+ All Categories
Home > Documents > Transport Phenomena in Fuel Cells - Thermal-Fluids Central

Transport Phenomena in Fuel Cells - Thermal-Fluids Central

Date post: 04-Oct-2021
Category:
Upload: others
View: 3 times
Download: 0 times
Share this document with a friend
18
1 Transport Phenomena in Fuel Cells Chao-Yang Wang Electrochemical Engine Center (ECEC), and Department of Mechanical and Nuclear Engineering The Pennsylvania State University University Park, PA 16802
Transcript
Page 1: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

1

Transport Phenomena in Fuel Cells

Chao-Yang Wang

Electrochemical Engine Center (ECEC), andDepartment of Mechanical and Nuclear Engineering

The Pennsylvania State UniversityUniversity Park, PA 16802

Page 2: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

2

• Background and Societal Impact– FC is enabling technology for H2 economy– Automotive application for energy

independence– Micro/portable power for tether-free

electronics– FC interfaces with nanotech, IT, and bio-tech– FC is highly interdisciplinary system

requiring breakthroughs not only from materials science but also transport phenomena communities.

– FC physics is fascinating– Ability to control transport of reactants and

products is critical to FC performance, durability, and cost

Page 3: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

3

• Technical Principles– H2/air polymer electrolyte fuel cells

(PEFC)• H2 + O2 produces H2O• Operation temperatures: -40oC to 80oC• A large range of length and time scales• Power density reaches ICE

– Water transport and removal• Water transport thru ionomeric membranes• Liquid H2O transport through nano-pore

catalyst layer (CL), microporous layer (MPL), and gas diffusion layer (GDL)

• Impact of surface wettability (e.g. hydrophobic GDL)

• Two-phase flow in micro- and mini-channels, flow mal-distribution

Page 4: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

4

• Technical Principles (PEFC)– Coupled water and heat transport

• H2O vapor saturation pressure exponentially increase with temperature

• Evaporation/condensation – the heat pipe effect– Transient Behaviors

• Critical for PEFC startup, load change, gas purge during shutdown, and materials durability

• Time constants of membrane hydration/dehydration, membrane water diffusion, gas transport, GDL flooding and dewetting

– Subzero startup• Ice formation and melting in CL• Water transport properties at subfreezing T

Page 5: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

5

• State-of-the-Art (PEFC)

Water transport on CL

Ge & Wang, Electrochim. Acta, 2007

Capillary network theory Pore network modeling 2-phase LB simulation

In-situ imaging and quantification of liq. H2O saturation in GDL:• neutron radiography• NMR• X-ray microtomography

Page 6: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

6

• State-of-the-Art (PEFC)– Two-phase flow in channels and channel flooding

• Voltage loss due to channel flooding amounts to 120 mV and negates catalyst improvement (4x activity ⇒ 45 mV gain).• Fluctuation sets up voltage cycling at high potentials ⇒ Pt area loss + carbon corrosion

I=0.2 A/cm2

70/70/80oC150 kPa

0.4

0.5

0.6

0.7

0.8

0.9

1

0 20 40 60 80 100 120 140 160 180

Time (min)

E (

V)

0

0.3

0.6

0.9

1.2

1.5

1.8

∆ P (

kP

a)

ξ = 4 ξ = 3.5 ξ = 3 ξ = 2.5 ξ = 2

Page 7: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

7

Channel walls

(θ<45°)

GDL surface

(θ~110°)

Channel walls

(θ<45°)

GDL surface

(θ~110°)

Channel walls

(θ<45°)

GDL surface

(θ~110°)

Channel walls

(θ<45°)

GDL surface

(θ~110°)

Channel walls

(θ<45°)

GDL surface

(θ~110°)

Channel walls

(θ<45°)

GDL surface

(θ~110°)

Channel walls

(θ<45°)

GDL surface

(θ~110°)

Channel walls

(θ<45°)

GDL surface

(θ~110°)

(a) corner flow w/ droplets on GDL

(b) annular film flow w/ droplets on GDL

(c) slug flow w/ channel clogging

Gas flow

Page 8: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

8

• State-of-the-Art (PEFC)– Transients

Electro-osmoticDrag

Back-diffusion in membrane

sD OHm

mdiff 101.0~2

2

−= δτsEOD µτ 1~

Membrane hydration/ dehydration

sm 10010~ −τ

ANODEANODE

CATHODECATHODE

MEMBRANEMEMBRANEElectroosmoticDrag= d

InF

Back Diffusion Flux= w

CDδ

ProductionHH22OO

H2/H2O

Air/H2O y

T i m e ( s )

