the 

649
00:30:14,600 --> 00:30:17,000
surface of the material is for 
the lithium ions. 

650
00:30:17,320 --> 00:30:18,920
You want the lithium to stick to
the material. 

651
00:30:18,920 --> 00:30:22,000
That's how it stores energy, but
not so much that it gets stuck 

652
00:30:22,000 --> 00:30:24,640
forever and can't leave. 
It's the Goldilocks principle 

653
00:30:24,640 --> 00:30:26,680
again. 
Not too hot, not too cold. 

654
00:30:26,760 --> 00:30:29,120
Exactly. 
And the final one here is phase 

655
00:30:29,120 --> 00:30:31,760
transformation. 
This is the swelling problem, 

656
00:30:31,760 --> 00:30:32,640
right? 
The reason? 

657
00:30:32,640 --> 00:30:34,840
Old phone batteries sometimes 
puff up. 

658
00:30:34,880 --> 00:30:36,680
That's it. 
When you shove a bunch of 

659
00:30:36,680 --> 00:30:40,400
lithium ions into a material 
like graphite or silicon, the 

660
00:30:40,400 --> 00:30:42,400
material has to expand to make 
room for them. 

661
00:30:43,000 --> 00:30:45,520
It physically changes its 
structure, its phase. 

662
00:30:45,600 --> 00:30:48,560
And that repeated swelling and 
shrinking with every charge 

663
00:30:48,560 --> 00:30:52,080
cycle causes stress. 
It causes immense stress which 

664
00:30:52,080 --> 00:30:55,320
leads to tiny cracks which grow 
overtime and actually kill the 

665
00:30:55,320 --> 00:30:57,640
battery. 
We can use simulations to 

666
00:30:57,640 --> 00:31:00,520
predict how much a material will
expand and if it's likely to 

667
00:31:00,520 --> 00:31:03,520
crack, all before we ever have 
to build a single physical 

668
00:31:03,520 --> 00:31:05,680
prototype. 
It's just incredible how much 

669
00:31:05,680 --> 00:31:09,360
violent physics is happening 
inside that little quiet black 

670
00:31:09,360 --> 00:31:12,720
brick in our phones. 
It is a dynamic and frankly a 

671
00:31:12,720 --> 00:31:16,080
pretty violent environment at 
the atomic scale, and we are 

672
00:31:16,080 --> 00:31:18,320
finally learning how to tame it 
with mathematics. 

673
00:31:18,480 --> 00:31:20,600
So let's look forward. 
We're heading into the future 

674
00:31:20,600 --> 00:31:23,040
now with Section 6, the future 
landscape. 

675
00:31:23,400 --> 00:31:28,000
The lecture actually references 
papers from 2024, 2025, which in

676
00:31:28,000 --> 00:31:31,880
the context of our 2026 source 
is the very recent past. 

677
00:31:32,160 --> 00:31:34,960
What is the cutting edge? 
The cutting edge is the 

678
00:31:34,960 --> 00:31:39,120
convergence of all these tools. 
The 2024 Advanced Materials 

679
00:31:39,120 --> 00:31:42,560
paper mentioned in the slides 
talk specifically about merging 

680
00:31:42,560 --> 00:31:45,880
first principles. 
That's our high accuracy DfT 

681
00:31:45,920 --> 00:31:48,280
with machine learning. 
And this brings us back to that 

682
00:31:48,280 --> 00:31:51,000
really important shift you 
mentioned earlier, the move from

683
00:31:51,000 --> 00:31:53,760
descriptive science to 
predictive science. 

684
00:31:53,760 --> 00:31:56,040
That is the single most 
important take away from this 

685
00:31:56,040 --> 00:31:58,800
whole discussion. 
For decades, computation and 

686
00:31:58,800 --> 00:32:00,320
chemistry was largely 
descriptive. 

687
00:32:00,600 --> 00:32:03,360
An experimentalist would run a 
reaction, something weird and 

688
00:32:03,360 --> 00:32:05,440
unexpected would happen, and 
they would go to the 

689
00:32:05,440 --> 00:32:07,640
computational chemist and ask 
them to explain it. 

690
00:32:07,680 --> 00:32:10,680
It was a post mortem. 
Why did my catalyst turn blue 

691
00:32:10,680 --> 00:32:12,320
and stop working? 
Exactly. 

692
00:32:12,360 --> 00:32:16,120
It was forensic science. 
Now we are firmly moving into 

693
00:32:16,120 --> 00:32:19,120
the predictive era. 
The computer is no longer the 

694
00:32:19,120 --> 00:32:22,440
last resort for explanation, 
it's the first step in design. 

