WEBVTT

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[SQUEAKING]

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[RUSTLING]

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[CLICKING]

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PROFESSOR: So the question
before in this module

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is, is there really a
linkage between nuclear power

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and nuclear proliferation?

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And it's inherently a
question about the export

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of nuclear power.

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We're not worried that the
United States might make a bomb

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from our civilian reactors.

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And most of the class
has been focused

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on domestic policy and domestic
economics for nuclear power

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here in the US.

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But it does relate to US policy
towards nuclear power because

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of several reasons.

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One is we're interested in
helping other countries reduce

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CO2.

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And nuclear power is
actually a good technology

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for some countries
that don't have access

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to cheap wind and solar.

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And second is that
if people want

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to support a nuclear
industry in the United States

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and the economics
of nuclear power

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remain as they are
today, which is to say,

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not competitive
with wind and solar,

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then the export industry
is the principal market

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for nuclear power.

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And so we then need to give some
consideration to this question

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if export is really the lifeline
for the US nuclear industry.

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So how do we think productively
about this intersection?

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How do we choose certain
technologies to invest in?

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How do we make sure that
whatever we're exporting

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isn't making the
proliferation problem worse?

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So maybe we should say, well,
why does this issue really

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arise at all?

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And maybe most of you know this,
but maybe some of you don't.

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The issue is basically that
the equipment and the materials

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in the nuclear fuel
cycle can be repurposed

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for making nuclear weapons.

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Now, just because there is
some technical connection

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doesn't mean that nuclear
power causes proliferation.

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Proliferation is a
process that entails

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both a political decision
and technical programs.

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So it's not surprising
that there is, however,

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an intersection of
these two things,

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the technical feasibility
for making nuclear weapons

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affects the political
decision to decide

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to pursue nuclear weapons.

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So if you believe
that your country just

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would have to develop all
this technology itself,

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your decision to pursue nuclear
weapons may not even come up.

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You may not consider it.

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If, however, you have all
the technology at hand,

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you might decide if
there's a security crisis,

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maybe we should be using
some of this nuclear stuff

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and build a bomb.

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And there's evidence for this.

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So Iraq, Libya, and Iran
are all countries that

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had nuclear weapons programs.

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And all of those
nuclear weapons programs

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started after they had been
offered nuclear technology

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on the black market.

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They probably, I would contend,
never have thought that they

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could have done it, except
once someone came to them--

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in this case, AQ Khan--

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said, would you like to
buy these gas centrifuges?

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Then they're like,
oh, we could do this,

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and we would have the
ability to defend ourselves.

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So the political science
professor, Matt Fuhrman,

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decided to do a big
regression, and he

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regressed over all the
civilian nuclear assistance

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agreements assigned between
1945 and the year 2000.

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And you may be
surprised that there

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are thousands of these
agreements between countries

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between that time period.

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And during that time,
there are 15 countries

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that initiated nuclear weapons
programs and a small handful

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that were finally successful,
nine depending on how you count.

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And so what did he find?

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He found that, in fact, there
are three factors that really

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correlate or predict whether
a country will acquire

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nuclear weapons-- a
slightly different result

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for start a nuclear
weapons program.

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And those that are
significant to the 1% level

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have three asterisks.

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And you see the
biggest predictors

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are have peaceful
nuclear cooperation, have

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a militarized dispute,
and GDP per capita.

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So these are correlates.

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That's all they are.

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But it kind of makes sense.

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The richest countries
in the world

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decide that we're the
leading countries.

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We ought to have
nuclear weapons--

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not to be surprised.

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Having militarized
dispute-- that makes sense.

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But the evidence also
suggests that, yeah,

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it also matters that you have
peaceful nuclear cooperation.

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So that does not
necessarily mean

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that giving a state nuclear
power will cause proliferation,

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but it does mean that
we are increasing

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the probability in the
future that some event might

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lead them to pursue weapons.

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Now, those charged
with preventing

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this political decision
will emphasize this role

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that technology seems to have,
whereas those who are advocates

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of nuclear power
will look at this

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and say, well, there are
other factors that matter.

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We just should deal
with these other factors

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and not worry about
the small effect

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that having peaceful nuclear
cooperation might have.

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Yeah?

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AUDIENCE: [INAUDIBLE]

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PROFESSOR: So the
coefficients are the-- this

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is a probit regression.

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So I believe this is the number
of standard deviations increased

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given the underlying model.

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It's pretty small
effect, I would say,

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but I have to go back
and double check that.

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I believe the result-- this is
for, I believe, acquisition.

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And I believe the
result for starting

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a program is a factor of
5, if my memory is correct.

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So you're five times more likely
to start a nuclear weapons

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program if you have civil
technology than if you don't.

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But the number of those
programs that actually succeed

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to acquiring a weapon
is actually small

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because we have a big
nonproliferation effort.

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And we'll talk about
the cost of maintaining

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that nonproliferation
effort as kind

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of an externality on the
cost of nuclear power.

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So what I'd like to try to
do is pull this apart for us

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and see if we can have a better
understanding of how this comes

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about and to give
you the data to make

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your own judgment about whether
the proliferation risk is

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a real risk or not really
a significant risk.

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Disco lights over here.

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So let's do a
thought experiment.

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Let's say you're a country
that sees itself as a rising

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power on the world stage.

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And you can imagine
a lot of countries

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might have that self-perception.

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Maybe you're already
a regional power,

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and maybe you have some
regional adversaries,

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and maybe some of
those adversaries

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have nuclear ambitions, or maybe
they even have nuclear weapons.

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And the example I want
to give is Saudi Arabia--

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a very large country,
a very wealthy country.

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It has adversaries in the
form of Israel and Iran.

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And both of those--

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Israel has nuclear
weapons, and Iran

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has had a nuclear
weapons program

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and potentially could
make nuclear weapons.

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It has an ally in Pakistan.

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Pakistan and Saudi are kind
of political sister countries.

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And they have nuclear weapons.

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And so if you're Saudi
Arabia and you're

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like, my enemies
have nuclear weapons,

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my friends have
nuclear weapons, why

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don't I have nuclear weapons?

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I'm a very rich country.

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I should have these things too.

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So imagine this
is the motivation.

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And what steps would
Saudi have to take?

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Well, first, it
would have to decide

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what kind of nuclear
weapon it wanted to build.

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So there are two principal
types that we talk about.

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One is gun type, and
one is implosion type.

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So this is the gun type.

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This is an illustration
of the Hiroshima bomb.

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And the idea is that you have
two chunks of fissile material,

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almost always highly
enriched uranium, though you

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could, in principle, do
this with uranium-233.

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And you shoot one down
a tube into the other,

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and you get a nuclear explosion.

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It's extremely simple to make.

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The design of the
Hiroshima weapon

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was so simple that we actually
never bothered to test it.

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We just dropped the
bomb on Hiroshima

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because there's just no way this
thing was not going to work.

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All of South Africa's nuclear
weapons were gun type weapons.

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You don't need any really
advanced engineering.

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You don't need to know
any hydrodynamics.

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You don't need fancy
equations of state.

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It's a very low-risk design.

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People even talked about
there's a substantial risk.

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If someone puts a chunk
of highly-enriched uranium

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on the ground and
stands on a ladder

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and drops another
chunk on top of it,

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you will also get a
nuclear explosion.

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It's really that simple to make.

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What you need, though, is
the highly-enriched uranium.

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And traditionally, so
highly-enriched uranium is

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defined as uranium
enriched to more than--

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just by definition
enriched to more than 20%.

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The Hiroshima bomb used
an average enrichment

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somewhere around 80%.

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Nowadays, if we were
to build weapons,

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we would choose something
like 93% or something

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like this because we can.

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It just makes it easier.

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Getting this is the hard part.

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And one of the readings
talks about whether,

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if we go to halo fuels that
are right at 19.75 weight

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percent, which is
19.9 atom percent,

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will this actually be
adequate for nuclear weapons?

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And there is some evidence--

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actually, we should say
substantial evidence,

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including testimony from
US weapons designers,

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that, yes, you could
make a weapon from 20%.

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So this is one of the concerns
is that you would-- even

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though it's technically
below the threshold

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of highly-enriched uranium,
from a statutory perspective,

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if we export reactors that have
large quantities of this stuff,

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we might be making
this problem worse.

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Anyway, why does it work?

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Basically, remember
that criticality

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is a geometric phenomenon.

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And as you have small chunks,
the mean-free path can be large

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compared to the
size of the chunk,

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but if we just put
two chunks together,

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then the mean-free
path will be smaller

00:12:43.270 --> 00:12:44.450 align:middle line:90%
than the size of the chunk.

00:12:44.450 --> 00:12:46.412 align:middle line:84%
And so then, on average,
more than one neutron

00:12:46.412 --> 00:12:47.870 align:middle line:84%
will stay in the
volume, and you'll

00:12:47.870 --> 00:12:50.150 align:middle line:90%
get a runaway chain reaction.

00:12:50.150 --> 00:12:53.350 align:middle line:84%
That's basically
the whole scheme.

00:12:53.350 --> 00:12:59.630 align:middle line:84%
To make a nuclear-sized
explosion, you need about 2

00:12:59.630 --> 00:13:03.870 align:middle line:84%
to the 8-- you need about
80 generations, so about 2

00:13:03.870 --> 00:13:05.770 align:middle line:90%
to the 80 fissions.

00:13:05.770 --> 00:13:07.870 align:middle line:84%
And you can just
do the calculation.

00:13:07.870 --> 00:13:12.010 align:middle line:84%
2 to the 80 fissions times
however much energy--

00:13:12.010 --> 00:13:13.930 align:middle line:84%
I forget what is the
immediate release.

00:13:13.930 --> 00:13:17.490 align:middle line:90%
Is it 180 MeV--

00:13:17.490 --> 00:13:19.470 align:middle line:84%
it's 200 MeV per
fission, but that's

00:13:19.470 --> 00:13:26.850 align:middle line:84%
if you include the energy
from delayed decay of stuff.

00:13:26.850 --> 00:13:32.990 align:middle line:84%
So I think it's 180 or ish MeV
for the prompt energy release.

00:13:32.990 --> 00:13:38.380 align:middle line:84%
And so 2 to the 80 of
those, and you have a bomb.

00:13:38.380 --> 00:13:42.540 align:middle line:84%
Now, all of that, the only
reason that is explosive

00:13:42.540 --> 00:13:46.060 align:middle line:84%
is because all of this
happens in 1 microsecond.

00:13:46.060 --> 00:13:50.660 align:middle line:84%
80 generations-- the average
time between one of these events

00:13:50.660 --> 00:13:54.340 align:middle line:90%
is about 10 nanoseconds.

00:13:54.340 --> 00:13:55.800 align:middle line:90%
That actually has a unit.

00:13:55.800 --> 00:13:58.620 align:middle line:84%
Does anyone know what
the name of the unit is?

00:13:58.620 --> 00:14:00.000 align:middle line:90%
I'm sure someone knows here.

00:14:00.000 --> 00:14:03.380 align:middle line:90%


00:14:03.380 --> 00:14:05.200 align:middle line:90%
One shake is 10 nanoseconds.

00:14:05.200 --> 00:14:07.540 align:middle line:84%
That's the fast
fission time constant.

00:14:07.540 --> 00:14:12.140 align:middle line:84%
These are the cross section is
a barn because as big as a barn,

00:14:12.140 --> 00:14:15.055 align:middle line:84%
and the time scale is
a shake because it's

00:14:15.055 --> 00:14:16.680 align:middle line:84%
as short as the shake
of a lamb's tail.

00:14:16.680 --> 00:14:20.060 align:middle line:90%
They all come from farm things.

00:14:20.060 --> 00:14:23.380 align:middle line:90%
There are other farm ones also.

00:14:23.380 --> 00:14:26.780 align:middle line:84%
It's all because the place where
we had developed nuclear weapons

00:14:26.780 --> 00:14:30.900 align:middle line:84%
was Los Alamos National Lab,
which was called The Ranch,

00:14:30.900 --> 00:14:31.630 align:middle line:90%
and so on.

00:14:31.630 --> 00:14:35.330 align:middle line:90%


00:14:35.330 --> 00:14:39.710 align:middle line:84%
Some people will say, well,
it's true that's very simple.

