WEBVTT

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[SQUEAKING]
[RUSTLING] [CLICKING]

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JUEJUN HU: OK.

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So as I said, this is
not the topic I proposed.

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You proposed it.

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So this is my 3071
final project.

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Now you get a chance to hear
the presentation and grade it.

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All right.

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I also just also want
to mention that this

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is a topic that's not in my
area of expertise, obviously.

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It's actually, in
fact, pretty far.

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But it's good.

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I actually get to learn
a lot of new stuff.

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So that's part of the good thing
I sometimes say about academia.

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People actually pay you
to learn new things.

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All right.

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So we are talking about
biomineralization.

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Specifically, I'm going
to talk a lot about what

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the role amorphous material has
played in that kind of process

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here.

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Some references.

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Obviously, you can
always find these books.

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Read a bit more.

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These are some of the ones I
referenced in the process here.

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This is the outline
of the lecture today.

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I will start out by giving
you a brief introduction

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of biomineralization.

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I will then delve into
a few specific examples

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about biomineralization and
talk about some of the processes

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there.

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Then I'll move on to talk about
some common features that you

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will see in biomineralization.

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In particular, if you look
from a structural perspective,

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a lot of these materials
form in this process.

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They all have a
hierarchical microstructure.

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So what I specifically
mean by that

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is that there are
different length scales.

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And at different length scales,
from macroscopic to mesoscopic,

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microscopic to nanoscale,
you have different kind

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of structure entities
that forms this kind

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of hierarchical microstructure.

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We'll go into that.

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That's a very common
feature in this kind

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of biomineralized materials.

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And in order to form this kind
of hierarchical microstructure,

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turns out the
common way of doing

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deposition and crystallization,
the common material growth

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techniques, they do
not really apply.

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And that's actually where
amorphous material comes in.

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What you will see is that
in a lot of these materials,

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instead of directly forming
the final microstructure,

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they always go through
an intermediate step

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by having this kind of
transient amorphous phase

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or transient
amorphous precursors

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and then crystallize it into
the final crystalline form.

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So amorphous material
does play a very big role

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in biomineralization.

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So you picked a
good topic that's

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very relevant to this class.

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And in the end, I'm
going to just talk

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about some applications.

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Basically, some
bioinspired different kind

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of applications leveraging the
principles of biomineralization.

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So what is biomineralization?

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Now, specifically,
what we are going

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to focus on in this
lecture is what

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we call the biologically
controlled mineralization.

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If you look at
literature, people

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like to categorize
biomineralization

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into two main classes.

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You have so-called biologically
induced mineralization.

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You also have biologically
controlled mineralization.

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So for biologically
induced mineralization,

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the organism does not
play an active role

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in trying to control essentially
growth steps of the materials.

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What they did is they
essentially facilitate or create

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the microenvironment that
then triggers mineralization.

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So the example will
be some bacteria.

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For example, their
metabolic products

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becomes essentially the
essential ingredient

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for subsequent
mineral precipitation.

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But in that case, the
bacteria has no active role

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in controlling
the microstructure

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of those kind of precipitation.

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So that's quite
different in the case

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of biologically controlled
mineralization, which

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is the focus of today,
where the organism actually

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play a very active role in
shaping the final product.

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We'll go through that
in the next few slides.

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So definition here.

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As I said, it's basically the
formation of inorganic solids

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by living organisms.

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But when we say
inorganic solids here,

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it turns out usually
it's a composite.

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It's a composite that contains
usually organic matrix and then

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and inorganic phase, which comes
from this precipitation process.

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So I'm giving you a
few examples here.

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This is where your first
proposal, talking about glass

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sponge.

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I'm going to discuss about
glass sponge a little bit.

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But you also see other
examples, even in us.

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We have teeth.

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We have bones.

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That's very typical products
of biomineralization.

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So now, let me go through
a few examples talking

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about biomineralization.

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The first one here, seashells.

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I actually have a little
YouTube video here,

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which I believe talk about the
material structure very well.

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[VIDEO PLAYBACK]

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- But durability goes
right along with this.

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You see, we have--

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JUEJUN HU: There we go.

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- Thanks to Curiosity Stream for
supporting PBS Digital Studios.

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Seashells and chalk are both
made of calcium carbonate.

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By itself, the mineral
is brittle, crumbly,

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and soft enough to write
out a homework assignment.

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Seashells, on the other hand,
are wonderfully resilient.

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They're tough, they
resist breaking,

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and they definitely can't be
used to doodle on the sidewalk,

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but they're still
primarily CaCO3.

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So what makes
seashells so different?

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How can this and this be
made of the same stuff?

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We're talking about the
mineral chalk, by the way.

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Sidewalk and classroom
chalk are usually

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made from a different mineral,
known as gypsum, but we digress.

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Both seashells and
mineral chalk are

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the product of living things.

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Those chalk deposits
were generally

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formed from the gradual
buildup and compression

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of single-celled ocean
organisms with calcified shells.

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But bivalve mollusks,
like oysters and mussels,

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are much more sophisticated
shell builders.

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When we use that mineral
chalk, it's long dead,

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and all that's left
is the crumbly stuff.

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But these mollusks are pulling
dissolved carbonate and calcium

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from the ocean for some pretty
fancy biological architecture.

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Seashells contain 95% or
more calcium carbonate.

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The rest is mostly protein
and a bit of sugar.

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But a little biochemistry
goes a long way.

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Calcium carbonate can take
on a variety of forms.

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Even though its chemical
formula never changes,

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its crystal structure, which is
the 3D arrangement of its atoms

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in space, does change.

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The two forms we
care about right

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now are calcite and aragonite.

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Calcite tends to be more stable
than aragonite, but many bivalve

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shells contain a layer of each--

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calcite on the
outside of the shell

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and aragonite on the inside.

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One benefit to layering is
that the crystal structures are

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oriented differently in space.

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If the calcite layer
fractures, that fracture

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will probably stop when it
hits the aragonite layer

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because aragonite doesn't
break the same way.

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But that alone isn't nearly
enough to make seashells so much

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tougher than chalk.

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We told you mollusks
were amazing builders.

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The aragonite layer in a shell
like an oyster's is called

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nacre, or mother of pearl.

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Here's how scientists have
speculated mollusks actually

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make the stuff.

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Nacre is made up of layers of
aragonite crystals separated

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by very thin layers of protein.

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Those layers are anchored by a
chain of sugars called chitin.

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Mono and disaccharides,
the kind of sugars we eat,

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are water soluble and not
good building materials

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by themselves.

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Try to build a castle
out of sugar cubes

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and see how long it lasts.

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But chain them together
in long strings called

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polysaccharides, and they
can become tough and fibrous.

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Chitin is one such
polysaccharide.

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Proteins attached
to the chitin layer

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give the calcium
carbonate crystals

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a place to start growing.

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Those proteins have
charged regions

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that attract the minerals.

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Because of how those
regions are spaced,

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the crystals can grow
in regular chunks

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until they get the next
layer and meet each other

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at the edges.

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That's not everything the
proteins and polysaccharides do.

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Shell formation
requires a whole army

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of complex biological molecules,
and scientists are still

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trying to understand
how it all goes down.

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Nacre is literally thousands
of times tougher than chalk,

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thanks to the layers
of protein and chitin

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and the precise
structural control.

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And then the oysters
go on to make pearls.

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They're so talented.

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What all that means is
that mollusks don't just

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wear these minerals as a hat.

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They control how the shell is
made and what kind of crystal

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forms, whether
calcite or aragonite.

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They can make all sorts
of neat shell shapes

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that don't look anything
like a stick of chalk.

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And they can even
remodel their shells

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throughout their lifetime.

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And that's why you can't
make sidewalk doodles

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with a seashell, which does
work out in the animal's favor

00:08:18.970 --> 00:08:19.850 align:middle line:90%
after all.

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Thank you to Curiosity Stream
for supporting PBS Digital

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Studios.

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[END PLAYBACK]

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JUEJUN HU: You get to see
a little bit about what

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seashells are composed of.

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So as the video
says, basically, it's

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similarly a composite material.

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You have a mineral
phase, which is either

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the calcite or aragonite.

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These are two polymorphs
of calcium carbonate.

00:08:41.210 --> 00:08:44.290 align:middle line:84%
And there's also some
organic materials

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like chitin, the polysaccharide,
as well as some proteins.

00:08:47.810 --> 00:08:53.280 align:middle line:84%
So the matrix
proteins, they actually

00:08:53.280 --> 00:08:55.960 align:middle line:84%
play a very important
role because scientists

00:08:55.960 --> 00:08:58.240 align:middle line:84%
have performed studies
looking into essentially how

00:08:58.240 --> 00:09:01.720 align:middle line:84%
these proteins can actually
suppress or promote

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the formation of one
polymorph over the other.

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Some proteins will
actually induce

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precipitation, for
example, of only aragonite,

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but not the other one.

00:09:08.700 --> 00:09:12.580 align:middle line:84%
And the reason they need
these two kind of polymorphs,

00:09:12.580 --> 00:09:14.560 align:middle line:84%
if you look at what
I'm showing you here,

00:09:14.560 --> 00:09:18.040 align:middle line:84%
this is basically what the
two polymorphs look like.

00:09:18.040 --> 00:09:19.803 align:middle line:90%
This is basically abalone shell.

00:09:19.803 --> 00:09:21.720 align:middle line:84%
So if you look at the
inside of abalone shell,

00:09:21.720 --> 00:09:24.986 align:middle line:90%
this is basically nacre.

00:09:24.986 --> 00:09:30.360 align:middle line:84%
It has this kind of prismatic
color with a smooth surface.

00:09:30.360 --> 00:09:32.160 align:middle line:90%
This is actually a nacre phase.

00:09:32.160 --> 00:09:34.540 align:middle line:84%
Outside is what they
call the prismatic phase.

00:09:34.540 --> 00:09:36.000 align:middle line:84%
But this is basically
the calcite.

00:09:36.000 --> 00:09:39.200 align:middle line:84%
So inside is aragonite,
outside is calcite.

00:09:39.200 --> 00:09:40.600 align:middle line:84%
They have different
complementary

00:09:40.600 --> 00:09:41.880 align:middle line:90%
mechanical properties.

00:09:41.880 --> 00:09:45.200 align:middle line:84%
Calcite tends to be very
resistant to puncture,

00:09:45.200 --> 00:09:46.400 align:middle line:90%
to puncture damage.

00:09:46.400 --> 00:09:49.960 align:middle line:84%
And they also help to suppress
any kind of crack propagation.

00:09:49.960 --> 00:09:54.080 align:middle line:84%
Whereas nacre, because of
the interlayer organic phase,

00:09:54.080 --> 00:09:57.080 align:middle line:84%
is actually a lot more
ductile and compliant

00:09:57.080 --> 00:09:59.100 align:middle line:90%
compared to calcite.

00:09:59.100 --> 00:10:01.720 align:middle line:84%
So this combination
of materials will

00:10:01.720 --> 00:10:05.600 align:middle line:84%
give a very excellent mechanical
toughness of the seashells.

00:10:05.600 --> 00:10:08.120 align:middle line:90%


00:10:08.120 --> 00:10:08.720 align:middle line:90%
OK.

00:10:08.720 --> 00:10:11.200 align:middle line:84%
So one more thing I also
want to mention here

00:10:11.200 --> 00:10:16.520 align:middle line:84%
is that these mollusks,
they do not directly

00:10:16.520 --> 00:10:18.520 align:middle line:90%
form this crystalline phase.

00:10:18.520 --> 00:10:21.880 align:middle line:84%
What they will do, before they
form the crystalline phase,

00:10:21.880 --> 00:10:25.640 align:middle line:84%
is they always go through
a Amorphous Calcium

00:10:25.640 --> 00:10:27.600 align:middle line:90%
Carbonate or ACC.

00:10:27.600 --> 00:10:30.840 align:middle line:84%
This is one of the transient
amorphous precursors

00:10:30.840 --> 00:10:32.520 align:middle line:90%
we're going to be talking about.

00:10:32.520 --> 00:10:35.280 align:middle line:84%
Now, this is a very
common strategy

00:10:35.280 --> 00:10:37.200 align:middle line:90%
for this kind of organisms.

00:10:37.200 --> 00:10:39.857 align:middle line:84%
In biomineralization,
they almost always

00:10:39.857 --> 00:10:41.440 align:middle line:84%
go through amorphous
phase before they

00:10:41.440 --> 00:10:42.640 align:middle line:90%
go to crystalline phase.

00:10:42.640 --> 00:10:44.960 align:middle line:84%
There are a few
reasons for that.

00:10:44.960 --> 00:10:49.430 align:middle line:84%
From a genetic perspective,
the amorphous structure

00:10:49.430 --> 00:10:53.150 align:middle line:84%
may look a lot similar
to the liquid phase that

00:10:53.150 --> 00:10:54.790 align:middle line:90%
come from solution.

00:10:54.790 --> 00:10:57.470 align:middle line:84%
So this structural
similarity, what it also means

00:10:57.470 --> 00:11:00.510 align:middle line:84%
is that the interface energy
between the amorphous phase

00:11:00.510 --> 00:11:03.350 align:middle line:84%
and the solution phase tends
to be a lot smaller compared

00:11:03.350 --> 00:11:06.710 align:middle line:84%
to the crystalline phase
and the solution phase.

00:11:06.710 --> 00:11:08.910 align:middle line:84%
So lower interface
energy essentially

00:11:08.910 --> 00:11:12.310 align:middle line:84%
means there's a lower energy
barrier to nucleation.

00:11:12.310 --> 00:11:16.690 align:middle line:84%
So kinetically, it can be more
favorable to form the ACC first,

00:11:16.690 --> 00:11:20.740 align:middle line:84%
and then go to
crystalline phase.

00:11:20.740 --> 00:11:24.430 align:middle line:84%
Also, we'll be talking about
this process a little bit more

00:11:24.430 --> 00:11:25.510 align:middle line:90%
later.

00:11:25.510 --> 00:11:28.520 align:middle line:84%
But typically, when they
actually precipitate out

00:11:28.520 --> 00:11:30.270 align:middle line:84%
this kind of amorphous
phase, it comes out

00:11:30.270 --> 00:11:35.350 align:middle line:84%
in the form of very small
clusters, nanoscale clusters.

00:11:35.350 --> 00:11:37.870 align:middle line:84%
So these nanoscale
amorphous clusters,

00:11:37.870 --> 00:11:39.650 align:middle line:84%
they reside in the
solution phase.

00:11:39.650 --> 00:11:42.530 align:middle line:84%
So it's basically like a liquid
with these amorphous clusters.

00:11:42.530 --> 00:11:46.270 align:middle line:84%
It's very easy for this phase
to essentially infiltrate

00:11:46.270 --> 00:11:52.030 align:middle line:84%
into usually the porous
structure of organic scaffold.

00:11:52.030 --> 00:11:54.270 align:middle line:84%
And then these little
part of clusters

00:11:54.270 --> 00:11:56.470 align:middle line:90%
then attach to the scaffold.

00:11:56.470 --> 00:11:59.330 align:middle line:84%
And this will be a
pretty quick process.

00:11:59.330 --> 00:12:02.650 align:middle line:84%
This kind of infiltration
and precipitation,

00:12:02.650 --> 00:12:06.030 align:middle line:84%
it can take place within
a few seconds to minutes.

00:12:06.030 --> 00:12:08.630 align:middle line:84%
And this is actually
advantageous

00:12:08.630 --> 00:12:12.310 align:middle line:84%
because, in lots of cases,
the organisms, or the animal,

00:12:12.310 --> 00:12:14.990 align:middle line:84%
basically, want to
have essentially

00:12:14.990 --> 00:12:17.218 align:middle line:84%
the biomineralized
products quickly

00:12:17.218 --> 00:12:19.010 align:middle line:84%
to adapt to different
kind of environments.

00:12:19.010 --> 00:12:20.910 align:middle line:84%
We are going to talk
about crustaceans.

00:12:20.910 --> 00:12:23.030 align:middle line:84%
For example, crustaceans,
when they molt,

00:12:23.030 --> 00:12:25.570 align:middle line:84%
they essentially shed their
old shell, put on a new one.

00:12:25.570 --> 00:12:28.310 align:middle line:84%
They need to have that
new shell quickly,

00:12:28.310 --> 00:12:30.910 align:middle line:84%
within a matter of
days, a couple of days,

00:12:30.910 --> 00:12:33.110 align:middle line:84%
or even shorter, just
to protect themselves.

00:12:33.110 --> 00:12:35.970 align:middle line:84%
So having this amorphous phase
is actually very convenient.

00:12:35.970 --> 00:12:37.990 align:middle line:84%
This allows this
very fast deposition

00:12:37.990 --> 00:12:42.190 align:middle line:84%
of the amorphous materials to
form essentially the prototype

00:12:42.190 --> 00:12:43.750 align:middle line:90%
of the shell.

00:12:43.750 --> 00:12:46.910 align:middle line:84%
And then after that, the
actual phase transformation,

00:12:46.910 --> 00:12:48.450 align:middle line:84%
going from amorphous
crystalline,

00:12:48.450 --> 00:12:50.390 align:middle line:84%
this tend to be
a slower process.

00:12:50.390 --> 00:12:52.670 align:middle line:90%
This can take hours or days.

00:12:52.670 --> 00:12:55.950 align:middle line:84%
And in the process, the
kinetics is basically

00:12:55.950 --> 00:12:58.590 align:middle line:84%
controlled by a lot of
the organic molecules.

00:12:58.590 --> 00:13:00.750 align:middle line:84%
They're called inhibitory
organic molecules.

00:13:00.750 --> 00:13:03.570 align:middle line:84%
They essentially suppress
the crystallization

00:13:03.570 --> 00:13:07.190 align:middle line:84%
so that the animal
can actually control

00:13:07.190 --> 00:13:09.790 align:middle line:84%
what is the kinetics of
the phase transformation.

00:13:09.790 --> 00:13:12.870 align:middle line:84%
And that's actually useful
because, in lots of cases,

00:13:12.870 --> 00:13:15.470 align:middle line:84%
in order to form this kind of
hierarchical microstructure,

00:13:15.470 --> 00:13:17.830 align:middle line:84%
the organic template
will then dictate

00:13:17.830 --> 00:13:20.550 align:middle line:84%
what is the orientation and
alignment of the resulting

00:13:20.550 --> 00:13:21.950 align:middle line:90%
crystals.

00:13:21.950 --> 00:13:24.950 align:middle line:84%
If you do that very
quickly-- from kinetics,

00:13:24.950 --> 00:13:27.710 align:middle line:84%
you know that it becomes very
difficult to actually control

00:13:27.710 --> 00:13:30.678 align:middle line:84%
the orientation of
those crystals--

00:13:30.678 --> 00:13:32.970 align:middle line:84%
essentially, you get a lot
of random atomic attachment.

00:13:32.970 --> 00:13:34.990 align:middle line:84%
You get highly
polycrystalline solids

00:13:34.990 --> 00:13:36.830 align:middle line:84%
with a random
orientation of grains.

00:13:36.830 --> 00:13:40.390 align:middle line:84%
It's sort of like
growing microepitaxy.

00:13:40.390 --> 00:13:42.800 align:middle line:84%
In order to get to this kind
of microepitaxy process,

00:13:42.800 --> 00:13:44.500 align:middle line:84%
you need to control the
atomic detachment, the phase

00:13:44.500 --> 00:13:46.417 align:middle line:84%
transformation, so that
it doesn't go too fast

00:13:46.417 --> 00:13:47.860 align:middle line:90%
and screw up everything.