695
00:32:23,200 --> 00:32:26,120
The computational chemist tells 
the experimentalist what to 

696
00:32:26,120 --> 00:32:30,000
build before they go into a lab.
If you put a single cobalt atom 

697
00:32:30,000 --> 00:32:33,400
right here surrounded by 4 
nitrogen atoms, it will work. 

698
00:32:33,720 --> 00:32:36,400
And the surrogate models that 
are mentioned in the lecture. 

699
00:32:36,840 --> 00:32:39,560
This is a fascinating idea. 
This is the solution to the 

700
00:32:39,560 --> 00:32:42,840
scaling problem we talked about.
You see, even though DfT is a 

701
00:32:42,840 --> 00:32:46,400
million times cheaper than an 
experiment, it's still too slow 

702
00:32:46,400 --> 00:32:50,240
to test, say, all 2.2 million of
those deep mind structures. 

703
00:32:50,240 --> 00:32:53,440
It would still take forever. 
So a surrogate model is an AI. 

704
00:32:53,680 --> 00:32:55,920
You take a few thousand of those
structures, a representative 

705
00:32:55,920 --> 00:32:59,560
sample, and you run the full 
expensive DfT calculation on 

706
00:32:59,560 --> 00:33:01,800
them. 
Then you feed all that data, the

707
00:33:01,800 --> 00:33:04,440
inputs and the outputs to a 
machine learning model. 

708
00:33:04,520 --> 00:33:08,120
So the AI learns the underlying 
laws of physics from the DfT 

709
00:33:08,120 --> 00:33:10,240
data. 
It learns an approximation of 

710
00:33:10,240 --> 00:33:12,160
the physics. 
It doesn't understand 

711
00:33:12,160 --> 00:33:14,960
Schrodinger's equation, but it 
learns the pattern. 

712
00:33:15,240 --> 00:33:18,320
It learns to recognize oh when 
the atoms are arranged in this 

713
00:33:18,320 --> 00:33:21,120
particular way, the binding 
energy is usually X. 

714
00:33:21,560 --> 00:33:25,000
And once it learns that pattern.
It can predict the properties of

715
00:33:25,080 --> 00:33:27,640
a brand new structure it's never
seen before in a matter of 

716
00:33:27,640 --> 00:33:30,520
milliseconds, instead of the 
hours or days it would take to 

717
00:33:30,520 --> 00:33:34,280
run a full DfT calculation. 
It's a virtual virtual 

718
00:33:34,280 --> 00:33:36,760
experiment, a simulation of the 
simulation. 

719
00:33:36,760 --> 00:33:40,440
You have a perfect description. 
You can use this cheap, fast 

720
00:33:40,440 --> 00:33:44,120
surrogate model to scan billions
of potential compounds in a 

721
00:33:44,120 --> 00:33:46,840
single day. 
Now it's less accurate for sure,

722
00:33:47,240 --> 00:33:50,440
but it acts as a massive filter.
To find the needles in the 

723
00:33:50,440 --> 00:33:51,480
haystack. 
Exactly. 

724
00:33:51,640 --> 00:33:54,760
You use the AI surrogate to scan
the billion options and find the

725
00:33:54,760 --> 00:33:57,400
top say 10,000 most promising 
ones. 

726
00:33:57,800 --> 00:34:00,840
Then you use the more accurate 
DfT to check those top 10,000 

727
00:34:00,840 --> 00:34:03,720
and narrow it down to the top 
100, and then you go into the 

728
00:34:03,720 --> 00:34:06,520
lab and synthesize the top 10. 
That is the funnel. 

729
00:34:06,520 --> 00:34:09,600
That is the modern pipeline for 
scientific discovery. 

730
00:34:09,639 --> 00:34:11,600
It's the future and it's 
happening right now. 

731
00:34:11,840 --> 00:34:14,639
It really makes you wonder about
the changing role of the 

732
00:34:14,639 --> 00:34:17,840
scientist in all of this. 
Let's try to synthesize this 

733
00:34:17,840 --> 00:34:22,400
deep dive now as we wrap up. 
We started with the old way, the

734
00:34:22,400 --> 00:34:27,199
slow, expensive luck based trial
and error method. 

735
00:34:27,199 --> 00:34:28,320
The shake and bake. 
Era. 

736
00:34:28,320 --> 00:34:31,440
Then we walk through the modern 
computational toolkit, the whole

737
00:34:31,440 --> 00:34:34,360
ladder from Schrodinger's 
quantum equation for electrons 

738
00:34:34,679 --> 00:34:38,639
all the way up to massive fluid 
dynamics for engineering. 

