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Fuel Cells and a Nanoscale Approach to Materials Design

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Fuel Cells and a Nanoscale Approach to Materials Design. Chris Lucas Department of Physics. Outline PEM fuel cells (issues) A nanoscale approach to materials design. What is a fuel cell?. A fuel cell is an electrochemical energy conversion device - PowerPoint PPT Presentation
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Fuel Cells and a Nanoscale Fuel Cells and a Nanoscale Approach to Materials Design Approach to Materials Design Chris Lucas Chris Lucas Department of Physics Department of Physics Outline PEM fuel cells (issues) A nanoscale approach to materials design
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Page 1: Fuel Cells and a  Nanoscale  Approach to Materials Design

Fuel Cells and a Nanoscale Approach to Fuel Cells and a Nanoscale Approach to Materials DesignMaterials Design

Chris LucasChris Lucas

Department of PhysicsDepartment of Physics

Outline

PEM fuel cells (issues)

A nanoscale approach to materials design

Page 2: Fuel Cells and a  Nanoscale  Approach to Materials Design

What is a fuel cell? A fuel cell is an electrochemical energy conversion device

It converts hydrogen and oxygen into water and produces electricity

The chemicals (fuel) flow continuously unlike in a battery

Several types:(1)PEM (transportation applications)(2)Solid oxide fuel cell (stationary applications, co-generation of heat and power)

Page 3: Fuel Cells and a  Nanoscale  Approach to Materials Design

Hydrogen Cars: Fad or the Future? Science, June 2009

Page 4: Fuel Cells and a  Nanoscale  Approach to Materials Design

Hydrogen Cars: Fad or the Future? Science, June 2009

Page 5: Fuel Cells and a  Nanoscale  Approach to Materials Design

Proton Exchange Membraneor

Polymer Electrolyte Membrane

PEM Fuel Cell Technology

Membrane is a permeable polymer sheet which allows protons (H atoms) to pass through Operate at low temperatures with high power density Low cost, small size, high performance Ideal for transportation, stationary and portable applications

Page 6: Fuel Cells and a  Nanoscale  Approach to Materials Design

Energy Storage and Conversion: Fuel Cells

Efficiency issues:

Membrane transport

Anode:Impurity-tolerant catalyst

Cathode:A good catalyst for oxygen reduction reaction (ORR)(1/2O2+2H++2e- = H2O)

Nanoscale and Surface Physics: Catalyst Materials by Design

Page 7: Fuel Cells and a  Nanoscale  Approach to Materials Design

Catalyst Issues

(1) Substantial overpotential for the ORR reduces the thermal efficiency to 43% at 0.7 V [compared to 87% at reversible ORR potential (1.23 V)]

(2) Pt is expensive (Pt-loading)

(3) Performance degrades too quickly due to dissolution (stability issue)

Question: Can we use modern experimental methods to design a nanoscale catalyst?

Page 8: Fuel Cells and a  Nanoscale  Approach to Materials Design

Tailoring surface properties at the atomic level

Bifunctional effects:

Effects can be: (1) Ensemble (2) Electronic

Nanoscale and Surface Physics: Catalyst Materials by Design

M to do something else?

Pt for catalysis

Bimetallic Pt-alloy surfaces - Pt3M

Page 9: Fuel Cells and a  Nanoscale  Approach to Materials Design

Modern Experimental Methods

UHV preparation and characterization

Transfer to liquid environment for activity measurements

Transfer back to observe changes-or even better, have a look in-situ

(1) Polycrystalline materials(2) Single crystals

Page 10: Fuel Cells and a  Nanoscale  Approach to Materials Design

Calculated d-band center [eV]

-3.0 -2.8 -2.6

Cal

cula

ted

acti

vity

[10

-2 e

V]

0

2

4

6

d-band center [eV]

2.63.03.4Spec

ific

Act

ivit

y: i k

@ 0

.9V

[m

A/c

m2 re

al]

0

1

2

3

4

Pt3Ti

Pt3V

Pt3Fe

Pt3CoPt3Ni

Pt-polyPt-skin surfaces

Pt-skeleton surfaces

Act

ivit

y im

prov

emen

t fa

ctor

vs.

Pt-

poly

1

2

3

d-band center [eV]

2.63.03.4Spec

ific

Act

ivit

y: i k

@ 0

.9V

[m

A/c

m2 re

al]

0

1

2

3

4

Pt3Ti

Pt3V

Pt3Fe

Pt3CoPt3Ni

Pt-polyPt-skin surfaces

Pt-skeleton surfaces

Act

ivit

y im

prov

emen

t fa

ctor

vs.

Pt-

poly

1

2

3

Calculated d-band center [eV]

-3.0 -2.8 -2.6

Cal

cula

ted

acti

vity

[10

-2 e

V]

0

2

4

6

d-band center [eV]

2.63.03.4Spec

ific

Act

ivit

y: i k

@ 0

.9V

[m

A/c

m2 re

al]

0

1

2

3

4

Pt3Ti

Pt3V

Pt3Fe

Pt3CoPt3Ni

Pt-polyPt-skin surfaces

Pt-skeleton surfaces

Act

ivit

y im

prov

emen

t fa

ctor

vs.