00:13:47.860 --> 00:13:50.793 align:middle line:84%
So that's why having this
kind of amorphous phase

00:13:50.793 --> 00:13:51.960 align:middle line:90%
is actually quite important.

00:13:51.960 --> 00:13:56.060 align:middle line:84%
And controlling the kinetics
of its precipitation and growth

00:13:56.060 --> 00:13:57.200 align:middle line:90%
is also quite important.

00:13:57.200 --> 00:13:59.785 align:middle line:90%


00:13:59.785 --> 00:14:01.160 align:middle line:84%
So this is basically
one example.

00:14:01.160 --> 00:14:04.060 align:middle line:84%
We're going to see that
in other cases as well.

00:14:04.060 --> 00:14:06.000 align:middle line:84%
So the second example
I'm going to talk about,

00:14:06.000 --> 00:14:09.880 align:middle line:84%
these are the exoskeleton
of crustaceans.

00:14:09.880 --> 00:14:13.660 align:middle line:84%
So I'm talking about basically
crabs, shrimps, lobsters,

00:14:13.660 --> 00:14:16.460 align:middle line:90%
crayfish.

00:14:16.460 --> 00:14:18.020 align:middle line:90%
In terms of composition--

00:14:18.020 --> 00:14:20.460 align:middle line:84%
oh, by the way, I forgot
one thing about the chemical

00:14:20.460 --> 00:14:21.200 align:middle line:90%
reaction here.

00:14:21.200 --> 00:14:22.260 align:middle line:90%
I should mention this.

00:14:22.260 --> 00:14:25.820 align:middle line:84%
This is a chemical reaction
for the seashells' formation.

00:14:25.820 --> 00:14:28.700 align:middle line:84%
Basically, the mollusks,
they were taking calcium

00:14:28.700 --> 00:14:29.960 align:middle line:90%
from the ocean.

00:14:29.960 --> 00:14:33.300 align:middle line:84%
There's actually lots of calcium
in the dissolved solution

00:14:33.300 --> 00:14:34.360 align:middle line:90%
form in the seawater.

00:14:34.360 --> 00:14:39.620 align:middle line:84%
They're also taking
this ion here, HCO3.

00:14:39.620 --> 00:14:43.100 align:middle line:84%
It basically come from dissolved
carbon dioxide in seawater.

00:14:43.100 --> 00:14:47.300 align:middle line:84%
Then they can react, form
the ACC, precipitate out,

00:14:47.300 --> 00:14:50.540 align:middle line:84%
and that's how you actually
form the seashell materials.

00:14:50.540 --> 00:14:53.860 align:middle line:84%
It's actually a very
similar chemical reaction

00:14:53.860 --> 00:14:59.915 align:middle line:84%
when it also comes to
the crustaceans that

00:14:59.915 --> 00:15:01.040 align:middle line:90%
actually live in the ocean.

00:15:01.040 --> 00:15:04.780 align:middle line:84%
They basically use the same
kind of chemical reaction.

00:15:04.780 --> 00:15:07.680 align:middle line:84%
So in terms of composition
of the exoskeleton,

00:15:07.680 --> 00:15:10.540 align:middle line:84%
it's also quite
similar to seashells.

00:15:10.540 --> 00:15:13.240 align:middle line:84%
You similarly have chitin,
the polysaccharides.

00:15:13.240 --> 00:15:14.300 align:middle line:90%
You get some proteins.

00:15:14.300 --> 00:15:15.520 align:middle line:90%
You get minerals.

00:15:15.520 --> 00:15:20.180 align:middle line:84%
The minerals are
mostly ACC and calcite.

00:15:20.180 --> 00:15:22.680 align:middle line:84%
Depending on different
species, it's a mix of the two.

00:15:22.680 --> 00:15:25.220 align:middle line:90%


00:15:25.220 --> 00:15:28.260 align:middle line:84%
Now let's take a look at actual
structure of the exoskeleton.

00:15:28.260 --> 00:15:29.940 align:middle line:84%
It's one typical
example of this kind

00:15:29.940 --> 00:15:31.460 align:middle line:90%
of hierarchical architecture.

00:15:31.460 --> 00:15:34.700 align:middle line:84%
So if you look at the shell--
let's say a lobster shell--

00:15:34.700 --> 00:15:38.060 align:middle line:84%
there are actually multiple
layers of the shell.

00:15:38.060 --> 00:15:42.170 align:middle line:90%
You have so-called exocuticle.

00:15:42.170 --> 00:15:45.490 align:middle line:90%
You get the smaller ones.

00:15:45.490 --> 00:15:47.670 align:middle line:84%
The outer layer is
called epicuticle.

00:15:47.670 --> 00:15:50.370 align:middle line:84%
It's basically a layer that has
essentially a wax-like feeling

00:15:50.370 --> 00:15:51.490 align:middle line:90%
on the surface.

00:15:51.490 --> 00:15:52.850 align:middle line:90%
And then you get exocuticle.

00:15:52.850 --> 00:15:54.330 align:middle line:90%
And then you get endocuticle.

00:15:54.330 --> 00:15:55.550 align:middle line:90%
So different layers there.

00:15:55.550 --> 00:15:58.690 align:middle line:84%
Now if you look closely into
the microstructure there,

00:15:58.690 --> 00:16:01.090 align:middle line:84%
they all consist of
essentially these kind

00:16:01.090 --> 00:16:04.970 align:middle line:90%
of basically little fibers.

00:16:04.970 --> 00:16:06.950 align:middle line:84%
The fibers are essentially
made of chitin,

00:16:06.950 --> 00:16:09.270 align:middle line:84%
but it's a chitin that's
heavily mineralized.

00:16:09.270 --> 00:16:13.010 align:middle line:84%
So chitin decorated
with calcite crystals.

00:16:13.010 --> 00:16:17.610 align:middle line:84%
So these fibers, if you look at
how they're actually arranged,

00:16:17.610 --> 00:16:20.170 align:middle line:84%
they form this kind of
a multilayer structure

00:16:20.170 --> 00:16:20.998 align:middle line:90%
between the layers.

00:16:20.998 --> 00:16:23.290 align:middle line:84%
The orientation of fibers
actually rotated with respect

00:16:23.290 --> 00:16:25.150 align:middle line:90%
to each other.

00:16:25.150 --> 00:16:30.285 align:middle line:84%
People call this helicoidal
Bouligand stacking.

00:16:30.285 --> 00:16:31.910 align:middle line:84%
I don't know where
the name comes from,

00:16:31.910 --> 00:16:35.090 align:middle line:84%
but basically, this actually has
a pretty important implication

00:16:35.090 --> 00:16:36.190 align:middle line:90%
of mechanical properties.

00:16:36.190 --> 00:16:39.528 align:middle line:84%
The reason you have
different orientations here,

00:16:39.528 --> 00:16:41.570 align:middle line:84%
one is that suppose there's
some cracks developed

00:16:41.570 --> 00:16:42.470 align:middle line:90%
in one of the layers.

00:16:42.470 --> 00:16:45.765 align:middle line:84%
Then, because of the
rotation of the orientation

00:16:45.765 --> 00:16:47.390 align:middle line:84%
of the fibers between
different layers,

00:16:47.390 --> 00:16:48.930 align:middle line:84%
it means that when
the crack tries

00:16:48.930 --> 00:16:52.370 align:middle line:84%
to propagate between layers,
it also has to rotate,

00:16:52.370 --> 00:16:54.810 align:middle line:84%
change orientation,
and then essentially

00:16:54.810 --> 00:16:57.450 align:middle line:84%
also have to branch out
in the process there.

00:16:57.450 --> 00:16:59.670 align:middle line:84%
So because of this
kind of configuration,

00:16:59.670 --> 00:17:01.810 align:middle line:84%
it means that as the
crack propagates,

00:17:01.810 --> 00:17:04.650 align:middle line:84%
the area of the
cracked surface has

00:17:04.650 --> 00:17:07.730 align:middle line:84%
to expand as it goes
through multiple layers.

00:17:07.730 --> 00:17:10.410 align:middle line:84%
Now that means you have to
overcome more surface energy

00:17:10.410 --> 00:17:11.450 align:middle line:90%
barrier.

00:17:11.450 --> 00:17:14.930 align:middle line:84%
So it effectively helps you
to absorb a lot of the energy.

00:17:14.930 --> 00:17:18.970 align:middle line:84%
And absorbing energy corresponds
to an enhanced toughness

00:17:18.970 --> 00:17:21.530 align:middle line:90%
of the material.

00:17:21.530 --> 00:17:24.682 align:middle line:84%
Also, if you just look at
the chitin fiber by itself,

00:17:24.682 --> 00:17:26.849 align:middle line:84%
it obviously has this kind
of anisotropic mechanical

00:17:26.849 --> 00:17:29.490 align:middle line:84%
properties-- stronger along
the direction and then weaker

00:17:29.490 --> 00:17:31.110 align:middle line:90%
in the parallel direction.

00:17:31.110 --> 00:17:33.850 align:middle line:84%
But by having this kind of
stacking with a rotating

00:17:33.850 --> 00:17:36.768 align:middle line:84%
orientation, it also eventually
creates isotropic material

00:17:36.768 --> 00:17:39.060 align:middle line:84%
that has uniform properties
along different directions,

00:17:39.060 --> 00:17:40.720 align:middle line:90%
which will be useful.

00:17:40.720 --> 00:17:43.800 align:middle line:84%
And finally, the
mixture of organic phase

00:17:43.800 --> 00:17:46.560 align:middle line:84%
in the organic phase is also
what made the shells actually

00:17:46.560 --> 00:17:49.380 align:middle line:84%
highly flexible, despite the
fact that it's made of calcite,

00:17:49.380 --> 00:17:51.080 align:middle line:90%
which is a pretty hard mineral.

00:17:51.080 --> 00:17:54.520 align:middle line:84%
Now, one thing I
have also found out

00:17:54.520 --> 00:17:56.480 align:middle line:84%
while I was looking
for the information

00:17:56.480 --> 00:17:59.500 align:middle line:84%
about crustacean
exoskeleton formation

00:17:59.500 --> 00:18:00.980 align:middle line:90%
is the process called molting.

00:18:00.980 --> 00:18:04.060 align:middle line:84%
So molting just means
that, for example,

00:18:04.060 --> 00:18:06.880 align:middle line:84%
crabs, as they grow bigger, they
need to essentially shed away

00:18:06.880 --> 00:18:09.380 align:middle line:84%
the old shell and
actually put on a new one

00:18:09.380 --> 00:18:12.520 align:middle line:84%
so that they can accommodate
their growing size.

00:18:12.520 --> 00:18:15.400 align:middle line:84%
In this process here, as
the crab, for example,

00:18:15.400 --> 00:18:18.600 align:middle line:84%
dumps its old shell, the old
shell contains lots of calcium.

00:18:18.600 --> 00:18:21.668 align:middle line:84%
So one priority
for the animal is

00:18:21.668 --> 00:18:23.960 align:middle line:84%
that it needs to be able to
essentially accumulate lots

00:18:23.960 --> 00:18:26.780 align:middle line:84%
of calcium and then deposit
them to form new shells,

00:18:26.780 --> 00:18:29.680 align:middle line:84%
as I said, within a short period
of time, just to protect itself.

00:18:29.680 --> 00:18:31.960 align:middle line:84%
So this comes with
the question--

00:18:31.960 --> 00:18:34.640 align:middle line:84%
how do they actually get
this large amount of calcium

00:18:34.640 --> 00:18:37.160 align:middle line:90%
within a short period of time?

00:18:37.160 --> 00:18:40.220 align:middle line:84%
For animals living in
the ocean, like lobsters,

00:18:40.220 --> 00:18:43.380 align:middle line:84%
this is much less of an
issue because, as I said,

00:18:43.380 --> 00:18:46.840 align:middle line:84%
ocean water, seawater, actually
has a high concentration

00:18:46.840 --> 00:18:48.100 align:middle line:90%
of calcium in itself.

00:18:48.100 --> 00:18:50.360 align:middle line:84%
So it's easier for
them to get it right.

00:18:50.360 --> 00:18:53.940 align:middle line:84%
But for terrestrial and
freshwater crustaceans,

00:18:53.940 --> 00:18:56.920 align:middle line:84%
for example, like
crayfish, it does not

00:18:56.920 --> 00:18:59.120 align:middle line:84%
have access to
this huge reservoir

00:18:59.120 --> 00:19:01.360 align:middle line:90%
of solution-phase calcium ion.

00:19:01.360 --> 00:19:06.320 align:middle line:84%
So what they would do is, in
fact, before they actually molt,

00:19:06.320 --> 00:19:10.200 align:middle line:84%
they will start to reabsorb
calcium in the exoskeleton

00:19:10.200 --> 00:19:13.440 align:middle line:84%
before they actually
molt. And in that process,

00:19:13.440 --> 00:19:15.300 align:middle line:84%
they have to store
the calcium somewhere.

00:19:15.300 --> 00:19:19.680 align:middle line:84%
So they store it in the form
of a so-called gastrolith.

00:19:19.680 --> 00:19:22.500 align:middle line:90%
Have you heard of the term?

00:19:22.500 --> 00:19:25.560 align:middle line:84%
It's basically like little
stones, technically.

00:19:25.560 --> 00:19:29.600 align:middle line:84%
They form little stones
in their stomach.

00:19:29.600 --> 00:19:32.135 align:middle line:84%
I don't know if you
have eaten crayfish.

00:19:32.135 --> 00:19:32.760 align:middle line:90%
AUDIENCE: Yeah.

00:19:32.760 --> 00:19:33.343 align:middle line:90%
JUEJUN HU: OK.

00:19:33.343 --> 00:19:34.715 align:middle line:90%
AUDIENCE: Do I eat the stones?

00:19:34.715 --> 00:19:35.590 align:middle line:90%
JUEJUN HU: Sometimes.

00:19:35.590 --> 00:19:36.673 align:middle line:90%
Only sometimes you see it.

00:19:36.673 --> 00:19:39.820 align:middle line:84%
It's right before they molt
you get those kind of stones.

00:19:39.820 --> 00:19:42.240 align:middle line:84%
So the stomach of
crayfish is actually

00:19:42.240 --> 00:19:43.300 align:middle line:90%
very close to their head.

00:19:43.300 --> 00:19:46.328 align:middle line:84%
It's right behind their head,
which you don't eat the head.

00:19:46.328 --> 00:19:48.620 align:middle line:84%
But you may find stones in
there if you look carefully.

00:19:48.620 --> 00:19:50.820 align:middle line:84%
The stones can get
actually pretty big.

00:19:50.820 --> 00:19:51.852 align:middle line:90%
You see the size here.

00:19:51.852 --> 00:19:54.060 align:middle line:84%
This is actually-- sorry,
they're scaled a bit small.

00:19:54.060 --> 00:19:55.360 align:middle line:90%
This is 5 millimeters.

00:19:55.360 --> 00:19:58.400 align:middle line:90%
So they can be this big.

00:19:58.400 --> 00:19:59.280 align:middle line:90%
Yeah.

00:19:59.280 --> 00:20:04.120 align:middle line:84%
And they primarily consist
of ACC, Amorphous Calcium

00:20:04.120 --> 00:20:05.960 align:middle line:90%
Carbonate.

00:20:05.960 --> 00:20:08.700 align:middle line:84%
Now the reason they put in
ACC is because, as I said,

00:20:08.700 --> 00:20:12.467 align:middle line:84%
ACC is easy to deposit
from the solution phase.

00:20:12.467 --> 00:20:14.800 align:middle line:84%
And when they need to return
it into the solution phase,

00:20:14.800 --> 00:20:18.280 align:middle line:84%
to return it to a body fluid
to build the exoskeleton,

00:20:18.280 --> 00:20:22.720 align:middle line:84%
the dissolution process can also
be very efficient and very fast.

00:20:22.720 --> 00:20:24.866 align:middle line:84%
So they essentially use
this amorphous phase sort

00:20:24.866 --> 00:20:28.800 align:middle line:84%
of as a reservoir
that's easily accessible

00:20:28.800 --> 00:20:30.920 align:middle line:84%
and can be expediently
transformed

00:20:30.920 --> 00:20:32.988 align:middle line:84%
into the calcium
in the body fluid.

00:20:32.988 --> 00:20:35.530 align:middle line:84%
Then they can transport it to
actually build the exoskeleton.

00:20:35.530 --> 00:20:38.510 align:middle line:90%


00:20:38.510 --> 00:20:43.527 align:middle line:84%
So essentially,
this is a diagram

00:20:43.527 --> 00:20:45.110 align:middle line:84%
that actually shows
the microstructure

00:20:45.110 --> 00:20:46.742 align:middle line:90%
of this exoskeleton.

00:20:46.742 --> 00:20:48.950 align:middle line:84%
This is what it looks like
in terms of cross-section.

00:20:48.950 --> 00:20:52.070 align:middle line:84%
And this last one
here, this panel,

00:20:52.070 --> 00:20:56.250 align:middle line:84%
shows the microstructure after
you etch away the ACC phase.

00:20:56.250 --> 00:21:00.590 align:middle line:84%
So what's left behind here is
basically the organic scaffold.

00:21:00.590 --> 00:21:02.630 align:middle line:84%
So it's basically
an organic scaffold

00:21:02.630 --> 00:21:06.750 align:middle line:84%
with lots of ACC essentially
infiltrated in there.

00:21:06.750 --> 00:21:08.550 align:middle line:84%
This is how these
animals actually

00:21:08.550 --> 00:21:11.390 align:middle line:84%
were able to very quickly
build the exoskeleton,

00:21:11.390 --> 00:21:12.630 align:middle line:90%
with this kind of storage.

00:21:12.630 --> 00:21:15.510 align:middle line:84%
AUDIENCE: And they're taking
it from their environment

00:21:15.510 --> 00:21:17.590 align:middle line:90%
or they're already--

00:21:17.590 --> 00:21:18.850 align:middle line:90%
JUEJUN HU: Well, both.

00:21:18.850 --> 00:21:20.190 align:middle line:84%
They essentially
accumulate it essentially

00:21:20.190 --> 00:21:21.065 align:middle line:90%
from the environment.

00:21:21.065 --> 00:21:22.538 align:middle line:84%
That's kind of the
primary source.

00:21:22.538 --> 00:21:23.330 align:middle line:90%
They have to do it.

00:21:23.330 --> 00:21:25.430 align:middle line:84%
But then, as I said,
before they molt,

00:21:25.430 --> 00:21:29.123 align:middle line:84%
they also reabsorb the calcium
from their own exoskeleton.

00:21:29.123 --> 00:21:30.123 align:middle line:90%
AUDIENCE: Kind of like--

00:21:30.123 --> 00:21:31.270 align:middle line:90%
OK.

00:21:31.270 --> 00:21:32.270 align:middle line:90%
JUEJUN HU: Yeah.

00:21:32.270 --> 00:21:34.190 align:middle line:90%
That's actually what they do.

00:21:34.190 --> 00:21:37.070 align:middle line:84%
And so that essentially
minimizes the calcium loss

00:21:37.070 --> 00:21:39.670 align:middle line:84%
when they actually molt.
So they recycle it.

00:21:39.670 --> 00:21:42.150 align:middle line:84%
But you only see the
gastrolith, as I said,

00:21:42.150 --> 00:21:45.070 align:middle line:84%
in terrestrial or
freshwater crustaceans.

00:21:45.070 --> 00:21:46.410 align:middle line:90%
You don't see that in lobsters.

00:21:46.410 --> 00:21:48.590 align:middle line:84%
You never see in lobsters
because they have lots

00:21:48.590 --> 00:21:50.390 align:middle line:90%
of calcium at their disposal.

