The PEM Fuel Cells. Frick Laboratory, Princeton University Catalyst Layer Pt/C with Proton...
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The PEM Fuel Cells
Frick Laboratory, Princeton University
0 200 400 600 800 1000 1200 1400 1600 18000.0
0.2
0.4
0.6
0.8
1.0 Nafion 115 80oC 130
oC
Silicon Oxide/Aciplex 1004 130oC
Ce
ll P
ote
ntia
l / V
Current Density / mA cm2
Nafion Thermal Behavior
Frick Laboratory, Princeton University
§The composite typically contains 3-6 wt% metal oxide.
§TGA indicates the same water content and dehydration temperature for pure Nafion and the composite.
§The conductivity of the composite measured in a mechanically unconstrained environment is the same or slightly worse than the conductivity of pure Nafion.
The metal oxide is not simply providing a water retentive or hydrated interface.
Is the Metal Oxide Phase Water Retentive?
Frick Laboratory, Princeton University
If it’s not a question of direct dehydration, then what is occurring?
• First, we will seek a molecular picture.
• Then, we will attempt to make connections between our understanding of the molecular structure and bulk materials properties.
Frick Laboratory, Princeton University
0 500 1000 15000.2
0.4
0.6
0.8
1.0
130oC (Degussa-Huls)
TiO2; 21nm; 50 m2 /g (R - 0.18)
SiO2; 20nm; 90 m2
/g (R - 0.21)
Al2O3; 13 nm; 100 m2
/g (R - 0.76)
Recast Nafion Control (R - 0.5)
Cel
l Pot
entia
l / V
Current Density / mA cm-2
Effect of Effect of Metal Oxide Identity on Membrane Metal Oxide Identity on Membrane PerformancePerformance
Frick Laboratory, Princeton University
0 200 400 600 800 1000 1200 1400 1600
0.2
0.4
0.6
0.8
1.0TiO2
(AA)/Recast Nafion; 130˚C
unmodified (R - 0.50) silylated (R - 0.29) H2SO4, HNO3, "degreased" (R - 0.25)
Cel
l Pot
entia
l / V
Current Density / mA cm-2
Interfacial Chemistry is Critical
Frick Laboratory, Princeton University
The Effect of Relative Humidity on Recast Nafion
0 200 400 600 800 1000 1200 1400 16000.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
cell potential(V)
current density (mA/cm 2)
Control membrane(H2-O
2)
1300C 30 psig 100% RH 88% RH 75% RH
Frick Laboratory, Princeton University
75% Relative Humidity
0 200 400 600 800 1000 1200 14000.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
cell potential(V)
current density (mA/cm 2)
1300C 75% RH Control Recast Degussa Huls SiO
2
Alfa Aesar SiO2
Degussa Huls TiO2
Alfa Aesar TiO2
125µ Film
3 atm pressure
40 ml/min
Frick Laboratory, Princeton University
----CF2-CF2---
OH OH
Metal Oxide
-----CF-----
O=S=O
OH
Metal Oxide
O
Ti
Metal Oxide
HO
-----CF-----
SO3-
Potential Chemical Interactions
Frick Laboratory, Princeton University
Thermal decomposition of Nafion
SO2
1st step
CFO+
2nd step C3F5+
H2O
H2O
0 100 200 300 400 500-70
-60
-50
-40
-30
-20
-10
0
Weight loss/ %
Temperature / °C
m/z 64 SO2
MS abundance / a.u.
m/z 47 COF
m/z 131 C3F
5
m/z 18 H2O
H2O SO2
C3F5+
CFO+
-
Temperature Programmed Decomposition (TG-MS) of Nafion 117
Frick Laboratory, Princeton University
Thermal decomposition of Nafion
SO2
1st step
CFO+
3rd stepC3F5
+
H2O
m/z 18 H2O
m/z 64 SO2
MS abundance / a.u.
m/z 47 COF
m/z 131 C3F
5
0 100 200 300 400 500-70
-60
-50
-40
-30
-20
-10
0
Weight loss/ %
Temperature / °C
H2O
SO2C3F5
+
CFO+
2nd step
-
HO
TiO2
TG-MS Profile of Nafion/TiO2 Composite Membranes
Frick Laboratory, Princeton University
TPD-MS profiles of Nafion/Inorganic composite membranes
-
200 250 300 350 400
Intensity / a.u.
Temperature / °C
117Nafion + 3% Nafion TiO2
+ 3% Nafion SiO2
+ 3% Nafion Al2O3
+ 3% Nafion ZrO2
200 250 300 350 400
Intensity / a.u.
Temperature / °C
117Nafion + 3% Nafion TiO2
+ 3% Nafion SiO2
+ 3% Nafion Al2O3
+ 3% Nafion ZrO2
SO2 (m/z 64)
H2O (m/z 18)
CFO (m/z 47)
200 250 300 350 400
Intensity / a.u.
Temperature / °C
117Nafion + 3% Nafion TiO2
+ 3% Nafion SiO2
+ 3% Nafion Al2O3
+ 3% Nafion ZrO2
200 250 300 350 400
Intensity / a.u.
Temperature / °C
117Nafion + 3% Nafion TiO2
+ 3% Nafion SiO2
+ 3% Nafion Al2O3
+ 3% Nafion ZrO2
C3F5 (m/z 131)
Frick Laboratory, Princeton University
MOx
•Crosslinking controls the mechanical properties of the polymer•Glass transition temperature•Bulk rigidity – better water retention under stress load
Molecular Model
Frick Laboratory, Princeton University
Dependence of Nafion Glass Transition on Metal Oxide
Frick Laboratory, Princeton University
SAXS Studies
Frick Laboratory, Princeton University
Heat
Self Assembled Disordered
Crystalline
Order-Disorder Transition
Frick Laboratory, Princeton University
Ionic inclusions swell with water uptake, requiring the membrane to push the electrodes apart.