00:14:39.710 --> 00:14:44.170 align:middle line:84%
But these weapons are heavy,
and they're not practical

00:14:44.170 --> 00:14:46.050 align:middle line:90%
military weapons these days.

00:14:46.050 --> 00:14:48.250 align:middle line:90%
That's not true.

00:14:48.250 --> 00:14:53.490 align:middle line:90%
So here is a photo of the W33.

00:14:53.490 --> 00:14:56.570 align:middle line:84%
This is an artillery shell,
a nuclear artillery shell

00:14:56.570 --> 00:15:00.850 align:middle line:90%
that is shot out of a gun.

00:15:00.850 --> 00:15:03.370 align:middle line:84%
This thing is 8
inches in diameter.

00:15:03.370 --> 00:15:07.250 align:middle line:84%
It weighs 114 kilograms,
which is the same weight

00:15:07.250 --> 00:15:09.970 align:middle line:84%
as essentially the W80
thermonuclear warhead

00:15:09.970 --> 00:15:13.890 align:middle line:90%
that we put on our ICBMs.

00:15:13.890 --> 00:15:17.090 align:middle line:90%
And it's a gun type weapon.

00:15:17.090 --> 00:15:19.970 align:middle line:84%
Super, super basic
and simple to make.

00:15:19.970 --> 00:15:24.170 align:middle line:84%
So I'm sure there are
people in this class that

00:15:24.170 --> 00:15:29.360 align:middle line:84%
could lift this thing
and just carry it around.

00:15:29.360 --> 00:15:34.540 align:middle line:84%
So yeah, these things can
be small and very nasty.

00:15:34.540 --> 00:15:38.040 align:middle line:84%
Oh, and I should also mention
that the yield of this weapon

00:15:38.040 --> 00:15:40.580 align:middle line:90%
is, I believe--

00:15:40.580 --> 00:15:46.000 align:middle line:90%


00:15:46.000 --> 00:15:49.520 align:middle line:90%
oh, blanking on the yield.

00:15:49.520 --> 00:15:52.760 align:middle line:84%
It's much larger than
the Hiroshima weapon.

00:15:52.760 --> 00:15:55.940 align:middle line:90%
53 kilotons, maybe?

00:15:55.940 --> 00:15:57.300 align:middle line:90%
I'd have to go back and check.

00:15:57.300 --> 00:16:01.560 align:middle line:84%
We built 1,200 of
these, starting in 1956.

00:16:01.560 --> 00:16:07.000 align:middle line:84%
So yeah, gun type weapons are
still a serious consideration.

00:16:07.000 --> 00:16:10.760 align:middle line:84%
The other type of weapon
that we talk about

00:16:10.760 --> 00:16:13.120 align:middle line:90%
are these implosion weapons.

00:16:13.120 --> 00:16:16.900 align:middle line:84%
And the famous version is
that dropped on Nagasaki,

00:16:16.900 --> 00:16:18.800 align:middle line:90%
which is illustrated here.

00:16:18.800 --> 00:16:23.880 align:middle line:84%
And the idea is
that you compress

00:16:23.880 --> 00:16:28.830 align:middle line:84%
the metal core-- in this
case, you can use uranium,

00:16:28.830 --> 00:16:32.710 align:middle line:84%
but why would you bother if
you can do this with uranium?

00:16:32.710 --> 00:16:33.830 align:middle line:90%
Just do this.

00:16:33.830 --> 00:16:39.990 align:middle line:84%
So if you want to use plutonium,
it turns out plutonium releases

00:16:39.990 --> 00:16:43.490 align:middle line:84%
too many neutrons
just sitting around.

00:16:43.490 --> 00:16:45.510 align:middle line:90%
It has spontaneous fission.

00:16:45.510 --> 00:16:47.790 align:middle line:84%
And so what happens
is if you try

00:16:47.790 --> 00:16:53.550 align:middle line:84%
to do this design with
plutonium, as this bullet is

00:16:53.550 --> 00:16:58.110 align:middle line:84%
being shot down the tube,
there are neutrons flying off

00:16:58.110 --> 00:17:04.310 align:middle line:84%
of this chunk, and it begins
having a nuclear reaction

00:17:04.310 --> 00:17:07.310 align:middle line:84%
well in advance of the two
chunks coming together.

00:17:07.310 --> 00:17:12.030 align:middle line:84%
And at that point, K,
the criticality factor,

00:17:12.030 --> 00:17:13.750 align:middle line:90%
isn't high enough.

00:17:13.750 --> 00:17:15.490 align:middle line:90%
And so it starts heating up.

00:17:15.490 --> 00:17:20.030 align:middle line:84%
But what it does is it runs the
reaction kind of too slowly.

00:17:20.030 --> 00:17:23.371 align:middle line:84%
And it makes a lot of
heat, but not fast enough.

00:17:23.371 --> 00:17:24.829 align:middle line:84%
And it eventually
makes enough heat

00:17:24.829 --> 00:17:29.260 align:middle line:84%
to push the thing apart before
it runs all 80 generations.

00:17:29.260 --> 00:17:31.980 align:middle line:90%
And that is called preignition.

00:17:31.980 --> 00:17:35.600 align:middle line:84%
So they couldn't do this
design with plutonium.

00:17:35.600 --> 00:17:40.140 align:middle line:84%
And one cannot do this design
with plutonium because you

00:17:40.140 --> 00:17:43.580 align:middle line:84%
can't really shoot that using
conventional explosives.

00:17:43.580 --> 00:17:47.260 align:middle line:84%
You can't really shoot
that chunk of uranium down

00:17:47.260 --> 00:17:49.980 align:middle line:90%
the pipe fast enough.

00:17:49.980 --> 00:17:53.660 align:middle line:84%
So the idea instead was that
we would hydrodynamically

00:17:53.660 --> 00:17:56.860 align:middle line:90%
compress the plutonium.

00:17:56.860 --> 00:18:02.540 align:middle line:84%
And this was a big part of the
engineering of the Manhattan

00:18:02.540 --> 00:18:04.780 align:middle line:90%
Project.

00:18:04.780 --> 00:18:09.260 align:middle line:84%
And so what you do is you go
from the environment on the left

00:18:09.260 --> 00:18:11.260 align:middle line:90%
to the environment on the right.

00:18:11.260 --> 00:18:14.280 align:middle line:84%
And to put this as
an illustration,

00:18:14.280 --> 00:18:17.020 align:middle line:84%
now the mean-free path
is getting shorter

00:18:17.020 --> 00:18:21.400 align:middle line:84%
because the space between
the atoms is more compressed.

00:18:21.400 --> 00:18:26.610 align:middle line:84%
And so we return our
subcritical chunk

00:18:26.610 --> 00:18:30.570 align:middle line:84%
of plutonium into a
supercritical chunk

00:18:30.570 --> 00:18:33.070 align:middle line:84%
by just reducing
the mean-free path.

00:18:33.070 --> 00:18:36.810 align:middle line:90%


00:18:36.810 --> 00:18:41.050 align:middle line:84%
Most of the nuclear weapons in
the arsenals of the world today

00:18:41.050 --> 00:18:44.650 align:middle line:90%
are variations of this design.

00:18:44.650 --> 00:18:48.250 align:middle line:90%
And it is more tricky.

00:18:48.250 --> 00:18:52.050 align:middle line:84%
But also, countries have mostly
got it right the first time

00:18:52.050 --> 00:18:52.710 align:middle line:90%
they've tried.

00:18:52.710 --> 00:18:55.550 align:middle line:84%
North Korea had some trouble
with their first test,

00:18:55.550 --> 00:18:59.690 align:middle line:84%
but it looks like, by the
second test, they got it right.

00:18:59.690 --> 00:19:02.810 align:middle line:84%
But most countries are
also not confident enough

00:19:02.810 --> 00:19:05.090 align:middle line:84%
in their designs
of these weapons

00:19:05.090 --> 00:19:07.870 align:middle line:84%
to field them
without testing them.

00:19:07.870 --> 00:19:11.670 align:middle line:84%
So we tested this
design in Alamogordo.

00:19:11.670 --> 00:19:14.730 align:middle line:84%
That's the test that you see
in the movie Oppenheimer.

00:19:14.730 --> 00:19:19.050 align:middle line:84%
And most other countries have
also tested these designs.

00:19:19.050 --> 00:19:22.560 align:middle line:84%
Today, these designs
have been miniaturized

00:19:22.560 --> 00:19:26.280 align:middle line:84%
to the point where they're
basically roughly this big.

00:19:26.280 --> 00:19:28.600 align:middle line:90%
They're pretty small.

00:19:28.600 --> 00:19:32.560 align:middle line:90%
This original thing was huge.

00:19:32.560 --> 00:19:35.280 align:middle line:84%
It was about as
high as a person.

00:19:35.280 --> 00:19:36.380 align:middle line:90%
It was a big thing.

00:19:36.380 --> 00:19:39.600 align:middle line:90%


00:19:39.600 --> 00:19:42.420 align:middle line:84%
So those are the
two basic designs.

00:19:42.420 --> 00:19:43.460 align:middle line:90%
So here's Saudi Arabia.

00:19:43.460 --> 00:19:45.710 align:middle line:84%
They're going to decide which
design they want to use.

00:19:45.710 --> 00:19:50.500 align:middle line:84%
And that will in part depend
on what technologies they have.

00:19:50.500 --> 00:19:55.040 align:middle line:84%
So if they just have reactors,
reactors will make plutonium,

00:19:55.040 --> 00:19:59.680 align:middle line:84%
and they will be forced to
choose the implosion design.

00:19:59.680 --> 00:20:03.840 align:middle line:84%
But if they have access to the
other parts of the fuel cycle,

00:20:03.840 --> 00:20:08.200 align:middle line:84%
or they have thorium, then
they could potentially

00:20:08.200 --> 00:20:10.680 align:middle line:90%
do the gun type design.

00:20:10.680 --> 00:20:13.820 align:middle line:84%
Does anyone know what the
story is with thorium,

00:20:13.820 --> 00:20:16.520 align:middle line:90%
why it's a proliferation risk?

00:20:16.520 --> 00:20:18.863 align:middle line:90%
Yeah?

00:20:18.863 --> 00:20:22.953 align:middle line:84%
AUDIENCE: [INAUDIBLE]
create protactinium-233,

00:20:22.953 --> 00:20:24.370 align:middle line:84%
which you can
separate chemically,

00:20:24.370 --> 00:20:26.810 align:middle line:90%
and then you have [INAUDIBLE].

00:20:26.810 --> 00:20:28.090 align:middle line:90%
PROFESSOR: Exactly.

00:20:28.090 --> 00:20:34.390 align:middle line:84%
So it's just the same as
making plutonium from uranium.

00:20:34.390 --> 00:20:45.390 align:middle line:84%
You just you go 232
Th plus N, 233 Th--

00:20:45.390 --> 00:20:58.550 align:middle line:84%
and that decays by a beta to
233 Pa 233 U. And turns out,

00:20:58.550 --> 00:21:01.670 align:middle line:84%
uranium-233 is the
very best isotope

00:21:01.670 --> 00:21:04.910 align:middle line:84%
there is to make
a nuclear weapon.

00:21:04.910 --> 00:21:08.950 align:middle line:84%
It has a smaller critical
mass than uranium-235.

00:21:08.950 --> 00:21:13.270 align:middle line:84%
Critical mass is similar to that
of uranium-- similar to that

00:21:13.270 --> 00:21:17.620 align:middle line:84%
of plutonium, but it doesn't
have the big spontaneous neutron

00:21:17.620 --> 00:21:21.020 align:middle line:90%
background that is a problem.

00:21:21.020 --> 00:21:24.780 align:middle line:84%
In fact, there are lots and
lots of different isotopes

00:21:24.780 --> 00:21:27.600 align:middle line:84%
from which you can, in
principle, make nuclear weapons.

00:21:27.600 --> 00:21:30.820 align:middle line:90%
And here's a list of them.

00:21:30.820 --> 00:21:33.500 align:middle line:84%
So here's their
half life in kilo

00:21:33.500 --> 00:21:37.140 align:middle line:84%
years, the bare critical
mass in kilograms.

00:21:37.140 --> 00:21:39.780 align:middle line:84%
And this is the production
rate and the number

00:21:39.780 --> 00:21:43.220 align:middle line:84%
of kilograms per year per
gigawatt of electricity

00:21:43.220 --> 00:21:45.580 align:middle line:90%
that you generate.