00:21:50.390 --> 00:21:52.930 align:middle line:90%


00:21:52.930 --> 00:21:54.990 align:middle line:84%
So next time, if
you try crayfish,

00:21:54.990 --> 00:21:57.490 align:middle line:84%
look out for this
kind of a gastrolith.

00:21:57.490 --> 00:22:00.150 align:middle line:90%


00:22:00.150 --> 00:22:00.990 align:middle line:90%
All right.

00:22:00.990 --> 00:22:06.230 align:middle line:84%
Now let's come back and
talk about ourselves.

00:22:06.230 --> 00:22:10.070 align:middle line:84%
So vertebrates like
us also always go

00:22:10.070 --> 00:22:11.710 align:middle line:84%
through a
biomineralization process

00:22:11.710 --> 00:22:14.290 align:middle line:90%
in order to form bone and teeth.

00:22:14.290 --> 00:22:17.710 align:middle line:84%
Now, for bone and
teeth, one thing

00:22:17.710 --> 00:22:19.390 align:middle line:84%
that's quite different
from seashells

00:22:19.390 --> 00:22:21.170 align:middle line:84%
is their composition
is different.

00:22:21.170 --> 00:22:23.490 align:middle line:84%
We do not rely on
calcium carbonate.

00:22:23.490 --> 00:22:27.630 align:middle line:84%
We rely on a different kind
of mineral, essentially

00:22:27.630 --> 00:22:29.820 align:middle line:90%
a calcium phosphate.

00:22:29.820 --> 00:22:31.380 align:middle line:90%
That's the main difference.

00:22:31.380 --> 00:22:34.520 align:middle line:84%
So if you look closely into
either the bone or teeth,

00:22:34.520 --> 00:22:36.523 align:middle line:90%
they have similar compositions.

00:22:36.523 --> 00:22:38.440 align:middle line:84%
They always consist of
three different phases.

00:22:38.440 --> 00:22:41.620 align:middle line:84%
Here you have a mineral phase,
which is basically taking

00:22:41.620 --> 00:22:44.200 align:middle line:90%
the form of hydroxyapatite.

00:22:44.200 --> 00:22:50.140 align:middle line:84%
Essentially, it's a hydrolyzed
form of calcium phosphate.

00:22:50.140 --> 00:22:53.100 align:middle line:84%
You then also have
an organic matrix.

00:22:53.100 --> 00:22:58.260 align:middle line:84%
Now, mainly, it's
actually collagen.

00:22:58.260 --> 00:23:00.622 align:middle line:90%
And some proteins, of course.

00:23:00.622 --> 00:23:02.080 align:middle line:84%
And then finally,
some water phase.

00:23:02.080 --> 00:23:04.538 align:middle line:84%
The water phase is basically
just to provide the hydration.

00:23:04.538 --> 00:23:07.100 align:middle line:84%
So the specific
composition really

00:23:07.100 --> 00:23:09.020 align:middle line:84%
depends on the specific
kind of tissue there.

00:23:09.020 --> 00:23:11.300 align:middle line:84%
If you're talking about
bone, you typically

00:23:11.300 --> 00:23:14.380 align:middle line:84%
have anywhere from 50% to
60% of the mineral phase

00:23:14.380 --> 00:23:16.860 align:middle line:84%
and then maybe 20% to 30%
organic phase, the rest

00:23:16.860 --> 00:23:18.880 align:middle line:90%
being the solution phase.

00:23:18.880 --> 00:23:26.060 align:middle line:84%
If it's dentin, which is
basically the core of the teeth,

00:23:26.060 --> 00:23:29.280 align:middle line:84%
dentin has about 70% mineral,
maybe 20% organic phase.

00:23:29.280 --> 00:23:30.380 align:middle line:90%
So it's more like bone.

00:23:30.380 --> 00:23:32.620 align:middle line:84%
But for the surface
layer of teeth,

00:23:32.620 --> 00:23:36.660 align:middle line:84%
which is the white outside,
the white shiny piece,

00:23:36.660 --> 00:23:38.820 align:middle line:90%
that's called the enamel.

00:23:38.820 --> 00:23:41.760 align:middle line:84%
The enamel is pretty much
just the mineral phase.

00:23:41.760 --> 00:23:43.440 align:middle line:90%
It's a very dense mineral phase.

00:23:43.440 --> 00:23:47.080 align:middle line:84%
It's about 95%
calcium phosphate.

00:23:47.080 --> 00:23:50.383 align:middle line:84%
And then just a little
bit of organic proteins.

00:23:50.383 --> 00:23:52.300 align:middle line:84%
So the composition also
depends on what tissue

00:23:52.300 --> 00:23:53.180 align:middle line:90%
you're looking for.

00:23:53.180 --> 00:23:58.675 align:middle line:84%
Now enamel is actually quite an
interesting part of the tissue

00:23:58.675 --> 00:24:00.300 align:middle line:84%
that I actually want
to talk a bit more

00:24:00.300 --> 00:24:01.842 align:middle line:90%
about in subsequent slides.

00:24:01.842 --> 00:24:03.300 align:middle line:84%
If you look at
enamel here, it also

00:24:03.300 --> 00:24:05.540 align:middle line:84%
has this kind of hierarchical
architecture here.

00:24:05.540 --> 00:24:09.100 align:middle line:84%
It actually consists of tiny
little rods called enamel rods.

00:24:09.100 --> 00:24:13.780 align:middle line:84%
And enamel rods basically
consists of mineralized collagen

00:24:13.780 --> 00:24:16.000 align:middle line:90%
fibers.

00:24:16.000 --> 00:24:18.560 align:middle line:84%
They stack together in a regular
array to form the enamel.

00:24:18.560 --> 00:24:19.600 align:middle line:84%
If you look at it
under a microscope,

00:24:19.600 --> 00:24:21.892 align:middle line:84%
you see these tiny little
rods arranged in more or less

00:24:21.892 --> 00:24:22.920 align:middle line:90%
a hexagonal lattice.

00:24:22.920 --> 00:24:25.920 align:middle line:90%


00:24:25.920 --> 00:24:29.410 align:middle line:90%
Now, how are those formed?

00:24:29.410 --> 00:24:33.610 align:middle line:84%
How do we humans, for example,
form these kind of minerals?

00:24:33.610 --> 00:24:36.610 align:middle line:90%
Again, amorphous phase.

00:24:36.610 --> 00:24:38.190 align:middle line:90%
We still use the precursor.

00:24:38.190 --> 00:24:41.590 align:middle line:84%
In this case, it's Amorphous
Calcium Phosphate, or ACP.

00:24:41.590 --> 00:24:44.110 align:middle line:90%


00:24:44.110 --> 00:24:47.890 align:middle line:84%
Now, the reason ACP is
used is very similar to why

00:24:47.890 --> 00:24:50.290 align:middle line:90%
other animals use ACC.

00:24:50.290 --> 00:24:52.570 align:middle line:84%
It reduces also
interfacial energy.

00:24:52.570 --> 00:24:54.810 align:middle line:84%
It also provides the
shape flexibility

00:24:54.810 --> 00:24:57.530 align:middle line:84%
because, again, these kind of
little clusters in the solution

00:24:57.530 --> 00:25:00.810 align:middle line:84%
phase can very easily infiltrate
into the tissues, bone tissues,

00:25:00.810 --> 00:25:03.210 align:middle line:84%
precipitate on them,
and eventually transform

00:25:03.210 --> 00:25:08.170 align:middle line:84%
into the crystalline
form of hydroxyapatite.

00:25:08.170 --> 00:25:13.410 align:middle line:84%
So one example of a
mineralization process

00:25:13.410 --> 00:25:16.210 align:middle line:84%
that's actually
actively ongoing, even

00:25:16.210 --> 00:25:19.703 align:middle line:84%
after you form the bone
and teeth, is the enamel.

00:25:19.703 --> 00:25:21.870 align:middle line:84%
Because enamel is actually
a surface layer of teeth,

00:25:21.870 --> 00:25:24.370 align:middle line:84%
it's always in interaction
with the microenvironment

00:25:24.370 --> 00:25:25.810 align:middle line:90%
in the mouth.

00:25:25.810 --> 00:25:31.470 align:middle line:84%
So for example, if you eat some
sugary food which feed bacteria,

00:25:31.470 --> 00:25:34.570 align:middle line:84%
the bacteria's metabolic
products tend to be acidic,

00:25:34.570 --> 00:25:37.878 align:middle line:84%
or you drink lemon juice or
whatever, that's also acidic,

00:25:37.878 --> 00:25:40.170 align:middle line:84%
then it can actually push
the chemical equilibrium goes

00:25:40.170 --> 00:25:41.070 align:middle line:90%
the other way around.

00:25:41.070 --> 00:25:44.450 align:middle line:84%
You start to cause dissolution
of the hydroxyapatite

00:25:44.450 --> 00:25:45.910 align:middle line:90%
or the enamel layer.

00:25:45.910 --> 00:25:47.310 align:middle line:90%
Go back into the saliva.

00:25:47.310 --> 00:25:49.110 align:middle line:84%
So essentially you lose
the mineralization.

00:25:49.110 --> 00:25:50.970 align:middle line:84%
That's how you actually
damage the teeth.

00:25:50.970 --> 00:25:54.210 align:middle line:84%
You can actually also
reverse the process

00:25:54.210 --> 00:25:56.530 align:middle line:84%
by going to a more
basic solution.

00:25:56.530 --> 00:25:59.770 align:middle line:84%
And you supply it with
sufficient amount of calcium ion

00:25:59.770 --> 00:26:01.750 align:middle line:90%
as well as the phosphate ion.

00:26:01.750 --> 00:26:03.450 align:middle line:84%
If you do that,
they can actually

00:26:03.450 --> 00:26:05.650 align:middle line:84%
go through a so-called
remineralization process

00:26:05.650 --> 00:26:08.730 align:middle line:84%
and repair any damage
to the enamel layer.

00:26:08.730 --> 00:26:11.048 align:middle line:84%
I will go through
that later when

00:26:11.048 --> 00:26:13.590 align:middle line:84%
we talk about the applications
of this kind of process there.

00:26:13.590 --> 00:26:16.010 align:middle line:84%
But that's a
biomineralization process

00:26:16.010 --> 00:26:19.490 align:middle line:84%
that's actually reversible and
is actually ongoing always.

00:26:19.490 --> 00:26:24.070 align:middle line:90%


00:26:24.070 --> 00:26:25.715 align:middle line:90%
All right.

00:26:25.715 --> 00:26:27.090 align:middle line:84%
Now, next example,
we are talking

00:26:27.090 --> 00:26:30.970 align:middle line:84%
about different class of
minerals now, silica or glass.

00:26:30.970 --> 00:26:32.890 align:middle line:84%
So there are quite a
few different kinds

00:26:32.890 --> 00:26:37.970 align:middle line:84%
of microorganisms
that can actually

00:26:37.970 --> 00:26:41.130 align:middle line:90%
mineralize SiO2, silica.

00:26:41.130 --> 00:26:46.490 align:middle line:84%
The two most notable examples
is diatoms and glass sponge.

00:26:46.490 --> 00:26:48.870 align:middle line:84%
So you obviously
know glass sponge.

00:26:48.870 --> 00:26:51.050 align:middle line:84%
That's how you propose
the lecture topic.

00:26:51.050 --> 00:26:55.050 align:middle line:84%
Diatoms, these are essentially
single-cell plankton

00:26:55.050 --> 00:26:56.970 align:middle line:90%
that live in the ocean.

00:26:56.970 --> 00:27:02.930 align:middle line:84%
And they are able to essentially
convert the silica dissolved

00:27:02.930 --> 00:27:05.610 align:middle line:90%
in seawater into a glass.

00:27:05.610 --> 00:27:07.810 align:middle line:84%
And for diatoms, in
fact, what they will do

00:27:07.810 --> 00:27:09.830 align:middle line:84%
is, essentially,
similar to glass sponge,

00:27:09.830 --> 00:27:12.370 align:middle line:84%
they basically build the
skeleton, or basically

00:27:12.370 --> 00:27:14.890 align:middle line:84%
their houses they
live in, out of glass,

00:27:14.890 --> 00:27:16.410 align:middle line:90%
which is quite remarkable.

00:27:16.410 --> 00:27:20.210 align:middle line:84%
So I have a little
YouTube video here

00:27:20.210 --> 00:27:22.550 align:middle line:84%
that essentially discusses
about this process.

00:27:22.550 --> 00:27:25.216 align:middle line:90%
So let me see.

00:27:25.216 --> 00:27:27.320 align:middle line:90%
[VIDEO PLAYBACK]

00:27:27.320 --> 00:27:30.600 align:middle line:84%
- The odds are high that
you'll run into a diatom.

00:27:30.600 --> 00:27:33.760 align:middle line:84%
They're both abundant and easy
to spot because of the shells

00:27:33.760 --> 00:27:36.120 align:middle line:90%
they encase themselves in.

00:27:36.120 --> 00:27:39.000 align:middle line:84%
The results are
beautiful, exacting

00:27:39.000 --> 00:27:46.560 align:middle line:84%
geometries that create a living
kaleidoscope in the microcosmos.

00:27:46.560 --> 00:27:49.760 align:middle line:84%
And even if you lived
your entire life

00:27:49.760 --> 00:27:54.160 align:middle line:84%
without ever seeing a diatom,
without ever hearing the word

00:27:54.160 --> 00:27:57.080 align:middle line:84%
diatom, you would
still be living

00:27:57.080 --> 00:28:01.200 align:middle line:84%
a life that's shaped by them,
all the way down to the oxygen

00:28:01.200 --> 00:28:04.040 align:middle line:84%
you breathe, thanks
in no small part

00:28:04.040 --> 00:28:08.840 align:middle line:84%
to their outsized contribution
to the world's photosynthesis.

00:28:08.840 --> 00:28:12.320 align:middle line:84%
But what remains captivating
about diatoms is,

00:28:12.320 --> 00:28:16.000 align:middle line:84%
well, the thing that remains
even when the diatom itself

00:28:16.000 --> 00:28:17.240 align:middle line:90%
is gone--

00:28:17.240 --> 00:28:20.480 align:middle line:84%
the hard silica shell
they once lived in, also

00:28:20.480 --> 00:28:23.400 align:middle line:90%
known as the frustule.

00:28:23.400 --> 00:28:25.200 align:middle line:84%
We've talked about
frustules a bit

00:28:25.200 --> 00:28:27.400 align:middle line:84%
before and how
they've given diatoms

00:28:27.400 --> 00:28:29.600 align:middle line:90%
the nickname jewels of the sea.

00:28:29.600 --> 00:28:32.840 align:middle line:84%
And today, we're going to
dive a bit more into how

00:28:32.840 --> 00:28:38.960 align:middle line:84%
those frustules are made and
the role they play in our world.

00:28:38.960 --> 00:28:43.320 align:middle line:84%
Diatoms are the architects
of their own glass houses,

00:28:43.320 --> 00:28:47.120 align:middle line:84%
and the scale of this
project is immense.

00:28:47.120 --> 00:28:51.320 align:middle line:84%
The silica shells aren't just
a smooth, uniform exterior.

00:28:51.320 --> 00:28:54.340 align:middle line:84%
There are pores and
elongated channels,

00:28:54.340 --> 00:28:57.280 align:middle line:84%
creating ornate
microscopic patterns

00:28:57.280 --> 00:29:00.560 align:middle line:84%
that the organism
depends on to survive.

00:29:00.560 --> 00:29:04.039 align:middle line:90%
[MUSIC PLAYING]

00:29:04.039 --> 00:29:07.520 align:middle line:90%


00:29:07.520 --> 00:29:11.400 align:middle line:84%
The source of diatoms'
building blocks is geology.

00:29:11.400 --> 00:29:14.300 align:middle line:84%
As rocks and land get
weathered and eroded,

00:29:14.300 --> 00:29:16.600 align:middle line:84%
silica enters the water,
where it dissolves

00:29:16.600 --> 00:29:20.310 align:middle line:84%
into silicic acid, which can
then diffuse into the diatom

00:29:20.310 --> 00:29:22.470 align:middle line:90%
and get converted into silica.

00:29:22.470 --> 00:29:25.850 align:middle line:84%
But if diffusion isn't
bringing in enough material,

00:29:25.850 --> 00:29:29.590 align:middle line:84%
the diatoms can also rely on
silicon transporter proteins

00:29:29.590 --> 00:29:32.750 align:middle line:84%
in their membranes
to gather more.

00:29:32.750 --> 00:29:35.190 align:middle line:84%
Inside the diatom
is a special area

00:29:35.190 --> 00:29:37.830 align:middle line:84%
called the silica
deposition vesicle,

00:29:37.830 --> 00:29:40.710 align:middle line:84%
and it's there that the silica
bits get linked together

00:29:40.710 --> 00:29:43.950 align:middle line:84%
to form bigger
and bigger pieces.

00:29:43.950 --> 00:29:46.830 align:middle line:84%
But while we know that this
is where the silica walls get

00:29:46.830 --> 00:29:49.550 align:middle line:84%
put together, the
chemistry and biology

00:29:49.550 --> 00:29:53.230 align:middle line:84%
of how they get put
together is still unclear.

00:29:53.230 --> 00:29:56.611 align:middle line:90%
[MUSIC PLAYING]

00:29:56.611 --> 00:30:04.830 align:middle line:90%


00:30:04.830 --> 00:30:08.610 align:middle line:84%
We know that the silica can
itself form a gel-like network,

00:30:08.610 --> 00:30:11.630 align:middle line:84%
so that could make up
a key assembly step.

00:30:11.630 --> 00:30:14.490 align:middle line:84%
But there may also be
other organic molecules,

00:30:14.490 --> 00:30:17.110 align:middle line:84%
like proteins, that bind
to the silica and help

00:30:17.110 --> 00:30:19.990 align:middle line:90%
create the final structure.

00:30:19.990 --> 00:30:23.650 align:middle line:84%
While scientists are still
untangling those mechanisms,

00:30:23.650 --> 00:30:26.270 align:middle line:84%
they have observed the way
that the silica deposition

00:30:26.270 --> 00:30:28.970 align:middle line:84%
vesicle and other
structures in the cell,

00:30:28.970 --> 00:30:31.270 align:middle line:84%
including the
mitochondria, can help

00:30:31.270 --> 00:30:36.390 align:middle line:84%
to mold the shape of the
final silica structure.

00:30:36.390 --> 00:30:39.570 align:middle line:84%
For example, elongated
symmetric diatoms,

00:30:39.570 --> 00:30:41.910 align:middle line:84%
also called pennate
diatoms, often

00:30:41.910 --> 00:30:44.030 align:middle line:90%
have a slit called the raphe.

00:30:44.030 --> 00:30:46.770 align:middle line:84%
The slit helps the
diatom move around,

00:30:46.770 --> 00:30:49.590 align:middle line:84%
serving as an opening through
which they can secrete

00:30:49.590 --> 00:30:53.070 align:middle line:90%
a viscous fluid to glide on.

00:30:53.070 --> 00:30:56.733 align:middle line:84%
And one of the ways that diatoms
make the raphe is by physically

00:30:56.733 --> 00:30:58.150 align:middle line:84%
molding it through
the arrangement

00:30:58.150 --> 00:31:00.350 align:middle line:90%
of their microtubules.

00:31:00.350 --> 00:31:03.612 align:middle line:90%
[MUSIC PLAYING]

00:31:03.612 --> 00:31:05.950 align:middle line:90%


00:31:05.950 --> 00:31:10.790 align:middle line:84%
Many diatoms are non-motile,
meaning they don't move around,

00:31:10.790 --> 00:31:13.870 align:middle line:84%
and the lack of visible
movement from the outside

00:31:13.870 --> 00:31:16.230 align:middle line:84%
is striking when
you consider all

00:31:16.230 --> 00:31:19.550 align:middle line:84%
of the activity that has
gone on inside of them

00:31:19.550 --> 00:31:23.430 align:middle line:90%
to make those frustules happen.