Membrane Mechanical Properties Affect Cell Response
Frick Laboratory, Princeton University
0 20 40 60 80 100 120 140 160 180 2000.0
5.0x1051.0x1061.5x1062.0x1062.5x1063.0x1063.5x1064.0x1064.5x1065.0x1065.5x106
Metal Oxide Composite Nafion 112
Str
ess
(N
/m2 )
Strain(%)
Stress-Strain Response
Frick Laboratory, Princeton University
Too Much of a Good Thing is Bad
Applied Pressure by Current Collector Plates
Swelling Pressure ofPolymer Membrane
50
55
60
20000 22000 24000 26000 28000 30000
Time (s)
Current (mA)
30
30.5
31
31.5
32
32.5
33
33.5
34
34.5
35
Power (mW)
Frick Laboratory, Princeton University
Membrane Swelling
(c)Additional pressure further increases the membrane/catalyst contact. However, the larger pressure forces water out of the membrane.
(a)The membrane is in contact with the catalyst support particles.
(b)Applied pressure enhances the membrane/catalyst contact.
mem
bra
ne
Carbon support
Frick Laboratory, Princeton University
Hydrogen Crossover
800
850
900
950
1000
Open Circuit Voltage (mV)
0.0
1.0
2.0
3.0
4.0
Crossover Current (m
A/cm2)
125µm 40µm 40µm Composite
Membrane
Frick Laboratory, Princeton University
•Increased Tg allows maintenance of hydrated proton conduction paths at elevated temperatures.
•Improved mechanical rigidity allows for dimensional stability under conditions where water content of the membrane may be changing.
•Maintains good catalyst contact on deswelling
•Eliminates water loss on swelling.
What Role Does the Metal Oxide Play?
Frick Laboratory, Princeton University
0 200 400 600 800 1000 1200 1400 16000.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0 Nafion 115 - 80o
C Pt Anode w/o CO w/100 ppm CO
TiO2 - 130
oC Pt/Ru Anode
w/100 ppm CO w/500 ppm CO
Cel
l Pot
entia
l / V
Current Density / mA cm-2
Carbon Monoxide Tolerance
Frick Laboratory, Princeton University
Summary
High Temperature Nafion Based PEM Fuel Cells overcome
several limitations associated with current cell design
Addition of a metal oxide phase affects the mechanical properties of the membrane:
Increased Tg
Improved gas barrier
Mitigation of swelling/deswelling effects
Bonus Material (It’s not electrochemistry, but it is interesting)
So, How Does One Store Hydrogen on the Run?
Frick Laboratory, Princeton University
Storage Issues Safety For mobile applications range & power should be maintained.
5-10Kg of H2 needed for a 65-75kW engine.
H2 feed rate is ~1000 liters/minute Weight Effective Density of Hydrogen Volume Requirements
Size Geometry
Refill Availability Recharge rate.
Cost
Frick Laboratory, Princeton University
Hydrogen Storage Phases
Limiting Densities of Molecular Hydrogen
Hydrogen Phase Moles HydrogenAtom/cm3 Weight Percent
Solid Hydrogen (4.2K) 0.088 100%
Liquid Hydrogen (20K) 0.070 100%
Hydrogen Gas 200bar (300K) 0.016 ~1%
Frick Laboratory, Princeton University
Storage Options Standard steel tanks (2000-5000psi)
Known technology. Good Safety Record
Subject to hydrogen imbrittlement Forms projectiles if structure is breached
Tanks are challenging to fill because hydrogen heats upon expansion Heavy
Storage capacity is only 0.5-1% by weight Poor volumetric storage due to non-ideality of hydrogen:
P +n2aV2
⎛
⎝ ⎜
⎞
⎠ ⎟ V −nb( ) =nRT
a=0.2444 b=0.02661
~20% volumetric expansion at 5000psi
Frick Laboratory, Princeton University
Storage Options
Composite Tanks (~10,000psi) High storage capacity: Light weight Can store 7% H2 by weight! Does not fragment upon failure Cost
Frick Laboratory, Princeton University
Storage Options
Generation on the fly: in-situ or ex-situ reforming of hydrocarbon fuels using an on-site reformer. Energy density of gasoline Easy access to fuel (gasoline stations) Systems integration is poor No carbon mitigation.
Solid-state storage by intercalation (metal hydrides, carbons) Safe Heavy Expensive Chemical thermodynamics and kinetics are difficult
Significant heating is required to release the hydrogen∆H losses up to 30% are typical with operating temperatures of 200-300C. Tank filling is very exothermic Chemical kinetics are a difficult to handle
Frick Laboratory, Princeton University
Hydride Storage Capacity
Metal Hydride Storage Systems
Hydrogen Phase Moles HydrogenAtom/cm3 Weight Percent
LaNi5H6 0.091 1.37%
TiFeH2 0.10 1.89%
Mg2NiH4 0.098 3.6%
MgH2 0.11 7.6%
Frick Laboratory, Princeton University
Storage Options Chemical Hydrides
“Hydrogen on Demand” (Sodium Borohydride) Not flammable High Effective hydrogen pressure (~7000psi) Low Volume Simple system Chemical Safety Recyclable Cost??
NaBH4 + Aqueous Base Catalyst ⏐ → ⏐ ⏐ H2 + NaBO2 •2H2O