00:21:45.580 --> 00:21:49.140 align:middle line:84%
And so we can just
look at these things.

00:21:49.140 --> 00:21:51.480 align:middle line:84%
There's only one that
is found in nature,

00:21:51.480 --> 00:21:54.400 align:middle line:90%
and that is uranium-235.

00:21:54.400 --> 00:21:57.200 align:middle line:84%
Technically, uranium-234
is also found in nature,

00:21:57.200 --> 00:22:00.700 align:middle line:90%
but it's pretty scarce.

00:22:00.700 --> 00:22:03.500 align:middle line:84%
And the bare critical
mass is pretty large,

00:22:03.500 --> 00:22:07.780 align:middle line:90%
so you would never use it.

00:22:07.780 --> 00:22:13.140 align:middle line:84%
But the other ones, we can
start eliminating some of them.

00:22:13.140 --> 00:22:15.850 align:middle line:90%
So the curium isotopes--

00:22:15.850 --> 00:22:22.250 align:middle line:84%
they're just really not produced
in any substantial quantity,

00:22:22.250 --> 00:22:25.810 align:middle line:84%
especially relative to
their critical masses.

00:22:25.810 --> 00:22:31.690 align:middle line:84%
So this is not an efficient
path to nuclear weapons.

00:22:31.690 --> 00:22:36.970 align:middle line:84%
The light uranium
isotopes, 233 synthesized

00:22:36.970 --> 00:22:39.830 align:middle line:84%
in a reactor from
uranium-235 and 238--

00:22:39.830 --> 00:22:41.570 align:middle line:90%
that's what this means.

00:22:41.570 --> 00:22:44.530 align:middle line:84%
They're basically never produced
because it's very rare that you

00:22:44.530 --> 00:22:50.730 align:middle line:84%
get those n, 2n reactions that
push the uranium isotope down

00:22:50.730 --> 00:22:52.690 align:middle line:90%
in number.

00:22:52.690 --> 00:22:57.430 align:middle line:84%
Same for neptunium-236--
just a very unlikely thing.

00:22:57.430 --> 00:23:01.130 align:middle line:90%
So we can eliminate these.

00:23:01.130 --> 00:23:05.170 align:middle line:84%
Then some of these have
obnoxiously short half-lives,

00:23:05.170 --> 00:23:10.930 align:middle line:84%
like americium,
plutonium-241, uranium-232.

00:23:10.930 --> 00:23:16.942 align:middle line:84%
And that means that they're
very hot, hard to handle.

00:23:16.942 --> 00:23:18.400 align:middle line:84%
If you try to make
a weapon, you're

00:23:18.400 --> 00:23:20.480 align:middle line:84%
going to be giving
yourself a big dose.

00:23:20.480 --> 00:23:23.200 align:middle line:84%
The people who talk about
the thorium fuel cycle

00:23:23.200 --> 00:23:29.040 align:middle line:84%
being proliferation-resistant
are talking about uranium-232.

00:23:29.040 --> 00:23:32.240 align:middle line:84%
What they're saying is
if you do this reaction,

00:23:32.240 --> 00:23:35.880 align:middle line:84%
then while this is in the
reactor, there will be an n,

00:23:35.880 --> 00:23:43.680 align:middle line:84%
2n reaction that will drive some
small fraction of this to U232.

00:23:43.680 --> 00:23:45.640 align:middle line:90%
And this is very spicy.

00:23:45.640 --> 00:23:49.240 align:middle line:84%
You can see from the
half life is very short.

00:23:49.240 --> 00:23:52.920 align:middle line:84%
But as Emil pointed
out, if we are clever,

00:23:52.920 --> 00:23:59.380 align:middle line:84%
and we separate out this before
it is turned into uranium,

00:23:59.380 --> 00:24:02.120 align:middle line:84%
so it's chemically different
and therefore chemically

00:24:02.120 --> 00:24:07.440 align:middle line:84%
discernible, we can bypass
this step and not make the 232,

00:24:07.440 --> 00:24:11.080 align:middle line:84%
let this just decay outside
of the reactor into 233.

00:24:11.080 --> 00:24:16.070 align:middle line:84%
So the thorium fuel
cycle is predicated--

00:24:16.070 --> 00:24:20.710 align:middle line:84%
is proliferation resistant only
if you have a dumb proliferator

00:24:20.710 --> 00:24:24.710 align:middle line:90%
who doesn't understand things.

00:24:24.710 --> 00:24:26.970 align:middle line:84%
This is really a
lot of noise today.

00:24:26.970 --> 00:24:32.790 align:middle line:90%


00:24:32.790 --> 00:24:37.150 align:middle line:84%
Then there are a few others
that just the critical mass

00:24:37.150 --> 00:24:39.550 align:middle line:90%
is kind of large.

00:24:39.550 --> 00:24:42.750 align:middle line:84%
These are also kind
of uninteresting.

00:24:42.750 --> 00:24:47.750 align:middle line:84%
Uranium-234-- uninteresting,
critical mass is too large.

00:24:47.750 --> 00:24:49.550 align:middle line:90%
Now what is left?

00:24:49.550 --> 00:24:52.570 align:middle line:84%
Well, uranium-235-- that's
highly enriched uranium.

00:24:52.570 --> 00:24:54.070 align:middle line:90%
We knew that.

00:24:54.070 --> 00:24:56.670 align:middle line:84%
The lower plutonium
isotopes, and

00:24:56.670 --> 00:25:00.510 align:middle line:84%
in particular, plutonium-239,
that's what we talk about.

00:25:00.510 --> 00:25:03.950 align:middle line:84%
And then one that everyone
kind of forgets about,

00:25:03.950 --> 00:25:10.140 align:middle line:84%
which is neptunium-237,
which it's not produced

00:25:10.140 --> 00:25:11.308 align:middle line:90%
in very large quantities.

00:25:11.308 --> 00:25:13.100 align:middle line:84%
If you're going to
choose one or the other,

00:25:13.100 --> 00:25:17.040 align:middle line:84%
you would choose the plutonium
because you make more of it

00:25:17.040 --> 00:25:19.720 align:middle line:90%
and you need less of it.

00:25:19.720 --> 00:25:25.100 align:middle line:90%


00:25:25.100 --> 00:25:26.980 align:middle line:90%
You need less of it.

00:25:26.980 --> 00:25:31.020 align:middle line:90%
But it's still a concern.

00:25:31.020 --> 00:25:33.580 align:middle line:84%
And there are
reprocessing programs

00:25:33.580 --> 00:25:38.020 align:middle line:84%
that have large quantities
of separated neptunium.

00:25:38.020 --> 00:25:44.220 align:middle line:84%
And it actually does not
fall under IAEA safeguards.

00:25:44.220 --> 00:25:49.280 align:middle line:84%
It's kind of a loophole
that we ought to deal with

00:25:49.280 --> 00:25:50.520 align:middle line:90%
but hasn't been dealt with.

00:25:50.520 --> 00:25:55.640 align:middle line:90%


00:25:55.640 --> 00:25:59.220 align:middle line:84%
So that's why we talk about
plutonium and uranium.

00:25:59.220 --> 00:26:03.900 align:middle line:84%
But the key takeaway here
is actually kind of subtle.

00:26:03.900 --> 00:26:07.260 align:middle line:84%
All of these things
are explosive

00:26:07.260 --> 00:26:09.850 align:middle line:90%
in the right quantities.

00:26:09.850 --> 00:26:15.170 align:middle line:84%
So if you take mostly neptune,
mostly plutonium, but then

00:26:15.170 --> 00:26:18.050 align:middle line:84%
you mix in some of
this other stuff,

00:26:18.050 --> 00:26:20.530 align:middle line:90%
it still has a critical mass.

00:26:20.530 --> 00:26:23.650 align:middle line:84%
It's some
superposition of these,

00:26:23.650 --> 00:26:26.650 align:middle line:84%
and you can still
make a bomb out of it.

00:26:26.650 --> 00:26:31.170 align:middle line:84%
You can't really
denature it and turn it

00:26:31.170 --> 00:26:34.650 align:middle line:84%
into something that
isn't usable for weapon.

00:26:34.650 --> 00:26:37.690 align:middle line:84%
All you can do is slightly
move the critical mass around

00:26:37.690 --> 00:26:40.330 align:middle line:90%
by adding some of these things.

00:26:40.330 --> 00:26:44.210 align:middle line:84%
And that's really an
important takeaway because,

00:26:44.210 --> 00:26:46.985 align:middle line:84%
a lot of times, we talk about
reactor-grade plutonium.

00:26:46.985 --> 00:26:48.610 align:middle line:84%
Some people say
reactor-grade plutonium

00:26:48.610 --> 00:26:50.250 align:middle line:90%
isn't usable for weapons.

00:26:50.250 --> 00:26:52.370 align:middle line:84%
Well, all reactor-grade
plutonium means

00:26:52.370 --> 00:26:55.010 align:middle line:84%
is it's got more of these
plutonium isotopes, these higher

00:26:55.010 --> 00:26:56.450 align:middle line:90%
plutonium isotopes.

00:26:56.450 --> 00:26:57.970 align:middle line:84%
And yeah, what it
does is it means

00:26:57.970 --> 00:27:02.130 align:middle line:84%
that it's a little bit
more spicy to deal with.

00:27:02.130 --> 00:27:06.080 align:middle line:84%
You're not having a lot of 241,
just a small amount of 241.

00:27:06.080 --> 00:27:11.360 align:middle line:84%
And it changes the
critical mass a little bit.

00:27:11.360 --> 00:27:12.420 align:middle line:90%
So you can still use it.

00:27:12.420 --> 00:27:17.840 align:middle line:84%
You just have to design the
weapon a little differently.

00:27:17.840 --> 00:27:21.120 align:middle line:90%
So that's an important takeaway.

00:27:21.120 --> 00:27:25.000 align:middle line:90%
So this is a summary.

00:27:25.000 --> 00:27:26.980 align:middle line:84%
We talked about
spontaneous neutrons,

00:27:26.980 --> 00:27:33.200 align:middle line:84%
which limits your plutonium
usage to just one design.

00:27:33.200 --> 00:27:37.960 align:middle line:84%
The amount that you need depends
on how you do the assembly.

00:27:37.960 --> 00:27:41.320 align:middle line:84%
Realistically, for
uranium, something

00:27:41.320 --> 00:27:47.320 align:middle line:84%
of the order of 15 to 20
kilograms of uranium-235

00:27:47.320 --> 00:27:52.440 align:middle line:84%
or 3 to 8 kilograms
of plutonium.

00:27:52.440 --> 00:27:57.960 align:middle line:84%
Now the IAEA has
an official number

00:27:57.960 --> 00:28:03.400 align:middle line:84%
for the amount that they deem
to be a notional nuclear weapon.

00:28:03.400 --> 00:28:06.890 align:middle line:84%
If you ask them today if it's
a notional nuclear weapon,

00:28:06.890 --> 00:28:08.730 align:middle line:84%
some people there
will say it's not,

00:28:08.730 --> 00:28:11.890 align:middle line:84%
but it absolutely is and
was when it was developed.

00:28:11.890 --> 00:28:13.550 align:middle line:84%
And you have the
historical documents

00:28:13.550 --> 00:28:16.547 align:middle line:90%
that show this very clearly.

00:28:16.547 --> 00:28:18.630 align:middle line:84%
And these are the numbers
that they came up with--

00:28:18.630 --> 00:28:21.150 align:middle line:90%
25 kilograms and 8 kilograms.

00:28:21.150 --> 00:28:24.922 align:middle line:84%
And this is what they want
to make sure is not diverted.

00:28:24.922 --> 00:28:26.630 align:middle line:84%
And you might look at
this and say, well,

00:28:26.630 --> 00:28:29.830 align:middle line:84%
if you only need
3 kilograms, why

00:28:29.830 --> 00:28:34.030 align:middle line:84%
are they saying the minimum
acceptable quantity is 8?

00:28:34.030 --> 00:28:36.870 align:middle line:84%
And yeah, people have
worried about that.

00:28:36.870 --> 00:28:40.310 align:middle line:84%
And their historical
answer was, well,

00:28:40.310 --> 00:28:42.290 align:middle line:84%
if you're in an advanced
state, you need 3.