00:31:23.430 --> 00:31:25.830 align:middle line:84%
Like we said earlier,
they're doing more than

00:31:25.830 --> 00:31:28.950 align:middle line:84%
creating a smooth,
transparent surface.

00:31:28.950 --> 00:31:31.990 align:middle line:84%
They're creating a
molded, ornate structure

00:31:31.990 --> 00:31:36.870 align:middle line:84%
personalized to their own
shape, like a house couture.

00:31:36.870 --> 00:31:40.630 align:middle line:84%
And not only is this
process a lot of work,

00:31:40.630 --> 00:31:44.830 align:middle line:84%
it renders diatoms dependent
on silica, a chemical

00:31:44.830 --> 00:31:47.830 align:middle line:90%
they can't make for themselves.

00:31:47.830 --> 00:31:50.670 align:middle line:90%
So why do it?

00:31:50.670 --> 00:31:54.790 align:middle line:84%
Well, for one, it's cheaper
than both making and assembling

00:31:54.790 --> 00:31:56.670 align:middle line:90%
your own materials.

00:31:56.670 --> 00:32:01.510 align:middle line:84%
Silica is already out there, so
why not take advantage of it?

00:32:01.510 --> 00:32:04.830 align:middle line:84%
One study found that the
materials in diatoms' frustules

00:32:04.830 --> 00:32:08.250 align:middle line:84%
might help the organism
take in carbon dioxide,

00:32:08.250 --> 00:32:11.470 align:middle line:84%
improving their
photosynthetic capabilities.

00:32:11.470 --> 00:32:14.823 align:middle line:90%
[MUSIC PLAYING]

00:32:14.823 --> 00:32:16.740 align:middle line:90%


00:32:16.740 --> 00:32:19.220 align:middle line:84%
These advantages seem
to translate over

00:32:19.220 --> 00:32:21.980 align:middle line:84%
into the immense
capacity of diatoms

00:32:21.980 --> 00:32:27.140 align:middle line:84%
to grow and dominate over other
algae that share their waters.

00:32:27.140 --> 00:32:30.380 align:middle line:84%
But taking over a body of
water is all fun and games

00:32:30.380 --> 00:32:32.560 align:middle line:90%
until the silica runs out.

00:32:32.560 --> 00:32:35.180 align:middle line:90%


00:32:35.180 --> 00:32:37.140 align:middle line:84%
Diatoms are known
for their ability

00:32:37.140 --> 00:32:40.860 align:middle line:84%
to form large, visible blooms,
whether in your local lake

00:32:40.860 --> 00:32:42.780 align:middle line:90%
or the Arctic Ocean.

00:32:42.780 --> 00:32:45.140 align:middle line:84%
But scientists studying
those Arctic blooms

00:32:45.140 --> 00:32:48.940 align:middle line:84%
found that as the diatom
population expanded,

00:32:48.940 --> 00:32:52.540 align:middle line:84%
they also depleted their
waters of silicic acid,

00:32:52.540 --> 00:32:54.500 align:middle line:84%
and that in turn
halted their growth

00:32:54.500 --> 00:32:57.800 align:middle line:84%
and began to increase the
number of dead diatoms.

00:32:57.800 --> 00:33:00.860 align:middle line:90%


00:33:00.860 --> 00:33:04.780 align:middle line:84%
And both of these things, the
lack of growth and the dying,

00:33:04.780 --> 00:33:08.340 align:middle line:84%
have another impact on
diatom populations--

00:33:08.340 --> 00:33:09.940 align:middle line:90%
sinking.

00:33:09.940 --> 00:33:13.300 align:middle line:84%
Healthy growing diatoms can
up their buoyancy to keep them

00:33:13.300 --> 00:33:17.180 align:middle line:84%
afloat, while
dying cells cannot.

00:33:17.180 --> 00:33:20.980 align:middle line:84%
It might be sad to imagine those
blooms dying and descending

00:33:20.980 --> 00:33:24.060 align:middle line:84%
to lower depths, the
ornate jewels collapsing

00:33:24.060 --> 00:33:26.140 align:middle line:90%
like a microbial Empire.

00:33:26.140 --> 00:33:31.060 align:middle line:84%
But nature doesn't trade in
inconsequential tragedies.

00:33:31.060 --> 00:33:33.780 align:middle line:84%
The death of diatoms
leaves behind frustules

00:33:33.780 --> 00:33:37.980 align:middle line:84%
like this one, which means
it leaves behind silica.

00:33:37.980 --> 00:33:41.500 align:middle line:84%
Some of that silica can be
recycled by other diatoms.

00:33:41.500 --> 00:33:43.500 align:middle line:84%
But over time, it
will eventually

00:33:43.500 --> 00:33:49.020 align:middle line:84%
descend further and further down
until it gathers on sediments.

00:33:49.020 --> 00:33:51.940 align:middle line:84%
When a diatom takes
in silicic acid,

00:33:51.940 --> 00:33:55.620 align:middle line:84%
it's taking in the remnants
of a geological process--

00:33:55.620 --> 00:33:59.220 align:middle line:84%
the weathering and erosion that
brought the silicon to water

00:33:59.220 --> 00:34:01.020 align:middle line:90%
in the first place.

00:34:01.020 --> 00:34:03.820 align:middle line:84%
And then, through the
construction of its shell,

00:34:03.820 --> 00:34:07.260 align:middle line:84%
it recycles and transforms
the dissolved silicon

00:34:07.260 --> 00:34:11.020 align:middle line:84%
into a form that can become
geological once again.

00:34:11.020 --> 00:34:13.170 align:middle line:84%
And how that silica
gets used again

00:34:13.170 --> 00:34:17.449 align:middle line:84%
can vary, but as always with the
diatom, your chances of running

00:34:17.449 --> 00:34:19.850 align:middle line:90%
into it again are high.

00:34:19.850 --> 00:34:23.610 align:middle line:84%
Scientists found that dust from
a diatom shell-rich sediment

00:34:23.610 --> 00:34:28.010 align:middle line:84%
in Chad might travel
as far as the Amazon.

00:34:28.010 --> 00:34:29.969 align:middle line:84%
The diatom itself
may not be making

00:34:29.969 --> 00:34:34.370 align:middle line:84%
the trip, but the microcosmos
and the things built in it

00:34:34.370 --> 00:34:38.000 align:middle line:90%
have a way of sticking around.

00:34:38.000 --> 00:34:38.910 align:middle line:90%
[END PLAYBACK]

00:34:38.910 --> 00:34:40.730 align:middle line:90%


00:34:40.730 --> 00:34:44.610 align:middle line:84%
JUEJUN HU: So you see,
these amazing creatures

00:34:44.610 --> 00:34:47.710 align:middle line:84%
that can make these highly
delicate silica structures.

00:34:47.710 --> 00:34:49.489 align:middle line:84%
In fact, in the first
slide, I showed you

00:34:49.489 --> 00:34:51.090 align:middle line:84%
some photos of this
kind of structures

00:34:51.090 --> 00:34:53.050 align:middle line:90%
that were made by diatoms.

00:34:53.050 --> 00:34:55.435 align:middle line:84%
You see the geometric
variety of the structure

00:34:55.435 --> 00:34:56.810 align:middle line:84%
they were able to
make, this kind

00:34:56.810 --> 00:34:58.570 align:middle line:84%
of highly irregular
structure there.

00:34:58.570 --> 00:35:02.450 align:middle line:84%
And also, I want to mention
that the silica shell they made

00:35:02.450 --> 00:35:04.090 align:middle line:84%
is actually not
just a solid piece.

00:35:04.090 --> 00:35:05.715 align:middle line:84%
It's actually a highly
porous structure

00:35:05.715 --> 00:35:07.598 align:middle line:84%
with very large
surface-to-volume ratio.

00:35:07.598 --> 00:35:09.390 align:middle line:84%
So the porous structure
is actually useful.

00:35:09.390 --> 00:35:10.848 align:middle line:84%
It helps them to
essentially-- they

00:35:10.848 --> 00:35:14.170 align:middle line:84%
need to exchange change with
the surrounding environment.

00:35:14.170 --> 00:35:15.653 align:middle line:84%
So that's why they
actually make it

00:35:15.653 --> 00:35:17.070 align:middle line:84%
into the kind of
porous structure.

00:35:17.070 --> 00:35:18.630 align:middle line:84%
Again, the
hierarchical structure.

00:35:18.630 --> 00:35:23.130 align:middle line:84%
So we'll see later on that
how this kind of structure

00:35:23.130 --> 00:35:25.970 align:middle line:84%
can be useful for practical
applications, leveraging

00:35:25.970 --> 00:35:29.210 align:middle line:84%
the fact that they have this
kind of nanoporous architecture

00:35:29.210 --> 00:35:30.530 align:middle line:90%
there.

00:35:30.530 --> 00:35:34.270 align:middle line:84%
Now, in terms of how the
silica shell is formed,

00:35:34.270 --> 00:35:37.650 align:middle line:84%
similarly, it's also a
composite with organic phase

00:35:37.650 --> 00:35:39.770 align:middle line:84%
and the mineral
amorphous silica.

00:35:39.770 --> 00:35:43.110 align:middle line:84%
And the organic molecules
also play similar roles.

00:35:43.110 --> 00:35:45.810 align:middle line:84%
It serves as a
scaffold that catalyzes

00:35:45.810 --> 00:35:51.450 align:middle line:84%
the precipitation of silica and
also guides its microstructure.

00:35:51.450 --> 00:35:53.170 align:middle line:84%
So in the case of
diatoms, they actually

00:35:53.170 --> 00:35:55.570 align:middle line:90%
use a protein called silaffins.

00:35:55.570 --> 00:35:58.090 align:middle line:84%
So silaffins
basically can actually

00:35:58.090 --> 00:36:02.410 align:middle line:84%
trigger precipitation of
silica from surrounding

00:36:02.410 --> 00:36:05.770 align:middle line:84%
silicic solutions and
then they can actually

00:36:05.770 --> 00:36:07.930 align:middle line:84%
interact with other
molecules to actually form

00:36:07.930 --> 00:36:10.840 align:middle line:84%
organized nanostructures that
form the intricate structure

00:36:10.840 --> 00:36:14.120 align:middle line:90%
of the glass house for diatoms.

00:36:14.120 --> 00:36:17.620 align:middle line:84%
For glass sponges, they
develop their own chemistry,

00:36:17.620 --> 00:36:18.220 align:middle line:90%
interestingly.

00:36:18.220 --> 00:36:19.760 align:middle line:84%
All the silica-grown
animals, they all

00:36:19.760 --> 00:36:21.552 align:middle line:84%
have different chemistry
to actually do it.

00:36:21.552 --> 00:36:23.400 align:middle line:84%
For glass sponge,
they use silicatein,

00:36:23.400 --> 00:36:26.840 align:middle line:84%
which is actually an
enzyme that catalyzes

00:36:26.840 --> 00:36:28.260 align:middle line:90%
the precipitation of silica.

00:36:28.260 --> 00:36:32.200 align:middle line:84%
So similar biochemistry
process, but with very different

00:36:32.200 --> 00:36:35.730 align:middle line:90%
specific molecules involved.

00:36:35.730 --> 00:36:38.100 align:middle line:84%
Now, because you talk
about glass sponge,

00:36:38.100 --> 00:36:40.600 align:middle line:84%
I'm going to discuss a little
bit more about glass sponges.

00:36:40.600 --> 00:36:44.120 align:middle line:84%
So glass sponge is
actually quite interesting

00:36:44.120 --> 00:36:48.640 align:middle line:84%
because they have these
highly hierarchical structures

00:36:48.640 --> 00:36:50.400 align:middle line:90%
in their glass skeleton there.

00:36:50.400 --> 00:36:54.000 align:middle line:84%
So I quote this figure
from the science paper

00:36:54.000 --> 00:36:56.520 align:middle line:84%
here, which gives a very
nice description about how

00:36:56.520 --> 00:36:59.400 align:middle line:84%
the structural hierarchy are
distributed in silica structure

00:36:59.400 --> 00:36:59.920 align:middle line:90%
there.

00:36:59.920 --> 00:37:04.680 align:middle line:84%
So macroscopically this is sort
of like a cage-like structure

00:37:04.680 --> 00:37:07.180 align:middle line:84%
that was precipitated by
one of these glass sponges.

00:37:07.180 --> 00:37:10.200 align:middle line:84%
Now if you look closely,
you see that you

00:37:10.200 --> 00:37:13.320 align:middle line:84%
have this kind of
square lattices

00:37:13.320 --> 00:37:17.640 align:middle line:84%
that's actually reinforced
by these diagonal struts

00:37:17.640 --> 00:37:19.280 align:middle line:90%
or diagonal rods.

00:37:19.280 --> 00:37:21.452 align:middle line:84%
So later on, we'll see
that scientists actually

00:37:21.452 --> 00:37:22.660 align:middle line:90%
study this kind of structure.

00:37:22.660 --> 00:37:24.035 align:middle line:84%
They figure that
this is actually

00:37:24.035 --> 00:37:26.240 align:middle line:84%
an optimized
configuration that give it

00:37:26.240 --> 00:37:29.480 align:middle line:84%
the maximum resistance
against buckling deformation

00:37:29.480 --> 00:37:31.600 align:middle line:84%
with the minimum
amount of material,

00:37:31.600 --> 00:37:34.310 align:middle line:90%
which is quite remarkable.

00:37:34.310 --> 00:37:37.000 align:middle line:84%
Again, we're going to talk
about that in a few slides.

00:37:37.000 --> 00:37:41.120 align:middle line:84%
But if you look closely,
basically, this silica fibers

00:37:41.120 --> 00:37:43.660 align:middle line:84%
actually has
core-shell structure.

00:37:43.660 --> 00:37:45.880 align:middle line:84%
So you can see these are
actually silica fibers.

00:37:45.880 --> 00:37:47.020 align:middle line:90%
It's a bundle.

00:37:47.020 --> 00:37:50.280 align:middle line:84%
And then, within bundle, you
have this essentially fibrils.

00:37:50.280 --> 00:37:52.920 align:middle line:90%
Each fibril is actually smaller.

00:37:52.920 --> 00:37:54.840 align:middle line:84%
And then they have a
core-shell structure.

00:37:54.840 --> 00:37:57.320 align:middle line:84%
With the core, it basically
contains more protein

00:37:57.320 --> 00:38:01.360 align:middle line:84%
or the organic phase, while
the outer layers, these

00:38:01.360 --> 00:38:04.200 align:middle line:84%
are primarily essentially
amorphous silica.

00:38:04.200 --> 00:38:07.280 align:middle line:84%
In between them, they
are bound together

00:38:07.280 --> 00:38:11.680 align:middle line:84%
by these very thin,
organic interlayers.

00:38:11.680 --> 00:38:13.655 align:middle line:84%
So there are some
interesting implications

00:38:13.655 --> 00:38:14.780 align:middle line:90%
for this kind of structure.

00:38:14.780 --> 00:38:16.560 align:middle line:84%
One is that this
actually helps to improve

00:38:16.560 --> 00:38:17.980 align:middle line:90%
the mechanical robustness.

00:38:17.980 --> 00:38:18.480 align:middle line:90%
Same thing.

00:38:18.480 --> 00:38:20.720 align:middle line:84%
Because you are combining
essentially flexible--

00:38:20.720 --> 00:38:22.700 align:middle line:84%
it's sort of like
a laminated glass.

00:38:22.700 --> 00:38:24.760 align:middle line:84%
It's one good example
of naturally occurring

00:38:24.760 --> 00:38:25.540 align:middle line:90%
laminated glass.

00:38:25.540 --> 00:38:27.873 align:middle line:84%
You have organic phase binding
different kinds of silica

00:38:27.873 --> 00:38:29.400 align:middle line:90%
plates together.

00:38:29.400 --> 00:38:32.440 align:middle line:84%
Also, it also means
that there's actually

00:38:32.440 --> 00:38:37.320 align:middle line:84%
a refractive index gradient from
the core to go to the outside

00:38:37.320 --> 00:38:38.440 align:middle line:90%
there.

00:38:38.440 --> 00:38:41.140 align:middle line:84%
It turns out, the core tends to
have a higher refractive index.

00:38:41.140 --> 00:38:43.180 align:middle line:84%
The cladding tends to
have low refractive index.

00:38:43.180 --> 00:38:47.975 align:middle line:84%
So effectively, you have
a fiber-optic waveguide.

00:38:47.975 --> 00:38:49.100 align:middle line:90%
People actually look at it.

00:38:49.100 --> 00:38:51.160 align:middle line:90%
This is actually a little photo.

00:38:51.160 --> 00:38:53.600 align:middle line:84%
These glass sponges can
grow these kind of fibers

00:38:53.600 --> 00:38:57.200 align:middle line:90%
to centimeters in length.

00:38:57.200 --> 00:38:59.960 align:middle line:84%
And people have actually
measured optical loss

00:38:59.960 --> 00:39:02.060 align:middle line:84%
by sending light from
one end of this fiber

00:39:02.060 --> 00:39:03.480 align:middle line:84%
and then measure how much
light actually escapes

00:39:03.480 --> 00:39:04.380 align:middle line:90%
from the other end of fiber.

00:39:04.380 --> 00:39:05.420 align:middle line:84%
You can actually see
this picture here.

00:39:05.420 --> 00:39:06.220 align:middle line:90%
This is actually a fiber.

00:39:06.220 --> 00:39:07.870 align:middle line:84%
It's glowing because
there's actually light

00:39:07.870 --> 00:39:09.930 align:middle line:84%
scattered from the surface
as they propagate inside.

00:39:09.930 --> 00:39:12.110 align:middle line:84%
And they were able to
measure loss that's actually

00:39:12.110 --> 00:39:14.293 align:middle line:84%
less than 1 dB per
centimeter, which is better

00:39:14.293 --> 00:39:15.710 align:middle line:84%
than some of the
waveguides people

00:39:15.710 --> 00:39:17.750 align:middle line:84%
actually made, for
example, on chip.

00:39:17.750 --> 00:39:19.110 align:middle line:90%
That's quite remarkable.

00:39:19.110 --> 00:39:21.010 align:middle line:84%
Now if you look
even more closely,

00:39:21.010 --> 00:39:22.690 align:middle line:84%
look at one of
these silica layers,

00:39:22.690 --> 00:39:24.990 align:middle line:84%
it's, again, not a solid
piece of silica glass.

00:39:24.990 --> 00:39:27.670 align:middle line:84%
Instead, you see this kind
of granular structure,

00:39:27.670 --> 00:39:30.370 align:middle line:84%
indicating that when this
layer is actually formed,

00:39:30.370 --> 00:39:32.870 align:middle line:84%
it's also formed
through attachment

00:39:32.870 --> 00:39:36.630 align:middle line:84%
of silica nanoparticles, which
is a very typical process

00:39:36.630 --> 00:39:40.270 align:middle line:90%
in biomineralization.

00:39:40.270 --> 00:39:42.430 align:middle line:84%
So this serves as
a good introduction

00:39:42.430 --> 00:39:45.550 align:middle line:84%
into some of the interesting
kinetic processes

00:39:45.550 --> 00:39:50.190 align:middle line:84%
that help to shape the
unique microstructure

00:39:50.190 --> 00:39:52.710 align:middle line:90%
of the biominerals.