Pt-

poly

1

2

3

ad) term

Gad termand

ad) term

Pt

Pt3Ni

Pt3Co

Pt3Fe

Pt3Ti

(a) (b)

Trends in catalytic activity across the Periodic Table (3d metals)

Strong link between atomic/electronic structure and activity both from theory and experiment(d-band center is proportional to adsorption strength)

Nature Materials, v6, p241 (2007)

Page 11: Fuel Cells and a  Nanoscale  Approach to Materials Design

Model Electrocatalysts: Pt3Ni crystals

Page 12: Fuel Cells and a  Nanoscale  Approach to Materials Design

electrolyte out

electrolyte in

counter electrode

crystal

working electrode

polypropylene film

reference electrode (SCE)

electrolyte out

electrolyte in

counter electrode

crystal

working electrode

polypropylene film

reference electrode (SCE)

Model Electrocatalysts: Pt3Ni crystals

XMaSthethe UK-CRGUK-CRG

Page 13: Fuel Cells and a  Nanoscale  Approach to Materials Design

( 1 1 1 ) f a c e t s

P t 3 N i - n a n o p a r t i c l e s

0 . 1 H C l O 4

6 0 o C@ 0 . 9 V v s . R H E

d - b a n d c e n t e r p o s i t i o n v s F . L . [ e V ]

2 . 42 . 52 . 62 . 72 . 82 . 93 . 03 . 13 . 2

Sp

ecif

ic A

ctiv

ity

i k [ m

A/c

m2 ]

0

5

1 0

1 5

P t ( 1 1 0 )P t ( 1 1 1 )

P t ( 1 0 0 )

P t 3 N i ( 1 1 1 )

P t - p o l y

P t 3 N i - p o l y

1 0

0

5

Act

ivit

y Im

pro

vem

ent

Fac

tor

vs. P

t-p

oly

P t 3 N i ( 1 0 0 )

P t 3 N i ( 1 1 0 )

E x t e r i o r S n a p s h o t [ 0 0 1 ] C r o s s S e c t i o n( b )

( a )

[ 0 1 1 ]

[ 0 1 - 1 ]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

x - S p u t t v s y - S p u t t

E / E 0

0 . 2 0 . 4 0 . 6 0 . 8

Inte

nsi

ty [

arb

. un

its]

P t 0 . 7 1

[ 0 1 1 ]

[ 0 1 - 1 ]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

x - S p u t t v s y - S p u t t

E / E 0

0 . 2 0 . 4 0 . 6 0 . 8

Inte

nsi

ty [

arb

. un

its]

P t 0 . 7 1

Key results from combined studies:

[ 0 1 1 ]

[ 0 1 - 1 ]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

x - S p u t t v s y - S p u t t

E / E 0

0 . 2 0 . 4 0 . 6 0 . 8

Inte

nsi

ty [

arb

. un

its]

P t 0 . 7 1

[ 0 1 1 ]

[ 0 1 - 1 ]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

x - S p u t t v s y - S p u t t

E / E 0

0 . 2 0 . 4 0 . 6 0 . 8

Inte

nsi

ty [

arb

. un

its]

P t 0 . 7 1

(1)Surfaces are 100% Pt

(2) Segregated surfaces are stable during reactions

(3) Activity depends on atomic geometry

Science, v315, p493 (2007)

Page 14: Fuel Cells and a  Nanoscale  Approach to Materials Design

Nanoscale and Surface Physics: Catalyst Materials by Design

Real catalysts are nanoparticle arrays

Page 15: Fuel Cells and a  Nanoscale  Approach to Materials Design

TEM shows nanoparticles governed by ECS

[ 0 1 1 ]

[ 0 1 - 1 ]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

B i n d i n g E n e r g y [ e V ]

02468

Inte

nsi

ty [

arb

. un

its]

x - S p u t t v s y - S p u t t

E / E 0

0 . 2 0 . 4 0 . 6 0 . 8

Inte

nsi

ty [

arb

. un

its]

P t 0 . 7 1

Page 16: Fuel Cells and a  Nanoscale  Approach to Materials Design

DFT and Monte-Carlo calculations for nanoparticles

These nanoparticles have yet to be engineered

Pt75Ni25 -[111]- Nanoparticles

Atomic Layer

Con

cen

trat

ion

of

Pt

Ato

ms

0

20

40

60

80

100

1 2 3Atomic Layer

[001] Cross Section

Monte Carlo iterations [x103]

0 20 40 60 80 100

Ave

rgae

Ato

mic

En

ergy

[eV

]-5.18

-5.16

-5.14

-5.12

-5.10

-5.08

-5.06(a) (b)- Pt - Ni

Bulk Ratio

Tetrahedron

Octahedron

Page 17: Fuel Cells and a  Nanoscale  Approach to Materials Design

Science, v324 (April, 2009)

Just a Dream-or Future Reality?

Nitrogen coordinated Fe in a carbon matrix now matches Pt/C

Turnover frequency= number of electrons per active site per second

Page 18: Fuel Cells and a  Nanoscale  Approach to Materials Design

Summary

• Fuel cells offer significant potential climate and energy security benefits

• Materials design from fundamental nanoscale studies

• This approach could be used in a range of materials (and energy) applications

Note: The University of Birmingham is the only UK institution to work on all aspects of Hydrogen energy research


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