00:28:42.290 --> 00:28:45.670 align:middle line:84%
But if you're not in
an advanced state,

00:28:45.670 --> 00:28:48.990 align:middle line:84%
you don't have a lot of
knowledge, you might need 8.

00:28:48.990 --> 00:28:52.270 align:middle line:84%
And also, there will
be some process losses

00:28:52.270 --> 00:28:56.790 align:middle line:84%
from the casting process of
making the plutonium pit and so

00:28:56.790 --> 00:28:57.470 align:middle line:90%
on.

00:28:57.470 --> 00:29:00.510 align:middle line:84%
And yeah, these are
all true statements,

00:29:00.510 --> 00:29:02.380 align:middle line:84%
but the real
motivation turned out

00:29:02.380 --> 00:29:07.140 align:middle line:84%
to be that they couldn't
do their accounting better

00:29:07.140 --> 00:29:08.800 align:middle line:90%
than these levels.

00:29:08.800 --> 00:29:12.100 align:middle line:84%
That was essentially if you
try to push down these numbers,

00:29:12.100 --> 00:29:14.100 align:middle line:84%
it just gets too expensive
to do the accounting,

00:29:14.100 --> 00:29:16.880 align:middle line:84%
and it becomes more than
their budget will support.

00:29:16.880 --> 00:29:19.580 align:middle line:84%
In fact, they already
can't do the accounting

00:29:19.580 --> 00:29:22.820 align:middle line:90%
for all the programs that exist.

00:29:22.820 --> 00:29:25.620 align:middle line:84%
And so what they do is
they say, well, we'll

00:29:25.620 --> 00:29:27.820 align:middle line:84%
discern based on
other information

00:29:27.820 --> 00:29:30.500 align:middle line:84%
other than the accounting
of fissile materials

00:29:30.500 --> 00:29:34.420 align:middle line:84%
that, for certain countries,
we don't really need to check.

00:29:34.420 --> 00:29:37.720 align:middle line:84%
Which is a reasonable
statement to make,

00:29:37.720 --> 00:29:40.040 align:middle line:84%
but it doesn't treat
everyone the same.

00:29:40.040 --> 00:29:49.100 align:middle line:90%


00:29:49.100 --> 00:29:52.900 align:middle line:90%
What else can I say here?

00:29:52.900 --> 00:29:54.900 align:middle line:84%
So just in case you're
wondering how much

00:29:54.900 --> 00:29:58.140 align:middle line:84%
8 kilograms of
plutonium is, there's

00:29:58.140 --> 00:30:01.870 align:middle line:84%
a photo of the
equivalent amount.

00:30:01.870 --> 00:30:04.690 align:middle line:90%


00:30:04.690 --> 00:30:05.790 align:middle line:90%
Yeah, that much.

00:30:05.790 --> 00:30:07.170 align:middle line:90%
It's heavy, though.

00:30:07.170 --> 00:30:10.130 align:middle line:90%


00:30:10.130 --> 00:30:12.450 align:middle line:90%
It's dense stuff.

00:30:12.450 --> 00:30:16.730 align:middle line:84%
So here's where we start having
the technical connections

00:30:16.730 --> 00:30:19.370 align:middle line:90%
to nuclear power.

00:30:19.370 --> 00:30:22.810 align:middle line:84%
Ideally, we want to use
nuclear power to mitigate

00:30:22.810 --> 00:30:24.110 align:middle line:90%
the effect of climate.

00:30:24.110 --> 00:30:26.450 align:middle line:84%
But we don't want to make
this problem any worse.

00:30:26.450 --> 00:30:30.770 align:middle line:84%
We don't want people diverting
plutonium from the fuel cycle,

00:30:30.770 --> 00:30:32.205 align:middle line:90%
from the reactor spent fuel.

00:30:32.205 --> 00:30:34.830 align:middle line:84%
We don't want people using the
enrichment process to make fuel,

00:30:34.830 --> 00:30:37.650 align:middle line:90%
to make highly enriched uranium.

00:30:37.650 --> 00:30:40.690 align:middle line:84%
And it turns out, as
I've kind of just shown

00:30:40.690 --> 00:30:44.070 align:middle line:84%
that, making the weapons
themselves are, in a way,

00:30:44.070 --> 00:30:45.670 align:middle line:90%
not all that complicated.

00:30:45.670 --> 00:30:47.550 align:middle line:90%
We did this in 1945.

00:30:47.550 --> 00:30:49.692 align:middle line:84%
North Korea has done
this successfully.

00:30:49.692 --> 00:30:51.650 align:middle line:84%
The hard part is actually
getting the plutonium

00:30:51.650 --> 00:30:53.530 align:middle line:84%
or getting the highly
enriched uranium.

00:30:53.530 --> 00:30:58.160 align:middle line:84%
And that's where various
stages of the fuel cycle

00:30:58.160 --> 00:30:59.680 align:middle line:90%
really come into play.

00:30:59.680 --> 00:31:04.400 align:middle line:84%
So the once through fuel cycle
is what we mostly talk about.

00:31:04.400 --> 00:31:07.880 align:middle line:84%
And that's what we have
in the United States.

00:31:07.880 --> 00:31:10.060 align:middle line:84%
We put the uranium in
the plant, we burn it,

00:31:10.060 --> 00:31:13.600 align:middle line:84%
and then we just put the spent
fuel in pool and call it a day.

00:31:13.600 --> 00:31:18.880 align:middle line:84%
And the nice thing about
that is, at no point is there

00:31:18.880 --> 00:31:25.260 align:middle line:84%
any material in the fuel cycle
that is directly weapons usable.

00:31:25.260 --> 00:31:28.440 align:middle line:84%
So the uranium that comes
out of the enrichment plant

00:31:28.440 --> 00:31:30.840 align:middle line:90%
is something like up to 5%--

00:31:30.840 --> 00:31:32.640 align:middle line:90%
too low to make a bomb.

00:31:32.640 --> 00:31:35.500 align:middle line:84%
Then you burn the
fuel in the reactor.

00:31:35.500 --> 00:31:38.260 align:middle line:84%
And yes, there is plutonium
in that spent fuel.

00:31:38.260 --> 00:31:41.540 align:middle line:84%
But remember, it's got all those
other fission products in there.

00:31:41.540 --> 00:31:44.152 align:middle line:84%
And so it's kind
of self protecting.

00:31:44.152 --> 00:31:45.860 align:middle line:84%
And you would need to
do that separation.

00:31:45.860 --> 00:31:49.320 align:middle line:84%
And so you would have to
build a reprocessing plant

00:31:49.320 --> 00:31:52.520 align:middle line:84%
to get your plutonium
for the weapon.

00:31:52.520 --> 00:31:58.190 align:middle line:84%
And as long as countries don't
build reprocessing plants,

00:31:58.190 --> 00:32:01.470 align:middle line:84%
they will not possess all
of the technology needed

00:32:01.470 --> 00:32:05.870 align:middle line:84%
to convert nuclear power into
a nuclear weapons program,

00:32:05.870 --> 00:32:10.510 align:middle line:84%
and that has been the
foundation of nonproliferation

00:32:10.510 --> 00:32:12.910 align:middle line:84%
since the Ford
administration, which

00:32:12.910 --> 00:32:15.730 align:middle line:84%
we said we will not reprocess
here in the United States,

00:32:15.730 --> 00:32:17.230 align:middle line:84%
and we will not
support other people

00:32:17.230 --> 00:32:22.030 align:middle line:84%
reprocessing because we
don't want this plant

00:32:22.030 --> 00:32:25.150 align:middle line:84%
to exist in any
country that might

00:32:25.150 --> 00:32:29.030 align:middle line:84%
convert their civil program
into a weapons program.

00:32:29.030 --> 00:32:31.550 align:middle line:84%
The problem arises when these
fast reactor people show up

00:32:31.550 --> 00:32:34.750 align:middle line:84%
and say, well, we want to do
this as a matter of course

00:32:34.750 --> 00:32:37.540 align:middle line:84%
or when the nuclear waste
people show up and are like,

00:32:37.540 --> 00:32:39.290 align:middle line:84%
we don't know where
to put our spent fuel.

00:32:39.290 --> 00:32:41.630 align:middle line:84%
Therefore, let's just
do some reprocessing

00:32:41.630 --> 00:32:43.895 align:middle line:84%
to kick the can down
the road and delay

00:32:43.895 --> 00:32:45.270 align:middle line:84%
the decision of
where we're going

00:32:45.270 --> 00:32:48.230 align:middle line:84%
to put our geologic
repository, like Japan.

00:32:48.230 --> 00:32:51.550 align:middle line:84%
And so now you have the
French and the Japanese

00:32:51.550 --> 00:32:56.020 align:middle line:84%
doing this thing with separation
plutonium as a matter of course.

00:32:56.020 --> 00:32:59.700 align:middle line:84%
And that gives us
this dedicated pathway

00:32:59.700 --> 00:33:03.660 align:middle line:84%
in which you don't need any
additional facilities to get

00:33:03.660 --> 00:33:06.020 align:middle line:90%
to a bomb.

00:33:06.020 --> 00:33:10.622 align:middle line:84%
The other concern--
this is the connection

00:33:10.622 --> 00:33:12.080 align:middle line:84%
to the civilian
nuclear fuel cycle.

00:33:12.080 --> 00:33:14.500 align:middle line:84%
But we should remember
that most countries that

00:33:14.500 --> 00:33:17.540 align:middle line:84%
have nuclear weapons
have dedicated

00:33:17.540 --> 00:33:20.300 align:middle line:84%
nuclear weapons
production reactors

00:33:20.300 --> 00:33:27.360 align:middle line:84%
that most countries have not
used these civilian-- now,

00:33:27.360 --> 00:33:30.340 align:middle line:84%
it's not true that no country
has contemplated this.

00:33:30.340 --> 00:33:33.720 align:middle line:84%
But this is how the United
States did it, for example.

00:33:33.720 --> 00:33:37.660 align:middle line:84%
So what's to stop
a country like Iran

00:33:37.660 --> 00:33:42.020 align:middle line:84%
building a dedicated
plutonium production reactor?

00:33:42.020 --> 00:33:42.680 align:middle line:90%
They had one.

00:33:42.680 --> 00:33:44.940 align:middle line:90%
It was called Arak.

00:33:44.940 --> 00:33:48.060 align:middle line:84%
And they could just
do this on their own

00:33:48.060 --> 00:33:49.860 align:middle line:90%
without civilian nuclear power.

00:33:49.860 --> 00:33:51.440 align:middle line:90%
So this is the counterargument.

00:33:51.440 --> 00:33:54.490 align:middle line:90%
Well, they can just do this.

00:33:54.490 --> 00:33:55.790 align:middle line:90%
Why don't they do that?

00:33:55.790 --> 00:33:58.730 align:middle line:84%
And then the second
thing is they could also

00:33:58.730 --> 00:34:01.930 align:middle line:84%
just build a dedicated
enrichment plant

00:34:01.930 --> 00:34:04.690 align:middle line:84%
to enrich uranium
and make a bomb.

00:34:04.690 --> 00:34:07.410 align:middle line:84%
And so again, this is
the other counterargument

00:34:07.410 --> 00:34:09.969 align:middle line:90%
against a connection.

00:34:09.969 --> 00:34:15.050 align:middle line:84%
So let's look at these
a little bit more.

00:34:15.050 --> 00:34:19.610 align:middle line:84%
So who has actually done this
plutonium from power reactors?

00:34:19.610 --> 00:34:21.850 align:middle line:84%
Two countries, France
and the United Kingdom,

00:34:21.850 --> 00:34:26.489 align:middle line:84%
both made weapons using
their power reactors.

00:34:26.489 --> 00:34:28.610 align:middle line:90%
So yeah, it has been done.

00:34:28.610 --> 00:34:32.170 align:middle line:84%
Argentina, Brazil,
Sweden, and Taiwan

00:34:32.170 --> 00:34:34.770 align:middle line:84%
all had programs where
this was the plan.

00:34:34.770 --> 00:34:38.570 align:middle line:84%
They would just divert fuel
from their power program

00:34:38.570 --> 00:34:40.210 align:middle line:90%
and build a bomb.

00:34:40.210 --> 00:34:43.389 align:middle line:84%
And any country that has a
power reactor can do this.

00:34:43.389 --> 00:34:47.250 align:middle line:90%


00:34:47.250 --> 00:34:50.480 align:middle line:84%
The Argentine and
Brazilian programs

00:34:50.480 --> 00:34:53.260 align:middle line:84%
were operated under
military governments.