00:39:52.710 --> 00:39:56.230 align:middle line:84%
So what I'm going to do
in this next section here,

00:39:56.230 --> 00:39:58.510 align:middle line:84%
I will essentially be giving
you a few-- introducing

00:39:58.510 --> 00:40:01.190 align:middle line:84%
a few general features
about the kinetic processes

00:40:01.190 --> 00:40:04.330 align:middle line:84%
in microstructure evolution
of these kind of biominerals.

00:40:04.330 --> 00:40:07.750 align:middle line:84%
So first thing is that,
as we have mentioned,

00:40:07.750 --> 00:40:09.870 align:middle line:84%
the formation of this
kind of biominerals

00:40:09.870 --> 00:40:13.950 align:middle line:84%
almost always involves a
transient amorphous phase.

00:40:13.950 --> 00:40:17.170 align:middle line:84%
So this can be summarized
with this quick phrase here.

00:40:17.170 --> 00:40:21.830 align:middle line:84%
It's always amorphous
first, crystalline later.

00:40:21.830 --> 00:40:24.470 align:middle line:84%
The reason this amorphous
phase is desirable

00:40:24.470 --> 00:40:27.270 align:middle line:84%
primarily is it helps to
lower the nucleation barrier.

00:40:27.270 --> 00:40:30.230 align:middle line:84%
So it's a lot easier to
form from solution phase.

00:40:30.230 --> 00:40:33.330 align:middle line:84%
This actually is dictated by the
so-called Ostwald's step rule.

00:40:33.330 --> 00:40:36.070 align:middle line:84%
I don't know if you talk about
it in your other classes,

00:40:36.070 --> 00:40:39.110 align:middle line:84%
but essentially
what it says is that

00:40:39.110 --> 00:40:42.590 align:middle line:84%
in a non-equilibrium
process, when you're

00:40:42.590 --> 00:40:46.270 align:middle line:84%
trying to precipitate some solid
phase from a solution, what

00:40:46.270 --> 00:40:49.790 align:middle line:84%
usually precipitates out tends
to be thermodynamically least

00:40:49.790 --> 00:40:50.850 align:middle line:90%
stable phase.

00:40:50.850 --> 00:40:52.810 align:middle line:90%
It's not the most stable phase.

00:40:52.810 --> 00:40:54.672 align:middle line:84%
Because part of
the argument there

00:40:54.672 --> 00:40:56.630 align:middle line:84%
is that the thermodynamically
most stable phase

00:40:56.630 --> 00:41:00.390 align:middle line:84%
tends to be structurally
most dissimilar

00:41:00.390 --> 00:41:02.270 align:middle line:90%
compared to the solution phase.

00:41:02.270 --> 00:41:04.140 align:middle line:84%
So the kinetic barrier
is actually high.

00:41:04.140 --> 00:41:07.020 align:middle line:84%
And that's why there's always
an intermediate phase that's

00:41:07.020 --> 00:41:09.860 align:middle line:84%
thermodynamically unstable,
but kinetically expedient

00:41:09.860 --> 00:41:12.460 align:middle line:90%
to form, guide the process.

00:41:12.460 --> 00:41:14.140 align:middle line:84%
So in this case,
it's actually usually

00:41:14.140 --> 00:41:16.060 align:middle line:84%
the amorphous phase that
actually forms first,

00:41:16.060 --> 00:41:18.060 align:middle line:84%
consistent with the
Ostwald's step rule.

00:41:18.060 --> 00:41:21.720 align:middle line:84%
So it helps to reduce
interfacial energy.

00:41:21.720 --> 00:41:22.900 align:middle line:90%
I mentioned that.

00:41:22.900 --> 00:41:25.000 align:middle line:84%
And also, these
organic matrices,

00:41:25.000 --> 00:41:28.740 align:middle line:84%
they also provide
preferential nucleation sites.

00:41:28.740 --> 00:41:32.100 align:middle line:84%
That's how they actually guide
the microstructural assembly

00:41:32.100 --> 00:41:35.660 align:middle line:84%
in this kind of
precipitation process.

00:41:35.660 --> 00:41:41.420 align:middle line:84%
And then subsequently--
So when you actually

00:41:41.420 --> 00:41:43.140 align:middle line:84%
grow these minerals,
you always start out

00:41:43.140 --> 00:41:45.360 align:middle line:84%
with a solution-phase
infiltration deposition.

00:41:45.360 --> 00:41:47.760 align:middle line:84%
As I said, this is a
kinetically fast process.

00:41:47.760 --> 00:41:49.620 align:middle line:84%
Takes seconds,
maybe two minutes.

00:41:49.620 --> 00:41:52.740 align:middle line:84%
The subsequent crystallization
is a lot slower.

00:41:52.740 --> 00:41:53.440 align:middle line:90%
It's kinetic.

00:41:53.440 --> 00:41:56.140 align:middle line:84%
It's basically controlled by
these organic molecules that

00:41:56.140 --> 00:42:00.860 align:middle line:84%
serve as inhibitory agents
that control the kinetics

00:42:00.860 --> 00:42:03.020 align:middle line:90%
of the crystal growth process.

00:42:03.020 --> 00:42:07.380 align:middle line:84%
And that's why you can actually
vary-- these organisms can

00:42:07.380 --> 00:42:10.060 align:middle line:84%
control the orientation
and spatial arrangement

00:42:10.060 --> 00:42:12.420 align:middle line:84%
of those crystals when
they actually form.

00:42:12.420 --> 00:42:17.620 align:middle line:84%
So this is one example of
the so-called non-classical

00:42:17.620 --> 00:42:19.780 align:middle line:90%
crystallization process.

00:42:19.780 --> 00:42:21.380 align:middle line:84%
I have this
schematic here that's

00:42:21.380 --> 00:42:23.620 align:middle line:84%
trying to illustrate
the difference

00:42:23.620 --> 00:42:26.580 align:middle line:84%
of this non-classical
crystallization

00:42:26.580 --> 00:42:27.920 align:middle line:90%
with classical crystallization.

00:42:27.920 --> 00:42:30.340 align:middle line:84%
So for classical
crystallization process,

00:42:30.340 --> 00:42:32.800 align:middle line:84%
this is what you have learned
in your kinetics class.

00:42:32.800 --> 00:42:36.940 align:middle line:84%
You have a supersaturation
of ions in the solution.

00:42:36.940 --> 00:42:40.540 align:middle line:84%
Then, once you have
a little nuclei

00:42:40.540 --> 00:42:42.860 align:middle line:84%
or you have little
nucleus, then these ions

00:42:42.860 --> 00:42:45.333 align:middle line:84%
can attach to the surface
essentially ion by ion.

00:42:45.333 --> 00:42:47.000 align:middle line:84%
And then you build
up the crystal there.

00:42:47.000 --> 00:42:49.140 align:middle line:84%
That's the classical
nucleation process.

00:42:49.140 --> 00:42:52.900 align:middle line:84%
Now, in bioorganisms,
usually this kind of process

00:42:52.900 --> 00:42:54.460 align:middle line:90%
is not what actually happens.

00:42:54.460 --> 00:42:57.020 align:middle line:84%
What happens is that
these ions will start out

00:42:57.020 --> 00:42:59.980 align:middle line:84%
by forming these little
amorphous clusters.

00:42:59.980 --> 00:43:02.570 align:middle line:84%
Instead of attaching
to a solid ion by ion,

00:43:02.570 --> 00:43:04.310 align:middle line:90%
its actually cluster by cluster.

00:43:04.310 --> 00:43:06.978 align:middle line:90%


00:43:06.978 --> 00:43:08.770 align:middle line:84%
And then that's eventually
how you actually

00:43:08.770 --> 00:43:09.970 align:middle line:90%
form the bulk crystal.

00:43:09.970 --> 00:43:13.750 align:middle line:84%
So this is actually one good
example here in this figure.

00:43:13.750 --> 00:43:15.970 align:middle line:84%
This schematically shows
how the ACC actually

00:43:15.970 --> 00:43:19.208 align:middle line:84%
attaches to the surface
in the form of clusters.

00:43:19.208 --> 00:43:21.250 align:middle line:84%
And that's why if, you
look at the microstructure

00:43:21.250 --> 00:43:22.810 align:middle line:84%
for a lot of the
biominerals, you

00:43:22.810 --> 00:43:27.570 align:middle line:84%
tend to see this essentially
nanoparticle formation

00:43:27.570 --> 00:43:31.130 align:middle line:84%
in the solid phase there
because of the kinetic pathway.

00:43:31.130 --> 00:43:34.850 align:middle line:84%
Now, one example to
actually illustrate

00:43:34.850 --> 00:43:39.970 align:middle line:84%
this kind of kinetic
pathway here,

00:43:39.970 --> 00:43:43.810 align:middle line:84%
I'm showing you, in this case,
this is actually a sea urchin.

00:43:43.810 --> 00:43:46.530 align:middle line:84%
Basically the spikes
of the sea urchin.

00:43:46.530 --> 00:43:49.810 align:middle line:84%
The spikes are basically
calcites, calcium carbonate.

00:43:49.810 --> 00:43:55.290 align:middle line:90%


00:43:55.290 --> 00:44:00.830 align:middle line:84%
Now, calcium carbonate is
actually in the solution phase.

00:44:00.830 --> 00:44:03.570 align:middle line:84%
If it's supersaturated,
it can crystallize

00:44:03.570 --> 00:44:06.170 align:middle line:90%
within a matter of seconds.

00:44:06.170 --> 00:44:12.070 align:middle line:84%
So in order to control the
kinetics of the amorphous phase

00:44:12.070 --> 00:44:15.410 align:middle line:84%
so that you can actually
control the microstructure,

00:44:15.410 --> 00:44:17.543 align:middle line:84%
different organisms,
like sea urchin,

00:44:17.543 --> 00:44:19.210 align:middle line:84%
they have developed
their own strategies

00:44:19.210 --> 00:44:23.290 align:middle line:84%
how to regulate the
kinetics of crystallization.

00:44:23.290 --> 00:44:25.830 align:middle line:84%
There can be different chemical
processes that's involved.

00:44:25.830 --> 00:44:28.390 align:middle line:84%
For example, you can have
organic macromolecules,

00:44:28.390 --> 00:44:31.010 align:middle line:84%
whether it's protein
or polysaccharides.

00:44:31.010 --> 00:44:33.890 align:middle line:84%
And the way these organic
molecules essentially slows down

00:44:33.890 --> 00:44:36.970 align:middle line:84%
the kinetics is by essentially
they attach to the surface

00:44:36.970 --> 00:44:39.010 align:middle line:90%
and block nucleation sites.

00:44:39.010 --> 00:44:41.490 align:middle line:84%
So that way, it can slow
down the crystallization.

00:44:41.490 --> 00:44:47.050 align:middle line:84%
You can also use small ions,
like magnesium, in ACC.

00:44:47.050 --> 00:44:49.170 align:middle line:84%
Magnesium works by
essentially distorting

00:44:49.170 --> 00:44:50.890 align:middle line:84%
the local coordination
environment

00:44:50.890 --> 00:44:54.290 align:middle line:84%
and making nucleation
more difficult.

00:44:54.290 --> 00:44:56.030 align:middle line:90%
Water and hydration shells.

00:44:56.030 --> 00:44:58.283 align:middle line:84%
This is also another
commonly used strategy here.

00:44:58.283 --> 00:45:00.950 align:middle line:84%
By essentially forming this kind
of liquid-like hydration shell,

00:45:00.950 --> 00:45:03.088 align:middle line:84%
it basically creates
a kinetic barrier

00:45:03.088 --> 00:45:05.130 align:middle line:84%
to prevent the growth of
the crystals, which also

00:45:05.130 --> 00:45:07.050 align:middle line:90%
helps to control the kinetics.

00:45:07.050 --> 00:45:12.530 align:middle line:84%
And then finally, geometric
confinement also plays a role.

00:45:12.530 --> 00:45:14.083 align:middle line:84%
Lots of the organic
scaffolds, they

00:45:14.083 --> 00:45:15.750 align:middle line:84%
have this kind of
nanoporous structures.

00:45:15.750 --> 00:45:18.125 align:middle line:84%
So it means that the actual
space that allows for crystal

00:45:18.125 --> 00:45:19.370 align:middle line:90%
growth is highly constrained.

00:45:19.370 --> 00:45:22.050 align:middle line:84%
So this prevents the formation
of large randomly oriented

00:45:22.050 --> 00:45:25.090 align:middle line:84%
crystals and is essentially
used as a template

00:45:25.090 --> 00:45:28.190 align:middle line:84%
to guide the crystal assembly
in the formation process.

00:45:28.190 --> 00:45:32.410 align:middle line:84%
So one example, as I said, is
this kind of sea urchins here.

00:45:32.410 --> 00:45:34.590 align:middle line:84%
So let me explain what
they actually did.

00:45:34.590 --> 00:45:39.450 align:middle line:84%
So basically, essentially,
the scientists

00:45:39.450 --> 00:45:40.730 align:middle line:90%
collected these urchins.

00:45:40.730 --> 00:45:49.850 align:middle line:84%
They intentionally cut the
little spines or the sharp ends

00:45:49.850 --> 00:45:51.610 align:middle line:90%
of these little spines.

00:45:51.610 --> 00:45:55.370 align:middle line:84%
So then the sea urchin actually
goes ahead and repairs it.

00:45:55.370 --> 00:45:58.160 align:middle line:84%
And they look at what happens
during this kind of repairing

00:45:58.160 --> 00:45:59.560 align:middle line:90%
process.

00:45:59.560 --> 00:46:02.840 align:middle line:84%
So what I have noticed here
is that this is actually

00:46:02.840 --> 00:46:07.620 align:middle line:84%
an example of one of these
spicules that was actually cut.

00:46:07.620 --> 00:46:10.200 align:middle line:84%
And after a few days,
you notice that this

00:46:10.200 --> 00:46:12.440 align:middle line:84%
is what the surface
actually looks like.

00:46:12.440 --> 00:46:15.360 align:middle line:84%
This liquid-like
structure, this is actually

00:46:15.360 --> 00:46:17.620 align:middle line:90%
amorphous calcium carbonate.

00:46:17.620 --> 00:46:20.400 align:middle line:90%
This is basically ACC formation.

00:46:20.400 --> 00:46:22.480 align:middle line:84%
And they use this
kind of liquid phase

00:46:22.480 --> 00:46:25.840 align:middle line:84%
to first infiltrate
the structure

00:46:25.840 --> 00:46:28.160 align:middle line:84%
and then transform it
into crystalline phase.

00:46:28.160 --> 00:46:31.800 align:middle line:84%
Now, to stabilize this
ACC, they actually

00:46:31.800 --> 00:46:34.960 align:middle line:84%
combine all the three strategies
I'm talking about here.

00:46:34.960 --> 00:46:39.280 align:middle line:84%
It's actually a magnesium-rich
hydrated ACC, also stabilized

00:46:39.280 --> 00:46:41.408 align:middle line:90%
with a specific kind of protein.

00:46:41.408 --> 00:46:43.700 align:middle line:84%
So that's how they actually
control the kinetics there.

00:46:43.700 --> 00:46:47.298 align:middle line:84%
And as this kind of
molecules, they dehydrate,

00:46:47.298 --> 00:46:48.840 align:middle line:84%
this usually causes
the precipitation

00:46:48.840 --> 00:46:52.000 align:middle line:84%
of the crystalline phase
and transformation.

00:46:52.000 --> 00:46:55.320 align:middle line:84%
What's also remarkable
is that by controlling

00:46:55.320 --> 00:47:00.040 align:middle line:84%
the kinetics, the
spicules that were formed,

00:47:00.040 --> 00:47:03.120 align:middle line:84%
each of the spicules is actually
a single crystal calcium

00:47:03.120 --> 00:47:07.640 align:middle line:84%
carbonate, which is quite
remarkable because naturally

00:47:07.640 --> 00:47:09.800 align:middle line:84%
occurring process
usually don't lead

00:47:09.800 --> 00:47:11.900 align:middle line:84%
to this kind of single
crystal minerals.

00:47:11.900 --> 00:47:13.440 align:middle line:84%
In most cases, it's
polycrystalline.

00:47:13.440 --> 00:47:15.140 align:middle line:84%
If you want to get
single crystalline,

00:47:15.140 --> 00:47:17.100 align:middle line:84%
you need to introduce
in epitaxial process.

00:47:17.100 --> 00:47:20.300 align:middle line:84%
You basically have to do
this transformation very,

00:47:20.300 --> 00:47:21.520 align:middle line:90%
very slowly.

00:47:21.520 --> 00:47:23.240 align:middle line:84%
That's what you
learn from kinetics.

00:47:23.240 --> 00:47:24.920 align:middle line:84%
If you have lots of molecules,
you dump all the molecules

00:47:24.920 --> 00:47:26.360 align:middle line:84%
into the surface,
they are just going

00:47:26.360 --> 00:47:28.240 align:middle line:84%
to randomly form essentially
randomly oriented

00:47:28.240 --> 00:47:29.260 align:middle line:90%
polycrystalline material.

00:47:29.260 --> 00:47:30.968 align:middle line:84%
If you want to get
the crystalline phase,

00:47:30.968 --> 00:47:33.720 align:middle line:84%
you need to ensure that all
the atoms essentially slowly

00:47:33.720 --> 00:47:37.200 align:middle line:84%
move, find the lowest energy
position, which corresponds

00:47:37.200 --> 00:47:40.160 align:middle line:84%
to atomic lattice sites, and
then they can form actually

00:47:40.160 --> 00:47:41.220 align:middle line:90%
the single crystal.

00:47:41.220 --> 00:47:43.000 align:middle line:84%
So the whole idea
here is that you

00:47:43.000 --> 00:47:45.640 align:middle line:84%
want to be able to suppress
the crystallization

00:47:45.640 --> 00:47:47.400 align:middle line:84%
kinetics, to the
extent that it's slow

00:47:47.400 --> 00:47:52.080 align:middle line:84%
enough so that you can have this
templated epitaxial process.

00:47:52.080 --> 00:47:53.960 align:middle line:84%
So there's something
that people actually

00:47:53.960 --> 00:47:57.150 align:middle line:84%
have verified using diffraction
and TEM to find that this indeed

00:47:57.150 --> 00:47:59.990 align:middle line:84%
is actually a single
crystal calcium carbonate.

00:47:59.990 --> 00:48:01.630 align:middle line:90%
OK.

00:48:01.630 --> 00:48:02.290 align:middle line:90%
All right.

00:48:02.290 --> 00:48:07.270 align:middle line:84%
So that's about the
kinetics and the involvement

00:48:07.270 --> 00:48:09.750 align:middle line:84%
of amorphous transient
phases in the formation

00:48:09.750 --> 00:48:11.370 align:middle line:90%
of the biominerals.

00:48:11.370 --> 00:48:14.390 align:middle line:84%
So another structural feature
I just want to highlight here

00:48:14.390 --> 00:48:17.070 align:middle line:84%
is that this kind
of process also

00:48:17.070 --> 00:48:20.910 align:middle line:84%
enables the formation of
hierarchical microstructures.

00:48:20.910 --> 00:48:24.310 align:middle line:84%
The typical kinetic process,
as I mentioned here,

00:48:24.310 --> 00:48:27.030 align:middle line:84%
is that they involve the
formation of amorphous precursor

00:48:27.030 --> 00:48:27.790 align:middle line:90%
phase.

00:48:27.790 --> 00:48:30.990 align:middle line:84%
You also have a mesoscale
scaffold that mostly

00:48:30.990 --> 00:48:33.190 align:middle line:90%
consists of organic materials.

00:48:33.190 --> 00:48:35.270 align:middle line:84%
The organic materials,
they get mineralized

00:48:35.270 --> 00:48:37.970 align:middle line:84%
because of infiltration of
the amorphous precursors.

