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CHM
11500Lecture
29Advanced
MaterialsSection
12.7and
pp.
249-252EnergyWorld
annual
energy
consumption
is
=
1.22
x
1014
kWhKnown
reserves
of
petroleum
will
provide
2.14
x
1015
kWhNote
that
energy
comes
from
oil,
coal,
gas,
nuclear,
biosources(e.g.,
wood)
and
renewables-
not
just
oil.Still,
these
numbers
may
help
us
to
see
why
renewable
sources
of
energyare
needed,
from
a
supply
perspective.Plus
there
are
also
environmental
issues
at
play.Let’s
talk
about
solar
energySolar
EnergySolar
energy
available
in
U.S.
in
1
year
is
about10
times
total
energy
available
in
ALL
known
oilreserves
on
the
planet.Solar
radiation
hitting
Earth’s
surface(for
overhead
midday
sun)
=
925
W/m2(power
=
energy
per
time, 1
W
=
1
J/s)Possibilities
for
Solar
Power4Current
solar
cells
operate
between20-30%
efficiency
(i.e.
100
J
in
assunlight,
20-30
J
out
as
electricity)Cost
is
currently
about
35¢/kWh
(versus
2¢/kWh
from
fossil
fuel-basedelectricity)Pollution-free
during
use. But
production
yields
toxic
waste.Grid
connected
solar
electricity
can
be
used
locally,
minimizingtransmission
losses
and
excess
generated
can
be
sold
to
powercompanies
(to
be
used
later.)Requires
energy
storage
through
battery
systems
(for
times
of
no
sun)Solar
cells
produce
DC
which
must
be
converted
to
AC
(for
existingpower
grids). This
incurs
an
energy
loss
of
4-12%Capturing
Solar
Energy“Passive”Allow
solar
radiation
to
be
captured
as
heat
–
such
as heating
water
or
bricks
or
other
“heat
sinks”. Heat
is then
released
as
needed.“Active”Allowing
solar
radiation
to
strike
a
solar
cell
which converts
it
to
an
electric
current. Store
the
electricity in
batteries
to
use
later
or
use
it
do
work
(example, powering
a
motor)5 Passive
Solar
Panels
“Solar
Thermal”
panels
–
the
original
solarpanelsGenerally
used
toheat
water6Passive
Solar
Home
DesignHeat
absorbing
materialwhich
will
radiate
heatback
out
at
night.Example:
brick
orcertain
tiles.8 Solar
Cells
(Photovoltaics)
Overview
of
how
they
work….To
understand
how
solar
cells
work,
wemust
understand
“n”
and
“p”
typesemiconductors
at
the
“band”
level.How
Does
Electrical
ConductionHappen
in
Solids?9Electronic
structure
of
solidsclasses:conductorssemiconductorsinsulatorsBand
TheoryRecall
atomic
energy
levels
and
orbitalsRecall:“valenceorbitals”=
outermostorbitals
withhighest
n
value101
valence
electron
/
Li
atom)Band
TheoryAs
the
number
ofatoms
in
a
crystallinesolid
increases,
thenumber
of
availableenergy
levelsincreases–
The
number
ofenergylevels
in
a
cluster
ofatoms
=
the
totalnumber
of
levelsavailable
from
theindividual
atoms(for
Li
2s
orbitals;11As
the
number
of
atoms
increases,
the
energy
levelsget
closer
together,
until
they
eventually
make
acontinuous
“band”Electrons
will
fill
energy
levels
from
the
bottom
up,forming
a
filled
band
and
an
unfilled
band.12Band
TheoryThe
closeness
of
theenergy
levels
results
in
afilled
band
(a
“valenceband”)
and
an
emptyband,
called“conduction
band”.Band
Theory13EgThey
are
separated
by
anenergy
gap
called
the“band
gap”,
Eg.Band
Gap14The
energy
gap,
Eg,
between
the
valence
band
andconduction
band
determines
the
electrical
propertiesof
the
material:
metal
(conductor),
semiconductor,insulator(NOTE:
the
bands
do
not
get
smaller
as
the
gap
gets
bigger
although
the
figurebelow
suggests
that)ConductivityTransfer
anelectron
fromvalence
band
toconduction
band–
This
creates
apositive
“hole”
inthe
valence
band(a
virtual
positivecharge)Electron
andhole
move
inoppositedirections
whenconducting
(inresponse
to
anapplied
voltagedifference)15Energy
Required
=
Eg16Need
to
put
in
Eg
of
energy
to
induce
acurrentIn
metals,
this
is
essentially
zero
(just
needto
apply
a
potential
difference).