00:34:53.260 --> 00:34:57.520 align:middle line:84%
Those governments collapsed
before they were successful.

00:34:57.520 --> 00:35:01.800 align:middle line:84%
The Swedish program has
an interesting story.

00:35:01.800 --> 00:35:05.480 align:middle line:84%
They designed their nuclear
power program from the beginning

00:35:05.480 --> 00:35:07.720 align:middle line:90%
to be dual use.

00:35:07.720 --> 00:35:11.620 align:middle line:84%
Then the cost started
getting out of control,

00:35:11.620 --> 00:35:15.560 align:middle line:84%
and there was a lot of domestic
opposition to nuclear power

00:35:15.560 --> 00:35:18.000 align:middle line:90%
that was becoming a problem.

00:35:18.000 --> 00:35:20.600 align:middle line:84%
But, of course, they
had this hidden agenda

00:35:20.600 --> 00:35:22.700 align:middle line:84%
of making nuclear
weapons with the program.

00:35:22.700 --> 00:35:24.800 align:middle line:84%
So they were kind of
trying to advance it.

00:35:24.800 --> 00:35:28.103 align:middle line:84%
And then the United States
realized what was happening.

00:35:28.103 --> 00:35:29.853 align:middle line:84%
And the United States
swooped in and said,

00:35:29.853 --> 00:35:32.800 align:middle line:84%
you know what, Sweden, if
you abandoned the reactors

00:35:32.800 --> 00:35:34.880 align:middle line:84%
that you've designed
for your program

00:35:34.880 --> 00:35:39.040 align:middle line:84%
and instead accept light water
reactor once-through fuel

00:35:39.040 --> 00:35:45.760 align:middle line:84%
cycle from us, then we'll
give you some discounts.

00:35:45.760 --> 00:35:50.350 align:middle line:84%
Then we'll make your domestic
political problem go away.

00:35:50.350 --> 00:35:54.030 align:middle line:84%
And so they finally gave
up their weapons ambitions.

00:35:54.030 --> 00:35:56.450 align:middle line:84%
And Taiwan also
tried to do this,

00:35:56.450 --> 00:35:59.830 align:middle line:84%
and the United States found out
and went to Taiwan and said,

00:35:59.830 --> 00:36:03.030 align:middle line:84%
you know what, if
you don't stop this,

00:36:03.030 --> 00:36:05.470 align:middle line:84%
we're not going to defend
you against Mainland China.

00:36:05.470 --> 00:36:09.150 align:middle line:90%
And they went, OK, sorry.

00:36:09.150 --> 00:36:14.750 align:middle line:84%
So nonproliferation
has been successful

00:36:14.750 --> 00:36:15.850 align:middle line:90%
in two of these cases.

00:36:15.850 --> 00:36:21.310 align:middle line:84%
And two of these cases
imploded on their own accord.

00:36:21.310 --> 00:36:24.010 align:middle line:84%
In case you're wondering
which reactors at France--

00:36:24.010 --> 00:36:31.950 align:middle line:84%
this is the G2 and G3 reactor
at Marcoule that they used.

00:36:31.950 --> 00:36:33.450 align:middle line:90%
We all know how that works.

00:36:33.450 --> 00:36:37.010 align:middle line:90%


00:36:37.010 --> 00:36:39.890 align:middle line:90%
So here's how you do it.

00:36:39.890 --> 00:36:43.790 align:middle line:84%
As I showed you earlier,
you can use any combination

00:36:43.790 --> 00:36:47.220 align:middle line:84%
of those isotopes to come
up with a combination that

00:36:47.220 --> 00:36:51.020 align:middle line:90%
is useful for nuclear weapons.

00:36:51.020 --> 00:36:55.380 align:middle line:84%
But typically, you
ideally don't want

00:36:55.380 --> 00:36:59.220 align:middle line:84%
to have a lot of these
isotopes, especially

00:36:59.220 --> 00:37:00.940 align:middle line:84%
these even numbered
isotopes, which

00:37:00.940 --> 00:37:05.100 align:middle line:84%
tend to have higher
spontaneous fission rates.

00:37:05.100 --> 00:37:10.000 align:middle line:84%
So you would ideally not want
to burn your fuel normally.

00:37:10.000 --> 00:37:12.380 align:middle line:84%
We talk about burning fuel
all the way up to, nowadays,

00:37:12.380 --> 00:37:16.040 align:middle line:84%
45,000-50,000 megawatt
days per metric ton.

00:37:16.040 --> 00:37:18.460 align:middle line:84%
So we're really over
here these days.

00:37:18.460 --> 00:37:22.620 align:middle line:84%
And so the plutonium
is not great.

00:37:22.620 --> 00:37:24.600 align:middle line:84%
It has a lot of
these other isotopes.

00:37:24.600 --> 00:37:28.420 align:middle line:84%
Ideally, we want just
pure plutonium-239.

00:37:28.420 --> 00:37:33.300 align:middle line:84%
But if you pull out
the uranium early,

00:37:33.300 --> 00:37:36.780 align:middle line:90%
you get weapons-grade stuff.

00:37:36.780 --> 00:37:40.980 align:middle line:90%
And so two ways you can do this.

00:37:40.980 --> 00:37:46.010 align:middle line:84%
One is you could just
stop the reactor.

00:37:46.010 --> 00:37:47.730 align:middle line:84%
Now maybe people
will be watching.

00:37:47.730 --> 00:37:50.170 align:middle line:84%
Oh, why did that
reactor shut down?

00:37:50.170 --> 00:37:52.510 align:middle line:84%
And why are they unloading
the fuel from that reactor?

00:37:52.510 --> 00:37:56.570 align:middle line:84%
And so you might be tipping your
hand as to what you're up to.

00:37:56.570 --> 00:37:59.690 align:middle line:84%
On the other hand, maybe
you have a problem.

00:37:59.690 --> 00:38:03.250 align:middle line:90%
Oh, a reactor had a leak.

00:38:03.250 --> 00:38:05.930 align:middle line:84%
One of our fuel pins
catastrophically

00:38:05.930 --> 00:38:07.110 align:middle line:90%
failed something.

00:38:07.110 --> 00:38:08.850 align:middle line:90%
We have to unload the fuel.

00:38:08.850 --> 00:38:10.490 align:middle line:90%
We have to do some maintenance.

00:38:10.490 --> 00:38:15.090 align:middle line:84%
And so you can come up with
an excuse for doing this.

00:38:15.090 --> 00:38:18.330 align:middle line:84%
But you don't really
even have to do that.

00:38:18.330 --> 00:38:22.050 align:middle line:84%
The other thing
you can do is when

00:38:22.050 --> 00:38:25.850 align:middle line:84%
we build PWRs, the
very first load

00:38:25.850 --> 00:38:29.690 align:middle line:84%
that we put in the PWR
has a lower enrichment

00:38:29.690 --> 00:38:34.370 align:middle line:84%
and is burned much less
to break in the system.

00:38:34.370 --> 00:38:38.850 align:middle line:84%
And that load that is
sitting in every spent fuel

00:38:38.850 --> 00:38:40.810 align:middle line:90%
pool in the world.

00:38:40.810 --> 00:38:44.320 align:middle line:84%
It's the first batch of fuel
that we put in every reactor,

00:38:44.320 --> 00:38:47.760 align:middle line:84%
and the plutonium in that
first batch is pretty good.

00:38:47.760 --> 00:38:52.280 align:middle line:84%
And so every reactor has this
first batch sitting around

00:38:52.280 --> 00:38:55.380 align:middle line:84%
that we could just reprocess
and turn into fuel.

00:38:55.380 --> 00:39:05.320 align:middle line:90%


00:39:05.320 --> 00:39:12.240 align:middle line:84%
This green area is the typical
fuel from CANDU reactors.

00:39:12.240 --> 00:39:15.200 align:middle line:84%
So CANDU reactors,
heavy water reactors,

00:39:15.200 --> 00:39:18.040 align:middle line:84%
they overcome the
need for enrichment

00:39:18.040 --> 00:39:22.200 align:middle line:84%
by having water
moderator that is already

00:39:22.200 --> 00:39:26.640 align:middle line:84%
full of extra neutrons by using
deuterium instead of protium

00:39:26.640 --> 00:39:27.840 align:middle line:90%
light water.

00:39:27.840 --> 00:39:31.880 align:middle line:84%
And so they go in with a higher
concentration of uranium-238.

00:39:31.880 --> 00:39:33.980 align:middle line:84%
So you have more
neutron capture on 238,

00:39:33.980 --> 00:39:35.360 align:middle line:90%
which makes more plutonium.

00:39:35.360 --> 00:39:40.510 align:middle line:84%
And so what you wind up with
is stuff that is already not

00:39:40.510 --> 00:39:43.070 align:middle line:84%
exactly weapons-grade
but pretty close to it

00:39:43.070 --> 00:39:44.950 align:middle line:90%
under normal operation.

00:39:44.950 --> 00:39:48.030 align:middle line:84%
So CANDU reactors are
particularly problematic,

00:39:48.030 --> 00:39:54.950 align:middle line:84%
and a number of countries,
like India and South Korea,

00:39:54.950 --> 00:39:57.550 align:middle line:84%
have built CANDU
reactors very early

00:39:57.550 --> 00:40:02.630 align:middle line:84%
on in their nuclear programs
because of this fact.

00:40:02.630 --> 00:40:07.790 align:middle line:84%
It gave them a
cache of spent fuel

00:40:07.790 --> 00:40:09.830 align:middle line:84%
from which they
could make weapons

00:40:09.830 --> 00:40:12.077 align:middle line:84%
in the event they
decided they needed it.

00:40:12.077 --> 00:40:13.910 align:middle line:84%
And then they said, oh,
they're not economic

00:40:13.910 --> 00:40:17.670 align:middle line:90%
and then switched to PWRs.

00:40:17.670 --> 00:40:23.238 align:middle line:84%
But yeah, this is the
beginning of many countries.

00:40:23.238 --> 00:40:25.030 align:middle line:84%
Now some people-- I
don't know, does anyone

00:40:25.030 --> 00:40:28.790 align:middle line:84%
not believe me about the
reactor-grade plutonium?

00:40:28.790 --> 00:40:30.790 align:middle line:84%
Or has anyone heard that
reactor-grade plutonium

00:40:30.790 --> 00:40:32.050 align:middle line:90%
can't be used?

00:40:32.050 --> 00:40:35.510 align:middle line:90%


00:40:35.510 --> 00:40:38.820 align:middle line:84%
I won't ask if you
don't believe me.

00:40:38.820 --> 00:40:41.500 align:middle line:84%
There's an official US
government Department

00:40:41.500 --> 00:40:44.340 align:middle line:90%
of Energy statement on this.

00:40:44.340 --> 00:40:46.220 align:middle line:84%
And I think this is
long, but I think

00:40:46.220 --> 00:40:48.015 align:middle line:90%
it's worth me just reading it.

00:40:48.015 --> 00:40:50.140 align:middle line:84%
"Designing and building an
effective nuclear weapon

00:40:50.140 --> 00:40:54.140 align:middle line:84%
using reactor-grade plutonium
is less convenient than using

00:40:54.140 --> 00:40:55.280 align:middle line:90%
weapon-grade plutonium.

00:40:55.280 --> 00:40:57.540 align:middle line:84%
The degree to which these
obstacles can be overcome

00:40:57.540 --> 00:41:01.220 align:middle line:84%
depends on the sophistication
of the state or group attempting

00:41:01.220 --> 00:41:02.957 align:middle line:90%
to produce a nuclear weapon.

00:41:02.957 --> 00:41:04.540 align:middle line:84%
At the lowest level
of sophistication,

00:41:04.540 --> 00:41:09.100 align:middle line:84%
a potential proliferating
state or subnational group--"

00:41:09.100 --> 00:41:11.020 align:middle line:90%
by which they mean terrorist--

00:41:11.020 --> 00:41:14.300 align:middle line:84%
"using designs and technologies
no more sophisticated than those

00:41:14.300 --> 00:41:16.460 align:middle line:84%
used in first-generation
nuclear weapons--" i.e.