00:48:37.970 --> 00:48:39.470 align:middle line:84%
And then over time,
they then slowly

00:48:39.470 --> 00:48:41.750 align:middle line:84%
transform into the final
crystalline structures

00:48:41.750 --> 00:48:44.425 align:middle line:84%
with the nanocrystals
essentially being--

00:48:44.425 --> 00:48:46.550 align:middle line:84%
their arrangement, their
alignment, and orientation

00:48:46.550 --> 00:48:52.550 align:middle line:84%
being controlled by the
local organic matrix.

00:48:52.550 --> 00:48:56.630 align:middle line:84%
So one example for this kind
of hierarchical structure

00:48:56.630 --> 00:49:00.350 align:middle line:84%
is basically bone,
like human bone.

00:49:00.350 --> 00:49:03.270 align:middle line:84%
So this diagram shows the
hierarchical structure

00:49:03.270 --> 00:49:04.792 align:middle line:90%
of the human cortical bone.

00:49:04.792 --> 00:49:06.750 align:middle line:84%
So cortical bone is
basically the surface layer

00:49:06.750 --> 00:49:10.110 align:middle line:84%
of bone, which is
the most dense.

00:49:10.110 --> 00:49:13.750 align:middle line:84%
And that's why it's also
called the compact bone.

00:49:13.750 --> 00:49:15.670 align:middle line:84%
So if you look at
the structure here,

00:49:15.670 --> 00:49:19.770 align:middle line:84%
the basic structural unit is
this kind of collagen molecules.

00:49:19.770 --> 00:49:23.590 align:middle line:84%
The collagen molecules have
this kind of long-chain form.

00:49:23.590 --> 00:49:25.630 align:middle line:84%
And then these long-chain
organic molecules,

00:49:25.630 --> 00:49:26.930 align:middle line:90%
they basically get mineralized.

00:49:26.930 --> 00:49:29.470 align:middle line:84%
A lot of the
hydroxyapatite crystals

00:49:29.470 --> 00:49:32.610 align:middle line:84%
attach to this
kind of long fibril

00:49:32.610 --> 00:49:35.710 align:middle line:84%
to form, essentially, a
mineralized composite.

00:49:35.710 --> 00:49:38.510 align:middle line:84%
And then these kind of
fibrils then stack together

00:49:38.510 --> 00:49:40.270 align:middle line:90%
to form the collagen fibers.

00:49:40.270 --> 00:49:43.070 align:middle line:84%
These collagen fibers
then subsequently

00:49:43.070 --> 00:49:45.090 align:middle line:84%
assemble into this
kind of structure here.

00:49:45.090 --> 00:49:50.110 align:middle line:84%
Essentially it's sort of
like core-shell filaments

00:49:50.110 --> 00:49:53.070 align:middle line:84%
where, within each
core-shell filaments,

00:49:53.070 --> 00:49:55.910 align:middle line:90%
this is called the osteons.

00:49:55.910 --> 00:49:59.510 align:middle line:84%
The osteons, they typically have
a size of maybe a couple hundred

00:49:59.510 --> 00:50:02.330 align:middle line:90%
microns in terms of diameter.

00:50:02.330 --> 00:50:07.250 align:middle line:84%
And in the osteon, the inside
basically is a hollow core.

00:50:07.250 --> 00:50:10.310 align:middle line:84%
That's where the blood vessels
and nerves run through.

00:50:10.310 --> 00:50:13.470 align:middle line:84%
The outside layers
is this collagen

00:50:13.470 --> 00:50:16.350 align:middle line:84%
decorated with
hydroxyapatite that give you

00:50:16.350 --> 00:50:18.120 align:middle line:90%
the mechanical strength.

00:50:18.120 --> 00:50:19.370 align:middle line:90%
So that's the basic structure.

00:50:19.370 --> 00:50:20.287 align:middle line:90%
You need to know both.

00:50:20.287 --> 00:50:22.453 align:middle line:84%
But you can see that you
have this kind of hierarchy

00:50:22.453 --> 00:50:24.830 align:middle line:84%
here, structural hierarchy
here, from microscale, which

00:50:24.830 --> 00:50:30.590 align:middle line:84%
is the basic osteon, then go to
essentially the submicron scale,

00:50:30.590 --> 00:50:32.230 align:middle line:84%
where you have the
collagen fibers,

00:50:32.230 --> 00:50:33.870 align:middle line:84%
and eventually you
go to even smaller,

00:50:33.870 --> 00:50:38.310 align:middle line:84%
go to essentially the individual
mineralized strands of collagen

00:50:38.310 --> 00:50:39.150 align:middle line:90%
fibrils.

00:50:39.150 --> 00:50:41.683 align:middle line:84%
So this is a very
typical characteristic

00:50:41.683 --> 00:50:43.350 align:middle line:84%
of a lot of biominerals
having this kind

00:50:43.350 --> 00:50:46.230 align:middle line:90%
of structural hierarchy there.

00:50:46.230 --> 00:50:49.095 align:middle line:84%
And amorphous materials, again,
plays a very important role

00:50:49.095 --> 00:50:51.220 align:middle line:84%
in forming this kind of
hierarchical microstructure

00:50:51.220 --> 00:50:53.077 align:middle line:90%
here.

00:50:53.077 --> 00:50:55.160 align:middle line:84%
I probably don't have to
talk too much about this.

00:50:55.160 --> 00:50:56.740 align:middle line:84%
I have already
mentioned about that,

00:50:56.740 --> 00:50:58.198 align:middle line:84%
that it helps to
essentially create

00:50:58.198 --> 00:51:00.260 align:middle line:84%
this kind of a
structural flexibility

00:51:00.260 --> 00:51:03.060 align:middle line:84%
by this infiltration
deposition process.

00:51:03.060 --> 00:51:07.240 align:middle line:84%
Also, by slowing down the
crystallization kinetics,

00:51:07.240 --> 00:51:10.060 align:middle line:84%
it avoids the formation of
large, randomly oriented

00:51:10.060 --> 00:51:12.820 align:middle line:84%
crystals, which may actually
cause a lot of internal stress

00:51:12.820 --> 00:51:13.700 align:middle line:90%
and cracking.

00:51:13.700 --> 00:51:16.980 align:middle line:84%
So it helps to decrease
the brittleness

00:51:16.980 --> 00:51:19.100 align:middle line:84%
of the composite in
the formation process

00:51:19.100 --> 00:51:21.060 align:middle line:84%
and ensure its
structural integrity.

00:51:21.060 --> 00:51:25.803 align:middle line:90%
And then kinetics control.

00:51:25.803 --> 00:51:27.220 align:middle line:84%
The organisms can
also essentially

00:51:27.220 --> 00:51:29.340 align:middle line:84%
control the amorphous
formation by essentially

00:51:29.340 --> 00:51:32.420 align:middle line:84%
using these inhibitory
molecules to control kinetics

00:51:32.420 --> 00:51:36.380 align:middle line:84%
and integrate them into
hierarchical microstructure.

00:51:36.380 --> 00:51:37.180 align:middle line:90%
All right.

00:51:37.180 --> 00:51:41.180 align:middle line:84%
So that's basically about
the kinetics of this kind

00:51:41.180 --> 00:51:42.720 align:middle line:90%
of biomineralized process.

00:51:42.720 --> 00:51:44.470 align:middle line:84%
Any questions about
that before we move on

00:51:44.470 --> 00:51:47.340 align:middle line:84%
to talk about how people
learn from the processes?

00:51:47.340 --> 00:51:49.220 align:middle line:84%
AUDIENCE: Well, maybe
this will be related.

00:51:49.220 --> 00:51:54.860 align:middle line:84%
For the sponges, the amorphous
silica, is that the same--

00:51:54.860 --> 00:51:57.640 align:middle line:84%
I guess you said it was
used for waveguides.

00:51:57.640 --> 00:52:01.780 align:middle line:84%
Is it the same structure as
amorphous silica that we--

00:52:01.780 --> 00:52:02.740 align:middle line:90%
JUEJUN HU: Not exactly.

00:52:02.740 --> 00:52:04.380 align:middle line:90%
AUDIENCE: --hydrated?

00:52:04.380 --> 00:52:06.540 align:middle line:90%
I tried to look at it.

00:52:06.540 --> 00:52:07.832 align:middle line:90%
JUEJUN HU: It contains protein.

00:52:07.832 --> 00:52:08.957 align:middle line:90%
That's the main difference.

00:52:08.957 --> 00:52:10.060 align:middle line:90%
It's a composite material.

00:52:10.060 --> 00:52:10.560 align:middle line:90%
Yeah.

00:52:10.560 --> 00:52:11.435 align:middle line:90%
It's not pure silica.

00:52:11.435 --> 00:52:11.935 align:middle line:90%
Yeah.

00:52:11.935 --> 00:52:13.940 align:middle line:84%
It always contains a
little bit of protein.

00:52:13.940 --> 00:52:15.873 align:middle line:84%
AUDIENCE: It still
worked well enough?

00:52:15.873 --> 00:52:16.540 align:middle line:90%
JUEJUN HU: Yeah.

00:52:16.540 --> 00:52:19.380 align:middle line:84%
I mean, protein itself
is pretty transparent to

00:52:19.380 --> 00:52:20.660 align:middle line:90%
certain wavelengths of light.

00:52:20.660 --> 00:52:24.100 align:middle line:84%
So that's why it can work as
basically a fiber-optic cable,

00:52:24.100 --> 00:52:24.800 align:middle line:90%
basically.

00:52:24.800 --> 00:52:25.300 align:middle line:90%
Yeah.

00:52:25.300 --> 00:52:26.760 align:middle line:90%
But it's essentially silica.

00:52:26.760 --> 00:52:29.620 align:middle line:84%
But when they die, essentially,
the organic molecules,

00:52:29.620 --> 00:52:30.658 align:middle line:90%
they decompose.

00:52:30.658 --> 00:52:32.700 align:middle line:84%
So what's really left
behind becomes pure silica,

00:52:32.700 --> 00:52:36.540 align:middle line:84%
essentially, in a more porous
form, in nanoporous form.

00:52:36.540 --> 00:52:37.140 align:middle line:90%
Yeah.

00:52:37.140 --> 00:52:40.040 align:middle line:84%
AUDIENCE: So that
maybe would be better?

00:52:40.040 --> 00:52:42.180 align:middle line:90%
Well, I don't know.

00:52:42.180 --> 00:52:49.450 align:middle line:84%
And then how are they turning
things in this kinetic control

00:52:49.450 --> 00:52:52.432 align:middle line:84%
so that you don't get a
polycrystalline thing?

00:52:52.432 --> 00:52:54.890 align:middle line:84%
JUEJUN HU: For silica, it's
easy because silica practically

00:52:54.890 --> 00:52:57.050 align:middle line:90%
almost never crystallizes.

00:52:57.050 --> 00:52:59.170 align:middle line:90%
So that's quite straightforward.

00:52:59.170 --> 00:53:01.370 align:middle line:84%
You need to inhibit
the crystallization

00:53:01.370 --> 00:53:05.370 align:middle line:84%
mostly for calcium carbonate
and calcium phosphate.

00:53:05.370 --> 00:53:09.450 align:middle line:84%
AUDIENCE: So
they're purposefully

00:53:09.450 --> 00:53:10.570 align:middle line:90%
slowing everything down?

00:53:10.570 --> 00:53:16.330 align:middle line:84%
Because every process--
it felt like every process

00:53:16.330 --> 00:53:19.130 align:middle line:84%
we talked about this
semester takes place

00:53:19.130 --> 00:53:21.290 align:middle line:84%
at some sort of
annealing temperature

00:53:21.290 --> 00:53:23.290 align:middle line:90%
or something like that.

00:53:23.290 --> 00:53:28.370 align:middle line:90%
And high temperatures.

00:53:28.370 --> 00:53:29.990 align:middle line:84%
JUEJUN HU: In fact,
bio organisms,

00:53:29.990 --> 00:53:32.790 align:middle line:84%
as I said, purposefully,
they want to slow it down.

00:53:32.790 --> 00:53:33.010 align:middle line:90%
AUDIENCE: Slow it down.

00:53:33.010 --> 00:53:33.510 align:middle line:90%
OK.

00:53:33.510 --> 00:53:35.730 align:middle line:90%
So the issue is that it's--

00:53:35.730 --> 00:53:38.230 align:middle line:84%
JUEJUN HU: The issue is not
that they cannot crystallize it.

00:53:38.230 --> 00:53:40.110 align:middle line:84%
It's usually they
want to do it slowly.

00:53:40.110 --> 00:53:40.610 align:middle line:90%
Yeah.

00:53:40.610 --> 00:53:42.510 align:middle line:84%
So that's a strategy
I talk about,

00:53:42.510 --> 00:53:45.930 align:middle line:84%
for example, for the crustacean,
when they're molting.

00:53:45.930 --> 00:53:47.970 align:middle line:84%
The idea always is they
want amorphous phase

00:53:47.970 --> 00:53:50.610 align:middle line:84%
to form essentially
a raw shape quickly,

00:53:50.610 --> 00:53:53.050 align:middle line:84%
but then they slowly
try to essentially mold

00:53:53.050 --> 00:53:55.508 align:middle line:84%
the microstructure into
the desired geometry.

00:53:55.508 --> 00:53:56.050 align:middle line:90%
AUDIENCE: OK.

00:53:56.050 --> 00:53:56.717 align:middle line:90%
JUEJUN HU: Yeah.

00:53:56.717 --> 00:53:57.930 align:middle line:90%
And that always takes time.

00:53:57.930 --> 00:54:01.130 align:middle line:84%
Whether it's the
spicules for sea urchin

00:54:01.130 --> 00:54:04.770 align:middle line:84%
or it's the exoskeleton
for crustaceans,

00:54:04.770 --> 00:54:07.530 align:middle line:84%
they all have this
specific microstructure.

00:54:07.530 --> 00:54:12.030 align:middle line:84%
If you allow the crystallization
to happen normally, on pace,

00:54:12.030 --> 00:54:14.110 align:middle line:84%
then you always get
randomly oriented crystals

00:54:14.110 --> 00:54:16.610 align:middle line:84%
that does not follow this
hierarchical microstructure.

00:54:16.610 --> 00:54:20.370 align:middle line:84%
They need a templated process,
such that the crystals only

00:54:20.370 --> 00:54:22.570 align:middle line:90%
attached to the side they want.

00:54:22.570 --> 00:54:25.950 align:middle line:84%
And to do that, you
need to do it slowly.

00:54:25.950 --> 00:54:26.450 align:middle line:90%
Yeah.

00:54:26.450 --> 00:54:28.510 align:middle line:90%
To ensure the--

00:54:28.510 --> 00:54:32.730 align:middle line:84%
AUDIENCE: I guess I was
surprised that it's kinetically

00:54:32.730 --> 00:54:35.382 align:middle line:90%
favorable to crystallize even--

00:54:35.382 --> 00:54:36.590 align:middle line:90%
JUEJUN HU: It's kinetically--

00:54:36.590 --> 00:54:39.215 align:middle line:84%
I mean, it's thermodynamically
always favorable to crystallize.

00:54:39.215 --> 00:54:41.690 align:middle line:84%
But it won't kinetically
slow it down, that process.

00:54:41.690 --> 00:54:45.452 align:middle line:84%
And kinetically, by forming
this amorphous phase first,

00:54:45.452 --> 00:54:47.160 align:middle line:84%
that gives them a lot
of control in terms

00:54:47.160 --> 00:54:50.180 align:middle line:84%
of geometry and the controlled
crystallization pathways.

00:54:50.180 --> 00:54:51.160 align:middle line:90%
AUDIENCE: OK.

00:54:51.160 --> 00:54:51.800 align:middle line:90%
OK.

00:54:51.800 --> 00:54:53.413 align:middle line:90%
I'm back on track.

00:54:53.413 --> 00:54:54.080 align:middle line:90%
JUEJUN HU: Yeah.

00:54:54.080 --> 00:54:56.680 align:middle line:90%
So that's why.

00:54:56.680 --> 00:54:57.748 align:middle line:90%
OK?

00:54:57.748 --> 00:54:58.540 align:middle line:90%
AUDIENCE: All good.

00:54:58.540 --> 00:54:58.940 align:middle line:90%
JUEJUN HU: All right.

00:54:58.940 --> 00:55:00.140 align:middle line:90%
Now just a few examples.

00:55:00.140 --> 00:55:01.040 align:middle line:84%
I mean, this slide
I actually quoted

00:55:01.040 --> 00:55:02.780 align:middle line:84%
from one of the
previous lectures.

00:55:02.780 --> 00:55:06.800 align:middle line:84%
This is essentially a
bioinspired nacre-like

00:55:06.800 --> 00:55:07.675 align:middle line:90%
composite.

00:55:07.675 --> 00:55:09.800 align:middle line:84%
You have essentially these
kind of glass platelets.

00:55:09.800 --> 00:55:11.617 align:middle line:84%
In between, you put
the polymer layers.

00:55:11.617 --> 00:55:13.200 align:middle line:84%
So when you actually
try to deform it,

00:55:13.200 --> 00:55:16.880 align:middle line:84%
essentially the glass
will slide with respect

00:55:16.880 --> 00:55:19.840 align:middle line:84%
to each other because of
the interpolymeric layers.

00:55:19.840 --> 00:55:21.840 align:middle line:84%
And that actually helps
to improve the toughness

00:55:21.840 --> 00:55:24.040 align:middle line:90%
of these kind of glass plates.

00:55:24.040 --> 00:55:26.440 align:middle line:84%
So that's just one
example how these kind

00:55:26.440 --> 00:55:29.680 align:middle line:84%
of hierarchical structures
can help boost the strength

00:55:29.680 --> 00:55:32.360 align:middle line:90%
of manmade structures.

00:55:32.360 --> 00:55:35.840 align:middle line:84%
Now, as I promised, I'm going
to talk about glass sponge.

00:55:35.840 --> 00:55:40.680 align:middle line:84%
So this is another example
where we humans can

00:55:40.680 --> 00:55:42.680 align:middle line:84%
learn from essentially
nature to create

00:55:42.680 --> 00:55:45.840 align:middle line:90%
a mechanically robust design.

00:55:45.840 --> 00:55:50.200 align:middle line:84%
So this is basically the silica
skeleton, glass skeleton,

00:55:50.200 --> 00:55:53.480 align:middle line:90%
of a specific kind of a sponge.

00:55:53.480 --> 00:55:55.257 align:middle line:84%
I will not pretend
that I know Latin.

00:55:55.257 --> 00:55:57.840 align:middle line:84%
I have no idea how to pronounce
it, but it's a kind of sponge,

00:55:57.840 --> 00:55:59.400 align:middle line:90%
basically.

00:55:59.400 --> 00:56:02.680 align:middle line:84%
So as I said, it has this kind
of very unique arrangement

00:56:02.680 --> 00:56:04.320 align:middle line:90%
of the silica skeleton here.

00:56:04.320 --> 00:56:06.320 align:middle line:84%
You have essentially
a square lattice

00:56:06.320 --> 00:56:10.680 align:middle line:84%
that's essentially reinforced
by these kind of diagonal rods.

00:56:10.680 --> 00:56:13.320 align:middle line:84%
So there are actually
two sets of diagonal rods

00:56:13.320 --> 00:56:14.220 align:middle line:90%
if you look at it.

00:56:14.220 --> 00:56:17.960 align:middle line:84%
So what the scientists
did, they try

00:56:17.960 --> 00:56:20.480 align:middle line:84%
to model this structure
here with a set

00:56:20.480 --> 00:56:21.540 align:middle line:90%
of geometric parameters.