Theelectrons
can
travel
freely
at
room
tempIn
insulators,
it
is
very
large
-
no
mobileelectrons
at
room
tempIn
semiconductors,
it
is
in
the
IR/Visiblerange.
A
small
number
of
electrons
aremobile
at
room
temp.Characteristics
of
TypicalSemiconducting
MaterialsMaterialEgdiamond(insulator)9.61
x
10-19
J(206
nm,
UV)puregermanium1.05
x
10-19
J(1886
nm,
mid-IR)pure
silicon1.79
x
10-19
J(1110
nm,
near
IR)pure
galliumarsenide2.27
x
10-19
J(874
nm,
near
IR)Band
gaps
often
reported
in
eV;1
eV=
1.602
x
10-19
J17QuestionIt
is
useful
for
solar
cells
to
be
responsivetolight
in
the
visible
portion
of
the
spectrum.Which
of
these
materials
would
be
mostuseful
for
such
an
application?Material
A:
bandgap
=
5.5
x
10-19
JMaterial
B:
bandgap
=
1.5
x
10-19
JMaterial
C:
bandgap
=
1.2
x
10-18
J18Extrinsic
and
IntrinsicSemiconductorsintrinsic
semiconductors
–
the
pure,crystalline
material
has
semiconductingproperties
(such
as
pure
Si
or
Ge)extrinsic
semiconductors
––
material
is
“doped”
with
a
small
amount
ofimpurity
of
a
similar
material
(about
1
in
106
to1
in
108
atoms)Doped
Semiconductors20decreased
Eg
(band
gap)
relative
to
intrinsicmaterialp-type:doped
with
an
element
with
fewer
electronsprovides
positive
charge
carriers
(“holes”)n-type:doped
with
element
with
more
electronsprovides
negative
charge
carriers
(electrons)Extrinsic
and
IntrinsicSemiconductorsintrinsic
silicon
(group
IV
element)silicondopedwithP
atoms
(groupV);
additionalelectronsavailable; smaller
bandgapsilicon
doped
with
Ga
atoms
(group
III);
additional
holes;
smaller bandgap21Doped
Semiconductor
BandStructureNote:Fermilevel:averageenergy
ofunpairedelectronsLevelsare
ofunequalenergyThe Big
PictureEnergy
bands
result
when
large
numbers
ofatoms
combine
to
form
a
crystal.The
spacing
between
the
filled
(“valence”
and
unfilled(“conduction”)
bands
is
the
“bandgap”
with
energy
Eg.The
size
of
Eg
willdetermine
the
properties
of
the
material.Nanomaterials
are
composed
of
substances
withstructures
on
the
nanometer
scale.Integrated
Circuits(Computer
“Chips”)put
n-type
and
p-typematerial
together
to
get
ap-n
rectifier,
or
“diode”current
can
only
move
inone
direction
across
the
p-njunctionother
combinations
of
pand
n
can
be
used
tomake
other
devices.combinations
can
beprinted
on
silicon
tomakesolid-state
integratedcircuits24How
an
LED
WorksLight
Emitting
Diodep-n
junctionwhen
an
electron
and
hole
get
to
the
junction,they
can
“combine”
and
emit
light. (This
isactually
the
electron
losing
energy
by
fallinginto
the
hole.)Electricity
in,
light
out2526Fermi
levels
areequal
at
the
junction.When
electron
andhole
get
to
junction,they
can
“combine”and
emit
light.Electricity
in,
lightoutLight
Emitting
DiodeSolarenergy27bodySolar
cellPlantsHeat,
steamBlackWind
(windmills)ElectricityHydrogenFossil
fuelsBiofuelsConversion
of
Solar
EnergyrenewableHow
a
Solar
Cell
WorksOpposite
of
an
LED. Apply
the
voltage
in
reverse.Light
in,
electricity
outSolar
panels
are
made
out
of
hundreds
of
solarcells
(photovoltaic
cells)
in
series.28DemoA
solar
car2930New
Materials
for
Solar
PowerTraditional
solar
cells
are
brittle
and
bulky.New
flexible
materials
are
being
developedand
researched.A
silicon
nanoparticle-basedflexible
solar
material….31New
Materials
for
Solar
PowerOthers
are
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