00:41:16.460 --> 00:41:23.420 align:middle line:84%
1945-- "could build
a nuclear weapon

00:41:23.420 --> 00:41:25.420 align:middle line:84%
from reactor-grade
plutonium that

00:41:25.420 --> 00:41:29.560 align:middle line:84%
would have an assured, reliable
yield of one or a few kilotons,

00:41:29.560 --> 00:41:32.745 align:middle line:84%
and probably a yield
significantly higher than that.

00:41:32.745 --> 00:41:34.120 align:middle line:84%
At the other end
of the spectrum,

00:41:34.120 --> 00:41:36.453 align:middle line:84%
advanced nuclear weapon states
such as the United States

00:41:36.453 --> 00:41:38.290 align:middle line:84%
and Russia, using
modern designs,

00:41:38.290 --> 00:41:40.770 align:middle line:84%
could produce weapons from
reactor-grade plutonium,

00:41:40.770 --> 00:41:43.630 align:middle line:84%
having reliable explosive
yields, weights,

00:41:43.630 --> 00:41:45.930 align:middle line:84%
and other characteristics
generally comparable to those

00:41:45.930 --> 00:41:48.770 align:middle line:84%
of weapons from
weapons-grade plutonium."

00:41:48.770 --> 00:41:52.690 align:middle line:84%
It is the case that you can
take any weapon, any US weapon,

00:41:52.690 --> 00:41:55.510 align:middle line:84%
and swap out the plutonium
for reactor-grade plutonium,

00:41:55.510 --> 00:41:58.850 align:middle line:90%
and it will work just fine.

00:41:58.850 --> 00:42:00.650 align:middle line:84%
"Proliferating
states using designs

00:42:00.650 --> 00:42:02.890 align:middle line:84%
of intermediate sophistication
could produce weapons

00:42:02.890 --> 00:42:04.570 align:middle line:84%
with assured yields
substantially higher

00:42:04.570 --> 00:42:08.010 align:middle line:84%
than the kiloton range possible
with simple, first-generation

00:42:08.010 --> 00:42:09.070 align:middle line:90%
nuclear devices.

00:42:09.070 --> 00:42:10.450 align:middle line:84%
In short,
reactor-grade plutonium

00:42:10.450 --> 00:42:14.350 align:middle line:84%
is weapons-usable, whether by
unsophisticated proliferators

00:42:14.350 --> 00:42:16.090 align:middle line:84%
or advanced nuclear
weapon states.

00:42:16.090 --> 00:42:18.450 align:middle line:84%
Theft of separated plutonium,
whether weapons-grade

00:42:18.450 --> 00:42:22.090 align:middle line:84%
or reactor-grade, would
pose a grave security risk."

00:42:22.090 --> 00:42:27.130 align:middle line:90%
And so that is why--

00:42:27.130 --> 00:42:29.490 align:middle line:90%
do I have a photo--

00:42:29.490 --> 00:42:32.210 align:middle line:84%
I worry about these
little canisters

00:42:32.210 --> 00:42:35.700 align:middle line:90%
of separated plutonium.

00:42:35.700 --> 00:42:41.003 align:middle line:84%
So let's say a state
has this-- yep?

00:42:41.003 --> 00:42:42.420 align:middle line:84%
AUDIENCE: I have
a quick question.

00:42:42.420 --> 00:42:47.560 align:middle line:84%
So reactor-grade plutonium is
essentially almost swappable

00:42:47.560 --> 00:42:49.520 align:middle line:90%
with weapons-grade plutonium?

00:42:49.520 --> 00:42:54.480 align:middle line:84%
Why did we spend so much on
making weapons-grade plutonium?

00:42:54.480 --> 00:42:56.520 align:middle line:90%
PROFESSOR: Safety.

00:42:56.520 --> 00:42:59.480 align:middle line:84%
The dose rate off of
reactor-grade plutonium

00:42:59.480 --> 00:43:01.840 align:middle line:90%
is substantially higher.

00:43:01.840 --> 00:43:07.400 align:middle line:84%
And our weapons are designed
so that the people who

00:43:07.400 --> 00:43:09.600 align:middle line:84%
handle those weapons
in the military

00:43:09.600 --> 00:43:11.560 align:middle line:90%
don't get a substantial dose.

00:43:11.560 --> 00:43:15.280 align:middle line:84%
In fact, we have very special
called ivory-grade plutonium,

00:43:15.280 --> 00:43:18.460 align:middle line:84%
which is ivory is 99 point
whatever percent pure--

00:43:18.460 --> 00:43:20.720 align:middle line:90%
you know the commercial--

00:43:20.720 --> 00:43:27.120 align:middle line:84%
that you can sleep on it so
that people in submarines

00:43:27.120 --> 00:43:32.350 align:middle line:84%
could literally sleep on
the nuclear torpedoes, which

00:43:32.350 --> 00:43:36.510 align:middle line:84%
I don't know if you've
ever been in a submarine.

00:43:36.510 --> 00:43:39.950 align:middle line:84%
Often, people bunk
in the torpedo room

00:43:39.950 --> 00:43:41.050 align:middle line:90%
next to the torpedo.

00:43:41.050 --> 00:43:43.770 align:middle line:90%
So you have to be-- that's why.

00:43:43.770 --> 00:43:50.810 align:middle line:90%


00:43:50.810 --> 00:43:54.290 align:middle line:84%
So let's say you're
Saudi Arabia.

00:43:54.290 --> 00:43:57.150 align:middle line:84%
You've bought your nuclear
reactor from the United States

00:43:57.150 --> 00:44:00.390 align:middle line:84%
because the United States
wants to give you a reactor.

00:44:00.390 --> 00:44:01.730 align:middle line:90%
What do you really have to do?

00:44:01.730 --> 00:44:04.110 align:middle line:84%
Well, you either have
spent fuel like this,

00:44:04.110 --> 00:44:06.790 align:middle line:84%
or you have it like
this, and now you

00:44:06.790 --> 00:44:09.230 align:middle line:90%
need to do the reprocessing.

00:44:09.230 --> 00:44:13.010 align:middle line:84%
How hard would it be to build
that reprocessing plant?

00:44:13.010 --> 00:44:16.810 align:middle line:84%
So I showed you in
the last lecture,

00:44:16.810 --> 00:44:19.510 align:middle line:84%
last set of slides,
this $20 billion

00:44:19.510 --> 00:44:25.270 align:middle line:84%
super complex reprocessing plant
that looked like a large city.

00:44:25.270 --> 00:44:31.620 align:middle line:84%
What if you really didn't
care about high volumes

00:44:31.620 --> 00:44:36.100 align:middle line:84%
and purified waste
streams and vitrification

00:44:36.100 --> 00:44:38.880 align:middle line:84%
and all the rest of it, and
you just wanted the plutonium?

00:44:38.880 --> 00:44:40.500 align:middle line:90%
How hard would it be?

00:44:40.500 --> 00:44:46.620 align:middle line:84%
Well, in 1977, Oak Ridge
asked this question,

00:44:46.620 --> 00:44:48.300 align:middle line:90%
and they did a study.

00:44:48.300 --> 00:44:51.780 align:middle line:84%
And this is the first page
of the memo from that study.

00:44:51.780 --> 00:44:57.440 align:middle line:84%
And if you read it, what they
propose is that, with a backhoe,

00:44:57.440 --> 00:45:01.460 align:middle line:84%
you could dig a swimming pool
hole, fill it with water.

00:45:01.460 --> 00:45:04.300 align:middle line:84%
You would put your fuel
bundle in the swimming pool

00:45:04.300 --> 00:45:07.140 align:middle line:84%
because you need to protect
yourself from radiation.

00:45:07.140 --> 00:45:09.240 align:middle line:90%
You need to cut the fuel.

00:45:09.240 --> 00:45:11.760 align:middle line:84%
So you get a carbide
cutting blade,

00:45:11.760 --> 00:45:14.555 align:middle line:84%
like you would use
on an angle grinder.

00:45:14.555 --> 00:45:16.180 align:middle line:84%
And it doesn't work
under water, so you

00:45:16.180 --> 00:45:20.140 align:middle line:84%
need a chain going up to a
motor which is above the water.

00:45:20.140 --> 00:45:21.860 align:middle line:84%
And you cut up the
fuel under the water,

00:45:21.860 --> 00:45:24.640 align:middle line:84%
and the fuel would
fall into a basket.

00:45:24.640 --> 00:45:27.940 align:middle line:84%
And then, using a crane, you
would transport that basket

00:45:27.940 --> 00:45:32.250 align:middle line:84%
into a series of
stainless steel tanks,

00:45:32.250 --> 00:45:35.530 align:middle line:84%
and they suggest you order the
tanks from the cheesemaking

00:45:35.530 --> 00:45:37.330 align:middle line:84%
industry, from the
dairy industry,

00:45:37.330 --> 00:45:40.170 align:middle line:84%
for use as stainless
steel tanks.

00:45:40.170 --> 00:45:45.450 align:middle line:84%
And you just do some
straightforward non purex

00:45:45.450 --> 00:45:51.170 align:middle line:84%
simplified chemical precipitate
lead bismuth process

00:45:51.170 --> 00:45:54.570 align:middle line:84%
and precipitate
out the plutonium.

00:45:54.570 --> 00:45:57.290 align:middle line:84%
And they conclude
that, when you're done,

00:45:57.290 --> 00:46:00.290 align:middle line:84%
it would take four to six months
to build this plant that you

00:46:00.290 --> 00:46:02.930 align:middle line:84%
could mail order from
the dairy catalog

00:46:02.930 --> 00:46:06.610 align:middle line:84%
and that, once you
had it built, you

00:46:06.610 --> 00:46:09.330 align:middle line:84%
could extract your first
weapon quantity of plutonium

00:46:09.330 --> 00:46:12.300 align:middle line:90%
in about one week.

00:46:12.300 --> 00:46:14.050 align:middle line:84%
And you could potentially
build this thing

00:46:14.050 --> 00:46:16.930 align:middle line:84%
without anyone really
noticing what you were up to.

00:46:16.930 --> 00:46:20.290 align:middle line:84%
It looks like you're building a
cheese factory with a swimming

00:46:20.290 --> 00:46:23.370 align:middle line:90%
pool.

00:46:23.370 --> 00:46:25.830 align:middle line:90%
And that's not that hard.

00:46:25.830 --> 00:46:29.520 align:middle line:90%


00:46:29.520 --> 00:46:31.360 align:middle line:90%
Are you likely to get caught?

00:46:31.360 --> 00:46:32.680 align:middle line:90%
You might.

00:46:32.680 --> 00:46:35.400 align:middle line:84%
It depends on how good you
are at operational security

00:46:35.400 --> 00:46:37.720 align:middle line:84%
and whether you go tell
large parts of the government

00:46:37.720 --> 00:46:40.360 align:middle line:90%
and some spy finds out.

00:46:40.360 --> 00:46:43.980 align:middle line:84%
But you might not, and you
might get away with this.

00:46:43.980 --> 00:46:48.000 align:middle line:84%
And once this plant were built
somewhere in the country, who

00:46:48.000 --> 00:46:51.360 align:middle line:84%
knows where, and you
divert your uranium fuel

00:46:51.360 --> 00:46:54.823 align:middle line:84%
bundles from your
reactor, maybe the IAEA

00:46:54.823 --> 00:46:56.740 align:middle line:84%
will notice that the
fuel bundles are missing.

00:46:56.740 --> 00:46:58.198 align:middle line:84%
Maybe they'll notice
it right away.

00:46:58.198 --> 00:47:00.520 align:middle line:84%
Maybe they'll take them
six months to notice it.

00:47:00.520 --> 00:47:02.400 align:middle line:84%
But if they notice
it right away,

00:47:02.400 --> 00:47:04.520 align:middle line:90%
who's to say where they went?

00:47:04.520 --> 00:47:06.160 align:middle line:90%
Where do I bomb?

00:47:06.160 --> 00:47:08.020 align:middle line:84%
You've got to find
that facility.

00:47:08.020 --> 00:47:15.640 align:middle line:84%
So this is the concern that
it's not actually all that hard.

00:47:15.640 --> 00:47:18.960 align:middle line:84%
Of course, it's much easier if
you have that facility already

00:47:18.960 --> 00:47:24.870 align:middle line:84%
built, and this is the other
pathway that countries can take.