00:56:21.540 --> 00:56:23.740 align:middle line:84%
So you have, for example,
the lattice period.

00:56:23.740 --> 00:56:26.180 align:middle line:84%
You have the width of
the square lattice.

00:56:26.180 --> 00:56:27.840 align:middle line:84%
You have the width
of the struct.

00:56:27.840 --> 00:56:29.640 align:middle line:90%
All those kind of things.

00:56:29.640 --> 00:56:33.240 align:middle line:84%
What they do is then
they put it into a model.

00:56:33.240 --> 00:56:36.880 align:middle line:84%
They try to optimize all
those parameters to maximize

00:56:36.880 --> 00:56:41.720 align:middle line:84%
the resistance of the structure
against buckling deformation.

00:56:41.720 --> 00:56:44.640 align:middle line:84%
They also look into several
reference structures.

00:56:44.640 --> 00:56:46.160 align:middle line:90%
These are alternative designs.

00:56:46.160 --> 00:56:47.920 align:middle line:84%
For all the alternative
designs, you also

00:56:47.920 --> 00:56:49.520 align:middle line:84%
have a few set of
geometric parameters

00:56:49.520 --> 00:56:51.620 align:middle line:84%
that characterize
essentially the arrangement.

00:56:51.620 --> 00:56:55.480 align:middle line:84%
So similarly, they optimize all
those parameters to maximize

00:56:55.480 --> 00:56:57.640 align:middle line:90%
its buckling resistance.

00:56:57.640 --> 00:57:00.440 align:middle line:84%
And what ends up happening here,
when you look at experiment,

00:57:00.440 --> 00:57:03.840 align:middle line:84%
this structure that's
bioinspired by sponges,

00:57:03.840 --> 00:57:06.480 align:middle line:84%
exhibits the highest
buckling resistance

00:57:06.480 --> 00:57:09.440 align:middle line:84%
compared to all the other
optimized structures.

00:57:09.440 --> 00:57:13.440 align:middle line:84%
What they also found out is that
the geometric parameters coming

00:57:13.440 --> 00:57:16.720 align:middle line:84%
from the natural
sponge is actually

00:57:16.720 --> 00:57:19.600 align:middle line:84%
very close to what
people optimized using

00:57:19.600 --> 00:57:22.665 align:middle line:90%
finite-element simulation.

00:57:22.665 --> 00:57:24.040 align:middle line:84%
So in other words,
the constraint

00:57:24.040 --> 00:57:26.082 align:middle line:84%
they are putting about
here, the figure of merit,

00:57:26.082 --> 00:57:27.780 align:middle line:84%
is the maximum
buckling resistance

00:57:27.780 --> 00:57:31.040 align:middle line:84%
with the same amount of
total material, total silica.

00:57:31.040 --> 00:57:34.180 align:middle line:84%
So it essentially means
that these glass sponges,

00:57:34.180 --> 00:57:36.400 align:middle line:84%
they are really
ingenious architects.

00:57:36.400 --> 00:57:38.100 align:middle line:84%
They were able to
find out this design,

00:57:38.100 --> 00:57:39.620 align:middle line:84%
use the minimum
amount of silica,

00:57:39.620 --> 00:57:41.670 align:middle line:84%
it gives the maximum
mechanical strength.

00:57:41.670 --> 00:57:45.830 align:middle line:84%
They're very close to
optimal, within a few percent.

00:57:45.830 --> 00:57:48.270 align:middle line:84%
So to me that's
quite remarkable,

00:57:48.270 --> 00:57:51.410 align:middle line:84%
how nature were able to get to
this kind of optimized design.

00:57:51.410 --> 00:57:54.305 align:middle line:90%


00:57:54.305 --> 00:57:55.430 align:middle line:90%
So that's one example here.

00:57:55.430 --> 00:57:57.670 align:middle line:84%
We're talking about
mechanical properties.

00:57:57.670 --> 00:57:59.450 align:middle line:84%
Now let's take a look
at another example.

00:57:59.450 --> 00:58:01.250 align:middle line:84%
In this case, let's
look at diatoms.

00:58:01.250 --> 00:58:04.030 align:middle line:90%


00:58:04.030 --> 00:58:07.990 align:middle line:84%
So the silica shell of
diatoms, as I mentioned,

00:58:07.990 --> 00:58:11.910 align:middle line:84%
they have this kind of
nanoporous structure here.

00:58:11.910 --> 00:58:15.070 align:middle line:84%
So this nanoporous structure
and also the fact that

00:58:15.070 --> 00:58:17.370 align:middle line:84%
it's basically silica--
it's very abundant,

00:58:17.370 --> 00:58:19.190 align:middle line:90%
it's biocompatible--

00:58:19.190 --> 00:58:21.830 align:middle line:84%
has attracted lots of
attention for applications

00:58:21.830 --> 00:58:23.630 align:middle line:90%
like sensing or drug delivery.

00:58:23.630 --> 00:58:27.430 align:middle line:84%
So this is actually one example
of a single-molecule sensor

00:58:27.430 --> 00:58:30.652 align:middle line:84%
people were able to develop
using essentially this diatom.

00:58:30.652 --> 00:58:32.110 align:middle line:84%
So the technique
they're using here

00:58:32.110 --> 00:58:37.650 align:middle line:84%
is called SERS, Surface
Enhanced Raman Spectroscopy.

00:58:37.650 --> 00:58:39.538 align:middle line:84%
It's basically using
Raman scattering.

00:58:39.538 --> 00:58:40.830 align:middle line:90%
We talk about Raman scattering.

00:58:40.830 --> 00:58:42.788 align:middle line:84%
Different molecules,
they essentially

00:58:42.788 --> 00:58:44.330 align:middle line:84%
have different kind
of phonon energy,

00:58:44.330 --> 00:58:45.630 align:middle line:90%
different vibrational energy.

00:58:45.630 --> 00:58:48.590 align:middle line:84%
And that means that if you
essentially program, excite them

00:58:48.590 --> 00:58:51.590 align:middle line:84%
using a laser, they're going
to emit different frequencies

00:58:51.590 --> 00:58:52.890 align:middle line:90%
of Raman-scattered signals.

00:58:52.890 --> 00:58:55.190 align:middle line:84%
From that, they serve
as a molecular signature

00:58:55.190 --> 00:58:57.430 align:middle line:90%
to identify different species.

00:58:57.430 --> 00:58:59.850 align:middle line:84%
Downside, which I did not
talk about previously,

00:58:59.850 --> 00:59:02.310 align:middle line:84%
is that Raman is actually
a very weak process.

00:59:02.310 --> 00:59:06.430 align:middle line:84%
Compared to Rayleigh scattering,
Raman-scattering cross-section

00:59:06.430 --> 00:59:10.210 align:middle line:84%
is billions of times weaker
compared to Rayleigh scattering.

00:59:10.210 --> 00:59:14.110 align:middle line:84%
So normally, Raman tends to be
quite an insensitive technique.

00:59:14.110 --> 00:59:15.990 align:middle line:84%
And that's why, in
fact, Raman spectroscopy

00:59:15.990 --> 00:59:18.830 align:middle line:84%
was not even used when Raman
discovered Raman scattering.

00:59:18.830 --> 00:59:20.710 align:middle line:84%
Nobody cared about it
because it's so weak,

00:59:20.710 --> 00:59:25.170 align:middle line:84%
until '60s, '70s, when people
actually develop lasers.

00:59:25.170 --> 00:59:27.670 align:middle line:84%
They now have a very powerful
light source that can actually

00:59:27.670 --> 00:59:29.170 align:middle line:90%
excite enough Raman photons.

00:59:29.170 --> 00:59:31.070 align:middle line:84%
That's why it actually
became useful.

00:59:31.070 --> 00:59:35.030 align:middle line:84%
Now, that said, if you want to
detect a single molecule using

00:59:35.030 --> 00:59:38.020 align:middle line:84%
Raman, you can imagine it
can be quite difficult.

00:59:38.020 --> 00:59:40.500 align:middle line:84%
So the way it works is
to essentially create

00:59:40.500 --> 00:59:43.660 align:middle line:84%
these kind of microstructures,
where you can concentrate

00:59:43.660 --> 00:59:46.060 align:middle line:84%
the optical field into
a very small regime

00:59:46.060 --> 00:59:47.717 align:middle line:84%
to get into high
enough photon density

00:59:47.717 --> 00:59:49.800 align:middle line:84%
so that you can excite
enough number of molecules.

00:59:49.800 --> 00:59:51.300 align:middle line:90%
That's the basic idea of SERS.

00:59:51.300 --> 00:59:56.220 align:middle line:84%
So in this case, this kind of
porous structure of the silica,

00:59:56.220 --> 00:59:59.240 align:middle line:84%
biosilica, produced by diatom,
actually is very useful here.

00:59:59.240 --> 01:00:03.060 align:middle line:84%
It sort of acts optically
as a photonic crystal.

01:00:03.060 --> 01:00:05.340 align:middle line:84%
So when it's actually
decorated with these metallic

01:00:05.340 --> 01:00:07.700 align:middle line:84%
nanoparticles, they
can actually interact

01:00:07.700 --> 01:00:10.180 align:middle line:84%
with the metallic nanoparticles
to cause essentially

01:00:10.180 --> 01:00:13.820 align:middle line:84%
a plasmonic enhancement also
with the photonic crystal

01:00:13.820 --> 01:00:14.580 align:middle line:90%
effect.

01:00:14.580 --> 01:00:17.980 align:middle line:84%
And that produces a high density
of what are called hotspots.

01:00:17.980 --> 01:00:19.772 align:middle line:84%
So hotspots is the
terminology used in SERS

01:00:19.772 --> 01:00:21.313 align:middle line:84%
to essentially
describe regions where

01:00:21.313 --> 01:00:23.460 align:middle line:84%
you have very high local
electromagnetic field.

01:00:23.460 --> 01:00:25.553 align:middle line:84%
In those regions, if you
put a molecule there,

01:00:25.553 --> 01:00:27.720 align:middle line:84%
it's going to generate very
strong Raman scattering.

01:00:27.720 --> 01:00:29.303 align:middle line:84%
That's how you can
actually detect it.

01:00:29.303 --> 01:00:31.500 align:middle line:84%
So this kind of
porous structure helps

01:00:31.500 --> 01:00:34.660 align:middle line:84%
you to amplify the
density of these hotspots

01:00:34.660 --> 01:00:36.780 align:middle line:84%
through basically a
photonic crystal effect.

01:00:36.780 --> 01:00:40.080 align:middle line:84%
It also helps to have
large surface area.

01:00:40.080 --> 01:00:42.620 align:middle line:84%
You are able to absorb lots of
these metallic nanoparticles

01:00:42.620 --> 01:00:43.920 align:middle line:90%
to have plasmonic enhancement.

01:00:43.920 --> 01:00:47.900 align:middle line:84%
So optically, the nanoporous
structure is quite useful.

01:00:47.900 --> 01:00:50.900 align:middle line:90%
So that's one part.

01:00:50.900 --> 01:00:52.740 align:middle line:84%
What's really ingenious
about this study

01:00:52.740 --> 01:00:56.220 align:middle line:84%
is that they also use the
fact that silica is silica.

01:00:56.220 --> 01:00:58.940 align:middle line:90%
So it has hydrophilic surface.

01:00:58.940 --> 01:01:01.500 align:middle line:84%
It also has this kind
of nanoporous geometry.

01:01:01.500 --> 01:01:05.280 align:middle line:84%
So it means that it actually
wets solution really well.

01:01:05.280 --> 01:01:07.980 align:middle line:90%


01:01:07.980 --> 01:01:10.380 align:middle line:84%
So imagine you put
a droplet onto one

01:01:10.380 --> 01:01:13.620 align:middle line:84%
of these substrates that contain
this kind of diatoms, biosilica.

01:01:13.620 --> 01:01:19.460 align:middle line:84%
Then as the solution dries, this
diatom, the silica, biosilica,

01:01:19.460 --> 01:01:23.300 align:middle line:84%
essentially pulls the drying
liquid droplets towards itself.

01:01:23.300 --> 01:01:25.100 align:middle line:84%
In the process, anything
that's originally

01:01:25.100 --> 01:01:26.808 align:middle line:84%
in the solution phase,
all the molecules,

01:01:26.808 --> 01:01:28.500 align:middle line:84%
essentially get
concentrated down

01:01:28.500 --> 01:01:32.180 align:middle line:84%
into the surface of
the silica shell here.

01:01:32.180 --> 01:01:34.620 align:middle line:84%
So this also creates
very good spatial overlap

01:01:34.620 --> 01:01:37.290 align:middle line:84%
between the molecules
originally in the solution

01:01:37.290 --> 01:01:42.890 align:middle line:84%
phase to the hotspots, the SERS
hotspots on the surface there.

01:01:42.890 --> 01:01:45.010 align:middle line:84%
So that's why they were
able to actually detect

01:01:45.010 --> 01:01:47.670 align:middle line:84%
single molecules by using this
kind of architecture here.

01:01:47.670 --> 01:01:52.130 align:middle line:84%
It's like a self-concentrating
mechanism in the solution

01:01:52.130 --> 01:01:56.410 align:middle line:84%
and also provides
optical enhancement.

01:01:56.410 --> 01:01:58.863 align:middle line:84%
AUDIENCE: Can you repeat how
the optical enhancement--

01:01:58.863 --> 01:02:00.530 align:middle line:84%
JUEJUN HU: Yeah, the
optical enhancement

01:02:00.530 --> 01:02:01.862 align:middle line:90%
happens basically through--

01:02:01.862 --> 01:02:04.570 align:middle line:84%
so what they did is they have to
essentially decorate the surface

01:02:04.570 --> 01:02:06.130 align:middle line:90%
with silver nanoparticles.

01:02:06.130 --> 01:02:09.318 align:middle line:84%
So silver nanoparticles
provide plasmonic enhancement.

01:02:09.318 --> 01:02:11.610 align:middle line:84%
Essentially, because of
oscillations of free electrons,

01:02:11.610 --> 01:02:13.530 align:middle line:84%
it creates a very high
electromagnetic field

01:02:13.530 --> 01:02:14.570 align:middle line:90%
at the surface.

01:02:14.570 --> 01:02:17.290 align:middle line:84%
So by having this kind
of porous nanostructure,

01:02:17.290 --> 01:02:19.370 align:middle line:84%
you can have essentially
many attachment sites

01:02:19.370 --> 01:02:23.610 align:middle line:84%
for the silver nanoparticles,
which helps in that regard.

01:02:23.610 --> 01:02:25.367 align:middle line:90%
Itself is also photonic crystal.

01:02:25.367 --> 01:02:27.450 align:middle line:84%
So that helps essentially
also locally concentrate

01:02:27.450 --> 01:02:28.970 align:middle line:90%
electromagnetic field.

01:02:28.970 --> 01:02:30.650 align:middle line:84%
And the whole game
about SERS is just

01:02:30.650 --> 01:02:33.050 align:middle line:84%
try to concentrate
electromagnetic field

01:02:33.050 --> 01:02:35.290 align:middle line:90%
to get enhanced scattering.

01:02:35.290 --> 01:02:38.270 align:middle line:84%
So basically, that's why they
call it double enhancement.

01:02:38.270 --> 01:02:41.210 align:middle line:84%
You have essentially
the fluid enhancement,

01:02:41.210 --> 01:02:43.230 align:middle line:84%
essentially pulling the
molecule towards it.

01:02:43.230 --> 01:02:45.890 align:middle line:84%
Also, optically, it helps
to boost the signal.

01:02:45.890 --> 01:02:48.290 align:middle line:84%
That's why I think it's quite
an interesting study there.

01:02:48.290 --> 01:02:48.790 align:middle line:90%
Yeah.

01:02:48.790 --> 01:03:06.730 align:middle line:90%


01:03:06.730 --> 01:03:08.090 align:middle line:90%
All right.

01:03:08.090 --> 01:03:13.170 align:middle line:84%
Next example for this kind
of nanoporous structure.

01:03:13.170 --> 01:03:16.290 align:middle line:84%
Because it has very large
surface-to-volume ratio,

01:03:16.290 --> 01:03:19.090 align:middle line:84%
you can imagine that they can
also be used for drug delivery,

01:03:19.090 --> 01:03:23.170 align:middle line:84%
to transport drug molecules
to biological tissues.

01:03:23.170 --> 01:03:25.350 align:middle line:84%
So in this particular
study I'm quoting here,

01:03:25.350 --> 01:03:26.970 align:middle line:84%
you can see this is actually
a diatom, biosilica,

01:03:26.970 --> 01:03:27.570 align:middle line:90%
they're using.

01:03:27.570 --> 01:03:33.010 align:middle line:84%
You can see it's a
highly porous structure.

01:03:33.010 --> 01:03:35.690 align:middle line:84%
So what they did is they
actually genetically engineered

01:03:35.690 --> 01:03:36.810 align:middle line:90%
the diatom.

01:03:36.810 --> 01:03:40.200 align:middle line:84%
So when they build the silica
shell, the silica shell,

01:03:40.200 --> 01:03:42.450 align:middle line:84%
the surface is actually
decorated with a specific kind

01:03:42.450 --> 01:03:43.290 align:middle line:90%
of protein.

01:03:43.290 --> 01:03:46.650 align:middle line:84%
And this protein actually
binds to antibody

01:03:46.650 --> 01:03:50.010 align:middle line:84%
that's present on the surface
of the targeted cells, targeted

01:03:50.010 --> 01:03:50.910 align:middle line:90%
biological cells.

01:03:50.910 --> 01:03:53.530 align:middle line:84%
They want to essentially
deliver the drugs specifically

01:03:53.530 --> 01:03:56.150 align:middle line:84%
to only one kind of
biological cells.

01:03:56.150 --> 01:03:58.650 align:middle line:84%
So that's why they biological
engineer, genetically engineer

01:03:58.650 --> 01:04:00.730 align:middle line:90%
the biosilica, the diatom.

01:04:00.730 --> 01:04:02.250 align:middle line:84%
So in this plot
here, this basically

01:04:02.250 --> 01:04:05.330 align:middle line:84%
shows essentially the
surface-binding capabilities.

01:04:05.330 --> 01:04:07.710 align:middle line:84%
This one, WT, this is
basically a wild type.

01:04:07.710 --> 01:04:10.470 align:middle line:84%
This is ungenetically
modified diatom.

01:04:10.470 --> 01:04:11.630 align:middle line:90%
It doesn't really bind.

01:04:11.630 --> 01:04:13.410 align:middle line:84%
It only has some
physical adsorption

01:04:13.410 --> 01:04:16.110 align:middle line:90%
to the kind of proteins.

01:04:16.110 --> 01:04:18.710 align:middle line:84%
But if it's genetically
modified, these four strands,

01:04:18.710 --> 01:04:21.730 align:middle line:84%
you can see that they exhibit
much stronger surface affinity

01:04:21.730 --> 01:04:24.342 align:middle line:90%
to the antibodies.

01:04:24.342 --> 01:04:26.050 align:middle line:84%
So they can selectively
bind to the cell.

01:04:26.050 --> 01:04:30.690 align:middle line:84%
Also, this porous surface also
means that they can actually

01:04:30.690 --> 01:04:33.000 align:middle line:84%
be essentially-- they
can electrostatically

01:04:33.000 --> 01:04:36.180 align:middle line:84%
attract to the hydrophobic
drug molecules with a larger

01:04:36.180 --> 01:04:37.180 align:middle line:90%
surface-to-volume ratio.

01:04:37.180 --> 01:04:38.980 align:middle line:84%
They can also carry
lots of drug molecules.