739
00:34:38,639 --> 00:34:41,960
And we saw how applying these 
tools creates better catalysts, 

740
00:34:42,080 --> 00:34:45,040
which leads to cleaner energy, 
more efficient industry, and 

741
00:34:45,040 --> 00:34:47,639
things like faster charging, 
longer lasting batteries and. 

742
00:34:47,639 --> 00:34:51,480
We ended on this incredible idea
of AI surrogates learning the 

743
00:34:51,560 --> 00:34:54,239
ways of physics to do most of 
the heavy lifting. 

744
00:34:54,239 --> 00:34:57,520
It is a complete, undenied 
paradigm shift in how we invent 

745
00:34:57,520 --> 00:34:59,240
the future. 
I want to leave our listener 

746
00:34:59,240 --> 00:35:01,200
with a final provocative thought
here. 

747
00:35:01,280 --> 00:35:05,080
The lecture mentions inverse 
design and this AI generated 

748
00:35:05,080 --> 00:35:08,680
library of 2.2 million materials
that have never existed before. 

749
00:35:08,760 --> 00:35:11,280
If we have computers that can 
predict a material that has 

750
00:35:11,280 --> 00:35:15,160
never been seen on Earth, and 
then simulate its properties 

751
00:35:15,160 --> 00:35:18,800
down to the individual electron,
and then verify that prediction 

752
00:35:18,800 --> 00:35:22,320
with a trained AI, are we 
rapidly approaching a point 

753
00:35:22,320 --> 00:35:24,480
where the lab is entirely 
digital? 

754
00:35:25,040 --> 00:35:26,480
It's a question of the century, 
isn't it? 

755
00:35:26,800 --> 00:35:29,920
If the simulation becomes 
perfect or near perfect, does 

756
00:35:29,920 --> 00:35:33,240
the physical experiment even 
matter anymore except as a final

757
00:35:33,240 --> 00:35:34,760
confirmation? 
Right. 

758
00:35:34,800 --> 00:35:37,080
I mean, if the computer model, 
which is validated against 

759
00:35:37,080 --> 00:35:39,920
decades of data says this new 
battery design will last for 

760
00:35:39,920 --> 00:35:44,040
10,000 charge cycles, do I 
really need to sit in a lab for 

761
00:35:44,040 --> 00:35:47,280
three years cycling it 10,000 
times to believe it? 

762
00:35:47,280 --> 00:35:51,480
Today, yes, you absolutely do. 
Verification is still king and 

763
00:35:51,480 --> 00:35:54,320
our models still have flaws and 
approximations. 

764
00:35:54,760 --> 00:35:57,760
But 50 years from now, when we 
have fault tolerant quantum 

765
00:35:57,760 --> 00:36:00,280
computers running these 
simulations with near perfect 

766
00:36:00,280 --> 00:36:01,640
accuracy. 
What happens then? 

767
00:36:01,800 --> 00:36:04,160
Then the physical world might 
just be from manufacturing. 

768
00:36:04,520 --> 00:36:07,200
All the discovery, all the R&D, 
might happen entirely in the 

769
00:36:07,200 --> 00:36:09,360
cloud. 
The Eureka moment moves 

770
00:36:09,360 --> 00:36:11,840
permanently from the lab bench 
to the server room. 

771
00:36:11,960 --> 00:36:13,840
For many researchers, it already
has. 

772
00:36:14,040 --> 00:36:16,920
It certainly has. 
Cheeky Wang's lecture is a clear

773
00:36:16,920 --> 00:36:20,840
road map to that future. 
It's a dense, highly technical 

774
00:36:20,840 --> 00:36:24,160
field, but the impact of this 
revolution is going to be felt 

775
00:36:24,160 --> 00:36:26,320
by every single person on the 
planet. 

776
00:36:26,320 --> 00:36:29,240
Absolutely no question. 
Thank you for joining us on this

777
00:36:29,360 --> 00:36:32,720
deep dive into the atomic scale.
Next time you plug in your phone

778
00:36:32,720 --> 00:36:35,800
to charge, just take a second to
remember there is a whole 

779
00:36:35,800 --> 00:36:38,960
universe of mathematics and 
quantum physics going on inside 

780
00:36:38,960 --> 00:36:41,600
that little battery. 
And chances are, a computer 

781
00:36:41,600 --> 00:36:44,920
choreographed that entire dance.
Thanks for listening, We'll see 

782
00:36:44,920 --> 00:36:45,600
you next time.