00:47:24.870 --> 00:47:28.950 align:middle line:84%
And China, France,
Germany, Japan, Russia,

00:47:28.950 --> 00:47:33.270 align:middle line:84%
and the UK basically all decided
this was an interesting pathway

00:47:33.270 --> 00:47:37.150 align:middle line:90%
to building their bomb.

00:47:37.150 --> 00:47:38.550 align:middle line:84%
So what they said
is, oh, we need

00:47:38.550 --> 00:47:42.270 align:middle line:84%
to do the closed fuel
cycle for various reasons.

00:47:42.270 --> 00:47:46.710 align:middle line:84%
It's true, for example, in
Japan, the Rokkasho Plant, which

00:47:46.710 --> 00:47:49.390 align:middle line:84%
cost them $20 billion,
is because they

00:47:49.390 --> 00:47:53.270 align:middle line:84%
don't know what to do with
the spent nuclear fuel.

00:47:53.270 --> 00:47:57.510 align:middle line:84%
But actually, there was a
reprocessing plant, Tokaimura,

00:47:57.510 --> 00:48:01.590 align:middle line:84%
which was built before
Rokkasho was built.

00:48:01.590 --> 00:48:03.390 align:middle line:84%
And this was why
it was like, oh, it

00:48:03.390 --> 00:48:06.750 align:middle line:84%
was a research plan to see if
we want to close the fuel cycle.

00:48:06.750 --> 00:48:09.910 align:middle line:84%
And it made a lot of plutonium,
and then they shut the plant.

00:48:09.910 --> 00:48:14.910 align:middle line:84%
And so people have countries
have said over time

00:48:14.910 --> 00:48:18.430 align:middle line:84%
that we're going to do some
research into this closed fuel

00:48:18.430 --> 00:48:21.190 align:middle line:84%
cycle concept, and they
build these plants.

00:48:21.190 --> 00:48:23.420 align:middle line:84%
And everyone knows that
these plants exist,

00:48:23.420 --> 00:48:25.500 align:middle line:84%
and they operate
them openly, and they

00:48:25.500 --> 00:48:28.300 align:middle line:84%
say that we're just doing
the fast reactor thing,

00:48:28.300 --> 00:48:32.900 align:middle line:84%
and then they go, oh, it's too
expensive, and they give up.

00:48:32.900 --> 00:48:36.620 align:middle line:84%
But it's really been
a weapons program

00:48:36.620 --> 00:48:39.700 align:middle line:90%
for quite a number of these.

00:48:39.700 --> 00:48:43.440 align:middle line:84%
Pakistan and South Korea
have been trying to do this.

00:48:43.440 --> 00:48:46.680 align:middle line:84%
South Korea has been
slowly inching along.

00:48:46.680 --> 00:48:48.920 align:middle line:84%
But they don't want to
irritate the US government.

00:48:48.920 --> 00:48:52.740 align:middle line:84%
So there's constant negotiations
about what they can and cannot

00:48:52.740 --> 00:48:53.620 align:middle line:90%
do.

00:48:53.620 --> 00:48:56.040 align:middle line:84%
But they are slowly
moving in this direction.

00:48:56.040 --> 00:48:59.420 align:middle line:90%


00:48:59.420 --> 00:49:01.140 align:middle line:84%
So of course, you go
from this situation

00:49:01.140 --> 00:49:02.980 align:middle line:84%
where you have to
divert the spent fuel

00:49:02.980 --> 00:49:07.820 align:middle line:84%
bundle to your secret
reprocessing site to this,

00:49:07.820 --> 00:49:09.900 align:middle line:84%
as we've talked
about, everything

00:49:09.900 --> 00:49:13.780 align:middle line:90%
has been done for you basically.

00:49:13.780 --> 00:49:15.380 align:middle line:84%
Fortunately, today,
most of the world

00:49:15.380 --> 00:49:19.100 align:middle line:84%
has been convinced that
routine separation of plutonium

00:49:19.100 --> 00:49:23.690 align:middle line:84%
is just not economic
and doesn't make sense.

00:49:23.690 --> 00:49:27.090 align:middle line:84%
Of the nonweapons states,
states that don't already

00:49:27.090 --> 00:49:31.490 align:middle line:84%
have nuclear weapons, Japan
is the only country doing it.

00:49:31.490 --> 00:49:35.130 align:middle line:84%
And because it does
it, and because it

00:49:35.130 --> 00:49:37.370 align:middle line:84%
is so close to having a
bomb at any given moment

00:49:37.370 --> 00:49:39.850 align:middle line:84%
because it has
separated plutonium,

00:49:39.850 --> 00:49:43.690 align:middle line:84%
the IAEA, the International
Atomic Energy Agency

00:49:43.690 --> 00:49:47.950 align:middle line:84%
that inspects these facilities,
last time I checked,

00:49:47.950 --> 00:49:50.770 align:middle line:84%
spends about a full
third of its inspection

00:49:50.770 --> 00:49:56.050 align:middle line:84%
budget on this plant in
Japan because it's just

00:49:56.050 --> 00:49:58.710 align:middle line:84%
so close to being ready
for nuclear weapons.

00:49:58.710 --> 00:50:01.490 align:middle line:84%
And you can imagine, if we
have the closed fuel cycle,

00:50:01.490 --> 00:50:04.490 align:middle line:84%
and this is being spread
all around the world,

00:50:04.490 --> 00:50:08.570 align:middle line:84%
just how difficult it would
be, almost impossible,

00:50:08.570 --> 00:50:15.850 align:middle line:84%
to prevent some country
from tipping over.

00:50:15.850 --> 00:50:19.000 align:middle line:84%
I've already talked
about this, so

00:50:19.000 --> 00:50:22.720 align:middle line:84%
let me talk about the
dedicated pathways

00:50:22.720 --> 00:50:25.220 align:middle line:84%
that countries could take,
and then we'll wrap up.

00:50:25.220 --> 00:50:28.120 align:middle line:90%


00:50:28.120 --> 00:50:31.380 align:middle line:84%
So this is also maybe
not that difficult,

00:50:31.380 --> 00:50:36.458 align:middle line:84%
but it does require building
up a dedicated program.

00:50:36.458 --> 00:50:38.000 align:middle line:84%
And you have to
decide whether you're

00:50:38.000 --> 00:50:40.863 align:middle line:84%
going to try to do it
secretly or overtly.

00:50:40.863 --> 00:50:42.780 align:middle line:84%
And generally, when
you're building a reactor,

00:50:42.780 --> 00:50:45.960 align:middle line:84%
it's too big of a construction
project to keep it secret.

00:50:45.960 --> 00:50:48.760 align:middle line:84%
So then you have to come
up with an excuse for why

00:50:48.760 --> 00:50:49.820 align:middle line:90%
you're doing this.

00:50:49.820 --> 00:50:52.480 align:middle line:90%


00:50:52.480 --> 00:50:55.680 align:middle line:84%
The excuse that
many countries give

00:50:55.680 --> 00:50:59.200 align:middle line:84%
is that they're interested
in nuclear power,

00:50:59.200 --> 00:51:02.480 align:middle line:84%
and they want to train people,
and they want to test materials

00:51:02.480 --> 00:51:03.960 align:middle line:90%
to design reactors.

00:51:03.960 --> 00:51:07.400 align:middle line:84%
And they're just building
MIT, MITR, the MIT reactor.

00:51:07.400 --> 00:51:11.520 align:middle line:84%
Basically, we're just doing
just doing what MIT does.

00:51:11.520 --> 00:51:15.280 align:middle line:84%
But then they choose the
design of their reactor,

00:51:15.280 --> 00:51:19.710 align:middle line:84%
unlike the MIT reactor, to be a
reactor that produces plutonium

00:51:19.710 --> 00:51:20.430 align:middle line:90%
well.

00:51:20.430 --> 00:51:25.070 align:middle line:84%
So the research reactor
that the Iranians designed

00:51:25.070 --> 00:51:28.950 align:middle line:84%
was a natural uranium-fueled
heavy water reactor,

00:51:28.950 --> 00:51:30.490 align:middle line:90%
just like a CANDU reactor.

00:51:30.490 --> 00:51:32.990 align:middle line:84%
It produces
great-quality plutonium,

00:51:32.990 --> 00:51:34.790 align:middle line:84%
and it was large
enough that it would

00:51:34.790 --> 00:51:41.110 align:middle line:84%
produce significant quantities
in on the order of a year.

00:51:41.110 --> 00:51:49.430 align:middle line:84%
So the problem is that unless
you have nuclear power, even

00:51:49.430 --> 00:51:53.670 align:middle line:84%
though you can do this
independently of nuclear power,

00:51:53.670 --> 00:51:59.550 align:middle line:84%
your excuse depends on the
idea that you are building

00:51:59.550 --> 00:52:02.150 align:middle line:90%
nuclear power at the same time.

00:52:02.150 --> 00:52:07.250 align:middle line:84%
So it still has this
connection into nuclear power.

00:52:07.250 --> 00:52:11.230 align:middle line:84%
And if instead we said,
well, nuclear power is only

00:52:11.230 --> 00:52:13.190 align:middle line:84%
for certain countries
that don't have access

00:52:13.190 --> 00:52:16.420 align:middle line:84%
to high-quality
wind and solar, it

00:52:16.420 --> 00:52:19.580 align:middle line:84%
would be really hard for
Saudi Arabia to do this

00:52:19.580 --> 00:52:22.020 align:middle line:84%
because you look at Saudi
Arabia and say, what exactly

00:52:22.020 --> 00:52:26.820 align:middle line:90%
is your solar shortage here?

00:52:26.820 --> 00:52:29.860 align:middle line:84%
But nevertheless, some reason
the US nuclear industry

00:52:29.860 --> 00:52:33.600 align:middle line:84%
is very excited about giving
Saudi Arabia nuclear power.

00:52:33.600 --> 00:52:36.980 align:middle line:90%


00:52:36.980 --> 00:52:42.340 align:middle line:84%
So let me just give you a sense
of what this path entails.

00:52:42.340 --> 00:52:52.660 align:middle line:84%
This is in 2005, is a satellite
image of the Arak site in Iran.

00:52:52.660 --> 00:52:55.660 align:middle line:84%
This is where they
were breaking ground.

00:52:55.660 --> 00:52:58.020 align:middle line:84%
They're going to build
an indigenously designed,

00:52:58.020 --> 00:53:02.220 align:middle line:84%
40-megawatt, heavy
water-moderated reactor.

00:53:02.220 --> 00:53:06.480 align:middle line:84%
It produced about 11 kilograms
of plutonium per year.

00:53:06.480 --> 00:53:08.960 align:middle line:84%
So that's enough for one
to two nuclear weapons,

00:53:08.960 --> 00:53:12.490 align:middle line:84%
depending on how advanced
your weapons are--

00:53:12.490 --> 00:53:13.450 align:middle line:90%
2005.

00:53:13.450 --> 00:53:20.290 align:middle line:84%
Here's what it looked like
five years later in 2010.

00:53:20.290 --> 00:53:24.290 align:middle line:90%
And it's almost complete.

00:53:24.290 --> 00:53:34.370 align:middle line:84%
At this point, they were really
getting ready to load fuel

00:53:34.370 --> 00:53:35.550 align:middle line:90%
into the reactor.

00:53:35.550 --> 00:53:38.730 align:middle line:84%
They had basically built
most of this stuff.

00:53:38.730 --> 00:53:40.850 align:middle line:84%
It looks like the
time scale for country

00:53:40.850 --> 00:53:44.290 align:middle line:84%
to do this that has
basically minimal experience

00:53:44.290 --> 00:53:48.470 align:middle line:84%
in nuclear engineering is
on the order of a decade,

00:53:48.470 --> 00:53:50.190 align:middle line:90%
12 years, maybe 15 years.

00:53:50.190 --> 00:53:53.290 align:middle line:84%
Depends on how much
money they pour into it

00:53:53.290 --> 00:53:57.090 align:middle line:84%
and how sophisticated
their existing engineering

00:53:57.090 --> 00:53:59.210 align:middle line:90%
infrastructure is.

00:53:59.210 --> 00:54:05.890 align:middle line:84%
So it is a pathway to a weapon,
but it's kind of the long play.

00:54:05.890 --> 00:54:09.770 align:middle line:84%
It's not the backup
option in case,

00:54:09.770 --> 00:54:12.660 align:middle line:84%
like, we don't need
nuclear weapons,

00:54:12.660 --> 00:54:14.170 align:middle line:84%
but just in case
someone attacks us,

00:54:14.170 --> 00:54:15.920 align:middle line:84%
we'd like to be able
to make them quickly.