01:04:38.980 --> 01:04:42.640 align:middle line:84%
So then they can then use
this kind of little biosilica

01:04:42.640 --> 01:04:44.840 align:middle line:84%
as a little vehicle
here to transport

01:04:44.840 --> 01:04:48.120 align:middle line:84%
the drug molecules in
a site-specific manner

01:04:48.120 --> 01:04:49.240 align:middle line:90%
to target the cells.

01:04:49.240 --> 01:04:51.612 align:middle line:84%
So this is actually
the image here.

01:04:51.612 --> 01:04:53.320 align:middle line:84%
This is a fluorescent
image of the cells.

01:04:53.320 --> 01:04:56.400 align:middle line:84%
So the blue part is
basically the nuclei.

01:04:56.400 --> 01:04:58.840 align:middle line:84%
The red part is the
surrounding region there.

01:04:58.840 --> 01:05:00.960 align:middle line:84%
And on the surface of
the cells, you actually

01:05:00.960 --> 01:05:05.460 align:middle line:84%
see this little silica,
little vehicles.

01:05:05.460 --> 01:05:08.320 align:middle line:84%
They serve as vehicles that
eventually attach to the surface

01:05:08.320 --> 01:05:11.120 align:middle line:84%
and deliver the drug
molecules specifically

01:05:11.120 --> 01:05:12.600 align:middle line:90%
to that kind of cell there.

01:05:12.600 --> 01:05:18.320 align:middle line:84%
So another example of using
these kind of diatom structures.

01:05:18.320 --> 01:05:22.880 align:middle line:84%
Now, last part I want
to quickly mention here

01:05:22.880 --> 01:05:27.560 align:middle line:84%
is kind of a material
synthetic strategy

01:05:27.560 --> 01:05:32.200 align:middle line:84%
that people have developed
by copying what the nature is

01:05:32.200 --> 01:05:33.620 align:middle line:90%
doing in biomineralization.

01:05:33.620 --> 01:05:36.160 align:middle line:84%
It's often called a
Polymer-Induced Liquid

01:05:36.160 --> 01:05:38.480 align:middle line:90%
Precursor, PILP.

01:05:38.480 --> 01:05:41.480 align:middle line:84%
The PILP process is
really a direct replica

01:05:41.480 --> 01:05:44.640 align:middle line:84%
of the natural
biomineralization process.

01:05:44.640 --> 01:05:46.680 align:middle line:84%
You start out by adding
these polymers that

01:05:46.680 --> 01:05:49.480 align:middle line:84%
contains ionic species in
a solution that's already

01:05:49.480 --> 01:05:51.520 align:middle line:90%
supersaturated with minerals.

01:05:51.520 --> 01:05:54.640 align:middle line:84%
In this case,
because the solution

01:05:54.640 --> 01:05:56.460 align:middle line:84%
is supersaturated
with mineral ions,

01:05:56.460 --> 01:05:59.720 align:middle line:84%
the ions then electrostatically
attract to the polymer chain.

01:05:59.720 --> 01:06:02.200 align:middle line:84%
And then they can then
assemble into essentially

01:06:02.200 --> 01:06:05.360 align:middle line:84%
these nanoclusters that
contains amorphous mineral

01:06:05.360 --> 01:06:07.160 align:middle line:90%
with the polymer matrix.

01:06:07.160 --> 01:06:08.840 align:middle line:90%
So these are the nanoclusters.

01:06:08.840 --> 01:06:12.600 align:middle line:84%
These clusters, people use
them to infiltrate whatever

01:06:12.600 --> 01:06:14.200 align:middle line:90%
template they have made.

01:06:14.200 --> 01:06:17.800 align:middle line:84%
And in the end, this
template, you then

01:06:17.800 --> 01:06:19.480 align:middle line:84%
essentially trigger
the crystallization

01:06:19.480 --> 01:06:21.180 align:middle line:90%
of those nanoclusters.

01:06:21.180 --> 01:06:22.760 align:middle line:84%
So then you form
the material that

01:06:22.760 --> 01:06:27.000 align:middle line:84%
follows whatever template you
have set for the crystallization

01:06:27.000 --> 01:06:27.740 align:middle line:90%
process.

01:06:27.740 --> 01:06:31.230 align:middle line:84%
So as you can tell, this
is very, very similar

01:06:31.230 --> 01:06:34.390 align:middle line:84%
to the biomineralization
process.

01:06:34.390 --> 01:06:37.630 align:middle line:84%
Some examples about the
application of this kind of PILP

01:06:37.630 --> 01:06:39.452 align:middle line:90%
process.

01:06:39.452 --> 01:06:40.910 align:middle line:84%
This is an example
where people are

01:06:40.910 --> 01:06:46.070 align:middle line:84%
trying to develop essentially
a bone-like microstructure

01:06:46.070 --> 01:06:48.110 align:middle line:84%
for a composite that
contains essentially

01:06:48.110 --> 01:06:52.310 align:middle line:84%
collagen with essentially
mineralized hydroxyapatite

01:06:52.310 --> 01:06:53.450 align:middle line:90%
that's decorated.

01:06:53.450 --> 01:06:55.930 align:middle line:90%
So create artificial bone.

01:06:55.930 --> 01:06:57.510 align:middle line:84%
That's what people
are trying to do.

01:06:57.510 --> 01:07:00.570 align:middle line:84%
So what's shown here
in this plot here,

01:07:00.570 --> 01:07:03.410 align:middle line:84%
this is basically they
call the collagen sponge.

01:07:03.410 --> 01:07:05.630 align:middle line:84%
It's basically a porous
structure containing

01:07:05.630 --> 01:07:07.710 align:middle line:90%
many collagen fibers.

01:07:07.710 --> 01:07:13.290 align:middle line:84%
And if you look at the SEM, this
is what the sponge looks like.

01:07:13.290 --> 01:07:16.350 align:middle line:84%
You can see this kind
of fibrous structures.

01:07:16.350 --> 01:07:18.910 align:middle line:84%
Now, if you directly use a
conventional crystallization

01:07:18.910 --> 01:07:21.110 align:middle line:84%
deposition process, this
is what you end up getting.

01:07:21.110 --> 01:07:22.990 align:middle line:90%
You see these little spheres?

01:07:22.990 --> 01:07:25.150 align:middle line:84%
These are essentially
a calcium carbonate

01:07:25.150 --> 01:07:27.630 align:middle line:84%
that crystallizes and
form little crystals that

01:07:27.630 --> 01:07:29.430 align:middle line:84%
directly then attach
to the surface there.

01:07:29.430 --> 01:07:31.510 align:middle line:84%
So this is not a
desirable microstructure.

01:07:31.510 --> 01:07:37.990 align:middle line:84%
If you use the polymer-induced
liquid precursor approach,

01:07:37.990 --> 01:07:41.070 align:middle line:84%
then you get these
kind of nanoclusters

01:07:41.070 --> 01:07:45.170 align:middle line:84%
that then attach to the surface
of the collagen fibers here.

01:07:45.170 --> 01:07:46.830 align:middle line:84%
And you get this kind
of microstructure

01:07:46.830 --> 01:07:49.430 align:middle line:84%
that's actually very similar
to what you get in the bone.

01:07:49.430 --> 01:07:52.350 align:middle line:84%
What's also interesting is
that they actually found out

01:07:52.350 --> 01:07:54.730 align:middle line:84%
that the nanocrystals
attached to fiber,

01:07:54.730 --> 01:07:57.710 align:middle line:84%
they are all aligned
crystallographically.

01:07:57.710 --> 01:08:01.710 align:middle line:84%
The long axis of the fibers,
they all align with 011

01:08:01.710 --> 01:08:05.327 align:middle line:84%
direction of the calcite
crystals that was formed,

01:08:05.327 --> 01:08:06.410 align:middle line:90%
which is quite remarkable.

01:08:06.410 --> 01:08:08.785 align:middle line:84%
This is actually the same as
what people observe actually

01:08:08.785 --> 01:08:10.150 align:middle line:90%
in human bone.

01:08:10.150 --> 01:08:10.695 align:middle line:90%
Same idea.

01:08:10.695 --> 01:08:12.070 align:middle line:84%
The crystals
crystallographically

01:08:12.070 --> 01:08:13.650 align:middle line:90%
are aligned along the fibers.

01:08:13.650 --> 01:08:20.410 align:middle line:90%


01:08:20.410 --> 01:08:23.350 align:middle line:84%
So one example about how we
can learn from nature to create

01:08:23.350 --> 01:08:27.590 align:middle line:84%
microstructures that
resembles natural biominerals.

01:08:27.590 --> 01:08:33.910 align:middle line:84%
Now, another example, this
is about enamels, the teeth.

01:08:33.910 --> 01:08:38.830 align:middle line:84%
So as I mentioned, if
you eat sugary foods,

01:08:38.830 --> 01:08:42.282 align:middle line:84%
if you drink acidic
liquids, you can

01:08:42.282 --> 01:08:44.490 align:middle line:84%
push the chemical equilibrium
to the other direction.

01:08:44.490 --> 01:08:48.710 align:middle line:84%
You start to get what's called
demineralization of the enamel.

01:08:48.710 --> 01:08:52.750 align:middle line:84%
And what shows up is this
kind of a so-called white spot

01:08:52.750 --> 01:08:54.122 align:middle line:90%
lesion.

01:08:54.122 --> 01:08:55.330 align:middle line:90%
This is actually one example.

01:08:55.330 --> 01:08:58.750 align:middle line:84%
You see these little white
spots here, like right here?

01:08:58.750 --> 01:09:01.470 align:middle line:84%
So this is actually indication
of the initial phase

01:09:01.470 --> 01:09:02.450 align:middle line:90%
of demineralization.

01:09:02.450 --> 01:09:04.950 align:middle line:84%
You are essentially
extracting the hydroxyapatite

01:09:04.950 --> 01:09:09.630 align:middle line:84%
from the surface, leaving behind
the porous enamel, which then,

01:09:09.630 --> 01:09:11.143 align:middle line:90%
of course that's bad.

01:09:11.143 --> 01:09:13.310 align:middle line:84%
Later on, you're going to
expose essentially dentin.

01:09:13.310 --> 01:09:17.149 align:middle line:84%
And then you have
basically a cavity.

01:09:17.149 --> 01:09:22.510 align:middle line:84%
So as I mentioned, good thing
is that this process is actually

01:09:22.510 --> 01:09:23.590 align:middle line:90%
reversible.

01:09:23.590 --> 01:09:29.060 align:middle line:84%
So if you supply it
more basic solution,

01:09:29.060 --> 01:09:33.720 align:middle line:84%
you supply enough amount of
essentially calcium phosphate,

01:09:33.720 --> 01:09:35.220 align:middle line:90%
you can reverse the process.

01:09:35.220 --> 01:09:37.925 align:middle line:84%
The problem though,
however, is that in order

01:09:37.925 --> 01:09:39.300 align:middle line:84%
to form the
microstructure that's

01:09:39.300 --> 01:09:40.920 align:middle line:84%
similar to what
you have in enamel,

01:09:40.920 --> 01:09:44.899 align:middle line:84%
you need to have a transient
amorphous phase, ACP.

01:09:44.899 --> 01:09:47.207 align:middle line:84%
So ACP itself is
also not stable.

01:09:47.207 --> 01:09:49.540 align:middle line:84%
It will crystallize quickly,
within a matter of minutes.

01:09:49.540 --> 01:09:51.617 align:middle line:84%
So that's why people
have developed

01:09:51.617 --> 01:09:53.700 align:middle line:84%
different kinds of strategies,
even different kind

01:09:53.700 --> 01:09:58.100 align:middle line:84%
of molecules, to essentially try
to stabilize the ACP molecules

01:09:58.100 --> 01:09:59.080 align:middle line:90%
in the solution phase.

01:09:59.080 --> 01:10:01.200 align:middle line:84%
I'm not going to go
through the details here.

01:10:01.200 --> 01:10:03.220 align:middle line:84%
There are many options
people have tried.

01:10:03.220 --> 01:10:06.020 align:middle line:84%
One, probably the most
commonly used option,

01:10:06.020 --> 01:10:07.860 align:middle line:84%
is to use a kind
of molecule called

01:10:07.860 --> 01:10:12.160 align:middle line:90%
a Casein Phosphopeptide, CPP.

01:10:12.160 --> 01:10:14.260 align:middle line:84%
CPP is basically a
polypeptide where

01:10:14.260 --> 01:10:18.860 align:middle line:84%
it has a certain arrangement
in its polypeptide chain

01:10:18.860 --> 01:10:22.200 align:middle line:84%
that can selectively
attract the ions

01:10:22.200 --> 01:10:24.180 align:middle line:84%
and then prevent
the crystallization.

01:10:24.180 --> 01:10:29.100 align:middle line:84%
So that's why this
kind of complex,

01:10:29.100 --> 01:10:36.300 align:middle line:84%
called CPP, ACP, if
you do a Google search,

01:10:36.300 --> 01:10:38.820 align:middle line:84%
you'll find lots
of dental products

01:10:38.820 --> 01:10:40.520 align:middle line:84%
that contain this
kind of complex there.

01:10:40.520 --> 01:10:41.020 align:middle line:90%
CPP.

01:10:41.020 --> 01:10:41.520 align:middle line:90%
ACP.

01:10:41.520 --> 01:10:47.140 align:middle line:84%
You find toothpaste, like
dental or tooth mousse

01:10:47.140 --> 01:10:49.640 align:middle line:84%
that you can put on
your teeth that contain

01:10:49.640 --> 01:10:50.640 align:middle line:90%
these kind of molecules.

01:10:50.640 --> 01:10:52.015 align:middle line:84%
And there are also
lots of papers

01:10:52.015 --> 01:10:53.780 align:middle line:84%
that study that,
indeed, clinically, they

01:10:53.780 --> 01:10:57.780 align:middle line:84%
have been verified to
be useful in catalyzing

01:10:57.780 --> 01:11:00.955 align:middle line:84%
so-called the
remineralization process.

01:11:00.955 --> 01:11:03.580 align:middle line:84%
So remineralization essentially
means that they can essentially

01:11:03.580 --> 01:11:07.020 align:middle line:84%
repair damages, something
like white spot lesions,

01:11:07.020 --> 01:11:10.980 align:middle line:84%
by essentially
redepositing this calcium

01:11:10.980 --> 01:11:12.360 align:middle line:90%
phosphate onto the teeth.

01:11:12.360 --> 01:11:14.562 align:middle line:84%
So this is actually
the one example

01:11:14.562 --> 01:11:16.020 align:middle line:84%
I quoted from this
paper that shows

01:11:16.020 --> 01:11:18.820 align:middle line:84%
one example of this kind of
remineralization process.

01:11:18.820 --> 01:11:20.620 align:middle line:90%
They do not use CPP.

01:11:20.620 --> 01:11:23.730 align:middle line:84%
They use another
molecule called PCBAA.

01:11:23.730 --> 01:11:24.722 align:middle line:90%
I'm not a biochemist.

01:11:24.722 --> 01:11:26.930 align:middle line:84%
I'm not going to tell you
what exactly a molecule is.

01:11:26.930 --> 01:11:31.250 align:middle line:84%
But what they claim is that
this PCBAA serves two functions.

01:11:31.250 --> 01:11:34.530 align:middle line:84%
On one hand, it helps to
slow down the crystallization

01:11:34.530 --> 01:11:38.030 align:middle line:84%
kinetics of the
calcium phosphate,

01:11:38.030 --> 01:11:40.210 align:middle line:84%
and they help with the
remineralization process.

01:11:40.210 --> 01:11:42.050 align:middle line:84%
They also have
this added function

01:11:42.050 --> 01:11:44.710 align:middle line:84%
that they can prevent the
formation of biofilms.

01:11:44.710 --> 01:11:47.210 align:middle line:84%
So the idea is that if you think
about the surface of tooth,

01:11:47.210 --> 01:11:48.430 align:middle line:90%
there are lots of bacteria.

01:11:48.430 --> 01:11:51.450 align:middle line:84%
These bacteria, their
metabolic activities

01:11:51.450 --> 01:11:53.570 align:middle line:84%
form this kind of
biofilm that covers

01:11:53.570 --> 01:11:56.650 align:middle line:84%
the surface of the tooth,
which prevents attachment

01:11:56.650 --> 01:12:00.810 align:middle line:84%
of the calcium
phosphate clusters.

01:12:00.810 --> 01:12:04.370 align:middle line:84%
So if you want to have
a sustainable, robust

01:12:04.370 --> 01:12:06.090 align:middle line:84%
remineralization
process, you need

01:12:06.090 --> 01:12:08.290 align:middle line:84%
to inhibit the
formation of biofilms.

01:12:08.290 --> 01:12:10.930 align:middle line:84%
So that's what they found
out, that this molecule also

01:12:10.930 --> 01:12:14.290 align:middle line:84%
helps to inhibit the formation
of the biofilm to facilitate

01:12:14.290 --> 01:12:16.330 align:middle line:90%
the remineralization process.

01:12:16.330 --> 01:12:18.170 align:middle line:90%
And yeah.

01:12:18.170 --> 01:12:19.450 align:middle line:90%
So that's why.

01:12:19.450 --> 01:12:21.150 align:middle line:90%
This could be useful here.

01:12:21.150 --> 01:12:21.930 align:middle line:90%
All right.

01:12:21.930 --> 01:12:25.650 align:middle line:90%
So OK.

01:12:25.650 --> 01:12:28.530 align:middle line:84%
I think we are running out of
time towards the end of class

01:12:28.530 --> 01:12:29.030 align:middle line:90%
here.

01:12:29.030 --> 01:12:31.480 align:middle line:84%
This is the last slide I
quoted from a review paper that

01:12:31.480 --> 01:12:33.730 align:middle line:84%
tells you that there are
lots of exciting applications

01:12:33.730 --> 01:12:38.370 align:middle line:84%
of biomimetic
mineralization process

01:12:38.370 --> 01:12:41.090 align:middle line:84%
that have yet to be
explored, with a lot

01:12:41.090 --> 01:12:42.570 align:middle line:90%
of exciting prospects.

01:12:42.570 --> 01:12:44.110 align:middle line:90%
So I'm going to stop here.

01:12:44.110 --> 01:12:45.770 align:middle line:90%
Any questions?

01:12:45.770 --> 01:12:47.583 align:middle line:84%
How do you grade my
final presentation?

01:12:47.583 --> 01:12:48.250 align:middle line:90%
AUDIENCE: Great.

01:12:48.250 --> 01:12:51.330 align:middle line:90%


01:12:51.330 --> 01:12:51.830 align:middle line:90%
Yeah.

01:12:51.830 --> 01:12:52.330 align:middle line:90%
Thank you.

01:12:52.330 --> 01:12:53.330 align:middle line:90%
This is cool.

01:12:53.330 --> 01:12:54.290 align:middle line:90%
JUEJUN HU: OK, great.

01:12:54.290 --> 01:12:54.850 align:middle line:90%
Yeah.

01:12:54.850 --> 01:12:57.410 align:middle line:84%
So you should get to the same
level for final presentation.

01:12:57.410 --> 01:12:59.007 align:middle line:90%
AUDIENCE: Oh, yeah.

01:12:59.007 --> 01:12:59.590 align:middle line:90%
JUEJUN HU: No.

01:12:59.590 --> 01:13:00.770 align:middle line:90%
It's fine.

01:13:00.770 --> 01:13:02.910 align:middle line:84%
But anyway, if you have
any questions, let me know.

01:13:02.910 --> 01:13:04.670 align:middle line:84%
I think this is a
quite exciting process.

01:13:04.670 --> 01:13:07.400 align:middle line:84%
Well, I got to
learn a lot myself.

01:13:07.400 --> 01:14:18.000 align:middle line:90%