00:54:15.920 --> 00:54:17.760 align:middle line:90%
That's how Japan thinks.

00:54:17.760 --> 00:54:20.880 align:middle line:84%
And so that's why Japan
wants to have the plutonium

00:54:20.880 --> 00:54:24.240 align:middle line:90%
ready to go just in case.

00:54:24.240 --> 00:54:26.400 align:middle line:84%
This option doesn't
give you that if you

00:54:26.400 --> 00:54:28.720 align:middle line:84%
have to start building
this thing from scratch.

00:54:28.720 --> 00:54:31.880 align:middle line:84%
And so that's again
where nuclear power

00:54:31.880 --> 00:54:34.200 align:middle line:90%
changes the calculation.

00:54:34.200 --> 00:54:39.460 align:middle line:84%
It says if you're not intending
to pursue nuclear weapons,

00:54:39.460 --> 00:54:43.560 align:middle line:84%
absolutely, but you just
want to security blanket,

00:54:43.560 --> 00:54:45.180 align:middle line:84%
nuclear power will
get you there.

00:54:45.180 --> 00:54:48.400 align:middle line:84%
And I think that's basically
why Saudi Arabia wants

00:54:48.400 --> 00:54:49.640 align:middle line:90%
nuclear power today.

00:54:49.640 --> 00:54:52.920 align:middle line:84%
They just they want to have
all this stuff just in case

00:54:52.920 --> 00:54:56.000 align:middle line:90%
they need it.

00:54:56.000 --> 00:55:01.400 align:middle line:90%
Finally, let's look at uranium.

00:55:01.400 --> 00:55:07.560 align:middle line:84%
Historically, this was regarded
as the most difficult path

00:55:07.560 --> 00:55:10.310 align:middle line:90%
to uranium enrichment.

00:55:10.310 --> 00:55:11.530 align:middle line:90%
Let me see if I have--

00:55:11.530 --> 00:55:14.150 align:middle line:90%


00:55:14.150 --> 00:55:16.710 align:middle line:90%
I have some slides--

00:55:16.710 --> 00:55:21.270 align:middle line:84%
the most difficult
path to a nuclear bomb.

00:55:21.270 --> 00:55:25.030 align:middle line:90%
That has since changed in 1990.

00:55:25.030 --> 00:55:28.670 align:middle line:84%
Pakistan broke the mold on
this when they developed

00:55:28.670 --> 00:55:32.070 align:middle line:90%
their own centrifuge program.

00:55:32.070 --> 00:55:36.950 align:middle line:84%
And if you want, I can
tell you the history

00:55:36.950 --> 00:55:38.650 align:middle line:90%
of this in a separate talk.

00:55:38.650 --> 00:55:43.230 align:middle line:90%
It's an interesting story.

00:55:43.230 --> 00:55:48.310 align:middle line:84%
Since then, Iraq, Iran,
Libya, and North Korea

00:55:48.310 --> 00:55:49.850 align:middle line:90%
have all followed suit.

00:55:49.850 --> 00:55:53.230 align:middle line:84%
They all also pursued
uranium enrichment,

00:55:53.230 --> 00:55:55.830 align:middle line:84%
dedicated uranium
enrichment, as a path

00:55:55.830 --> 00:55:59.390 align:middle line:84%
to building their
nuclear weapons.

00:55:59.390 --> 00:56:04.750 align:middle line:84%
The reason-- it turns out
that making gas centrifuges,

00:56:04.750 --> 00:56:06.150 align:middle line:84%
the modern way
you do enrichment,

00:56:06.150 --> 00:56:10.620 align:middle line:84%
is a lot easier than the old
form of enrichment, which

00:56:10.620 --> 00:56:11.920 align:middle line:90%
was called gaseous diffusion.

00:56:11.920 --> 00:56:15.420 align:middle line:84%
And I'll show you
that in a moment.

00:56:15.420 --> 00:56:19.300 align:middle line:84%
Now, again, what happens if you
get caught building this thing,

00:56:19.300 --> 00:56:21.700 align:middle line:90%
as the Iranians did?

00:56:21.700 --> 00:56:25.220 align:middle line:84%
Well, the Iranians said we
have this power reactor we're

00:56:25.220 --> 00:56:26.560 align:middle line:90%
building called [INAUDIBLE].

00:56:26.560 --> 00:56:30.660 align:middle line:84%
It's big-- it started as
a German reactor design,

00:56:30.660 --> 00:56:32.500 align:middle line:84%
and then was modified
by the Russians

00:56:32.500 --> 00:56:39.260 align:middle line:84%
as some weird hybrid reactor,
but basically a big PWR.

00:56:39.260 --> 00:56:42.420 align:middle line:84%
And they said, we want to be
able to make the fuel ourselves,

00:56:42.420 --> 00:56:45.340 align:middle line:84%
and that's why we have
enrichment program.

00:56:45.340 --> 00:56:48.620 align:middle line:90%
And no one really believed them.

00:56:48.620 --> 00:56:52.540 align:middle line:84%
But the fact that
they had that reactor

00:56:52.540 --> 00:56:59.660 align:middle line:84%
meant our hands were tied under
the NPT of really accusing Iran

00:56:59.660 --> 00:57:01.620 align:middle line:90%
of pursuing a weapons program.

00:57:01.620 --> 00:57:05.610 align:middle line:84%
And it kind of dragged
things out for decades

00:57:05.610 --> 00:57:08.608 align:middle line:84%
and made the
problem a lot worse.

00:57:08.608 --> 00:57:11.150 align:middle line:84%
If they had just been doing this
without the Bushehr reactor,

00:57:11.150 --> 00:57:14.290 align:middle line:84%
we would have been--
you're guilty of trying

00:57:14.290 --> 00:57:18.330 align:middle line:84%
to make nuclear weapons, and
there would be no discussion.

00:57:18.330 --> 00:57:23.515 align:middle line:90%
So again, you need the excuse.

00:57:23.515 --> 00:57:25.890 align:middle line:84%
And that's where the connection
to civilian nuclear power

00:57:25.890 --> 00:57:27.530 align:middle line:90%
comes in.

00:57:27.530 --> 00:57:29.810 align:middle line:84%
So just let's look
at what this entails.

00:57:29.810 --> 00:57:32.970 align:middle line:90%
First, you need uranium.

00:57:32.970 --> 00:57:34.490 align:middle line:90%
It's pretty common.

00:57:34.490 --> 00:57:36.450 align:middle line:90%
It's more common than tin.

00:57:36.450 --> 00:57:41.450 align:middle line:84%
Every country has enough uranium
except for, maybe, I don't know,

00:57:41.450 --> 00:57:44.170 align:middle line:90%
Monaco.

00:57:44.170 --> 00:57:48.770 align:middle line:84%
Every country has enough
uranium to build a bomb.

00:57:48.770 --> 00:57:51.450 align:middle line:84%
Not every country has
economically viable deposits

00:57:51.450 --> 00:57:54.050 align:middle line:84%
that they could extract
and sell uranium

00:57:54.050 --> 00:57:56.050 align:middle line:90%
competitively in the market.

00:57:56.050 --> 00:57:59.310 align:middle line:84%
But everyone has enough uranium
sitting around to make a bomb.

00:57:59.310 --> 00:58:02.050 align:middle line:84%
And just to give you
an example of that,

00:58:02.050 --> 00:58:07.640 align:middle line:84%
Iraq, during its weapons
program, had a phosphate mine.

00:58:07.640 --> 00:58:10.280 align:middle line:84%
You mine phosphates
to make soap,

00:58:10.280 --> 00:58:14.120 align:middle line:84%
and it happens to be
that uranium tends

00:58:14.120 --> 00:58:17.640 align:middle line:90%
to coexist in phosphate ores.

00:58:17.640 --> 00:58:20.120 align:middle line:84%
So they went to the
phosphate mine tailing pond,

00:58:20.120 --> 00:58:22.600 align:middle line:84%
where they had all this
waste, and they just

00:58:22.600 --> 00:58:26.400 align:middle line:84%
took that and reprocessed
it to extract the uranium

00:58:26.400 --> 00:58:28.120 align:middle line:90%
for their weapons program.

00:58:28.120 --> 00:58:30.520 align:middle line:90%
It's around.

00:58:30.520 --> 00:58:33.040 align:middle line:90%
It's not uncommon.

00:58:33.040 --> 00:58:36.463 align:middle line:84%
Previously, maybe
you could do that.

00:58:36.463 --> 00:58:37.880 align:middle line:84%
You could go and
take the tailings

00:58:37.880 --> 00:58:39.920 align:middle line:90%
out of at a phosphate mine.

00:58:39.920 --> 00:58:41.380 align:middle line:90%
You could do this.

00:58:41.380 --> 00:58:44.160 align:middle line:84%
We talked about this the other
day is in-situ leach mining.

00:58:44.160 --> 00:58:47.600 align:middle line:84%
You drill a hole in the ground,
and you pump sulfuric acid down

00:58:47.600 --> 00:58:51.680 align:middle line:84%
or hydrogen peroxide down,
and you dissolve uranium,

00:58:51.680 --> 00:58:53.440 align:middle line:90%
and then you pump it back up.

00:58:53.440 --> 00:58:56.453 align:middle line:84%
And this does not
look like a big--

00:58:56.453 --> 00:58:58.120 align:middle line:84%
you look at this from
a satellite photo,

00:58:58.120 --> 00:59:00.240 align:middle line:84%
and you have no idea
what's going on here.

00:59:00.240 --> 00:59:04.030 align:middle line:90%
Is this a well?

00:59:04.030 --> 00:59:06.230 align:middle line:84%
You could cover this
up with some sheds.

00:59:06.230 --> 00:59:08.170 align:middle line:90%
This is not hard to hide.

00:59:08.170 --> 00:59:11.095 align:middle line:90%


00:59:11.095 --> 00:59:12.970 align:middle line:84%
Of course, now you have
to do the enrichment.

00:59:12.970 --> 00:59:16.350 align:middle line:84%
You have to go from natural
uranium, which is only 0.7%

00:59:16.350 --> 00:59:19.370 align:middle line:84%
uranium-235, to
something up here.

00:59:19.370 --> 00:59:26.350 align:middle line:84%
And so you need to build
centrifuges to do that.

00:59:26.350 --> 00:59:30.590 align:middle line:84%
And here's an example of why
people thought this was hard.

00:59:30.590 --> 00:59:33.390 align:middle line:84%
Here's the building
that the United States

00:59:33.390 --> 00:59:35.110 align:middle line:84%
built at the end of
the Manhattan Project

00:59:35.110 --> 00:59:38.950 align:middle line:90%
to do its uranium enrichment.

00:59:38.950 --> 00:59:41.150 align:middle line:90%
It's called K-25.

00:59:41.150 --> 00:59:45.370 align:middle line:84%
It's 44 acres of land
in a single building,

00:59:45.370 --> 00:59:49.710 align:middle line:84%
employed 12,000 people,
and used, in one building,

00:59:49.710 --> 00:59:52.130 align:middle line:84%
three times the electricity
of the entire city of Detroit,

00:59:52.130 --> 00:59:54.110 align:middle line:90%
Michigan.

00:59:54.110 --> 00:59:56.510 align:middle line:84%
This is a photo
of a small section

00:59:56.510 --> 00:59:57.850 align:middle line:90%
of the inside of the building.

00:59:57.850 --> 01:00:03.140 align:middle line:84%
And you can see the
size of the pipe works.

01:00:03.140 --> 01:00:05.800 align:middle line:90%
And for scale, this is a person.

01:00:05.800 --> 01:00:09.140 align:middle line:90%


01:00:09.140 --> 01:00:12.380 align:middle line:84%
And there were 44
acres of this stuff--

01:00:12.380 --> 01:00:16.120 align:middle line:84%
huge compressors and
all of this stuff.

01:00:16.120 --> 01:00:23.280 align:middle line:84%
So this is why people thought
other countries can't do this.

01:00:23.280 --> 01:00:25.280 align:middle line:84%
We'll pick up on the
rest of enrichment.

01:00:25.280 --> 01:00:29.550 align:middle line:84%
We'll talk about centrifuges
next time, Monday.

01:00:29.550 --> 01:00:58.000 align:middle line:90%