Cel

lvo

ltage

(V)

0 2 4 6 80

0 . 1

0 . 2

0 . 3

0 . 4

0 . 5

0 . 6

0 . 7

0 . 8

S t e p c h a n g e i n c u r r e n t d e n s i t y f r o m 0 . 1 t o 0 . 8 A / c m 2

S t e p c h a n g e i n c u r r e n t d e n s i t y f r o m 0 . 1 t o 0 . 6 A / c m 2

S t e p c h a n g e i n c u r r e n t d e n s i t y f r o m 0 . 1 t o 0 . 8 A / c m 2

S t e p c h a n g e i n c u r r e n t d e n s i t y f r o m 0 . 1 t o 1 . 0 A / c m 2

R H a / c = 5 0 / 0 %

R H a / c = 1 0 0 / 1 0 0 %

R H a / c = 5 0 / 0 %

R H a / c = 5 0 / 0 %

Temporary power loss upon load increase

Page 9: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

9

• State-of-the-Art (PEFC)– Cold Start

Gaspurge studies

Cold startup cycling

Advanced in-situ diagnostics: imaging ice formation, measuring ice

in CL, etc.

Durability tests & degradation analysis

Multiphase modeling of cold-start

ValidationPredicted Product Water (mg/cm2)

Exp

erim

enta

lPro

duct

Wat

er(m

g/cm

2 )

0.2 0.4 0.6 0.8 1.0 1.20.0

0.2

0.4

0.6

0.8

1.0

1.2

Eq. Purge, 30 µ m membrane, 40 mA, -20° CEq. Purge, 60 µ m membrane, 40 mA, -20° CEq. Purge, 30 µ m membrane, 100 mA, -20° CEq. Purge, 60 µ m membrane, 100 mA, -20° CDry Purge, 30 µ m membrane, 100 mA, -20° CDry Purge, 30 µ m membrane, 40 mA, -20° CEq. Purge, 30 µ m membrane, 40 mA, -30° CDry Purge, 30 µ m membrane, 100 mA, -30° C

+20%

-20%

200 µ m200 µ m200 µ m

Gore-Select Membrane

-20oC -30oC

Sub-zero

Gore-Select Membrane

-20oC -30oC

Sub-zero

Interfacial delamination after 110 cycles of cold-start at 500 mA/cm2

Page 10: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

10

• Barriers (PEFC)– Liq. H2O transport in CL

• Mixed wettability: hydrophilic/hydrophobic pores• Role of evaporation driven by heat generation• Removal of liq. H2O from CL

– Liq. H2O transport thru GDL• Impact of surface wettability and structure• What is structural building block of GDL?• Pore-level physics of water transport• In-situ measurements of liquid saturation in CL,

MPL and GDL w/ spatial resolution ~1 µm.– Micron-resolution sensing

• Current, humidity, temperature in-plane distributions between channel and land

• In-situ diagnostics of FC stacks using MEMS sensors in a bandage form

– How to maintain intricate water balance btw anode and cathode

Feunberger et al., J Electrochem. Soc. 2006

Page 11: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

11

• Technical Principles– Direct oxidation fuel cells (DOFC)

• Oxidation of liquid fuel (methanol, ethanol, DME, etc.) at anode

• High energy density and suited for consumer electronics applications

– Methanol & water crossover thru membrane

Conventional DMFC system

New DMFC system using low-α MEA

MeO

H c

ross

over

cu

rren

t den

sity

H2O crossover coeff. α

Wang & Liu (2006)

Page 12: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

12

• State-of-the-Art (DOFC)– Direct methanol fuel cells (DMFC)

• Power density ~ 120 mW/cm2 @ 0.4V• MeOH feed concentration 70-100% directly into anode• Fuel efficiency >80%• Total Pt loading ~ 3.5 mg/cm2

• 3,000 hr durability with <20% power fade• All the above together

– Direct ethanol fuel cells (DEFC)• Power density is half of DMFC @ 0.4V• Electrolyte and catalyst are under active pursuit• Limited to lower operating temperatures• Durability studies are in infancy

Page 13: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

13

• Barriers (DOFC)– Direct methanol fuel cells (DMFC)

• Fundamental understanding of water, methanol and heat transport in DMFC

• How to manipulate surface wettability and porous structures to control water crossover from the anode to cathode

• More compact, more efficient cell design– Direct ethanol fuel cells

• Complete oxidation of ethanol (with C-C bond)• Water management• Pt-free catalysts• Electrolytes: proton or alkaline anion type?• Durability of DEFC materials

Page 14: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

14

• Technical Principles– Solid oxide fuel cells (SOFC)

• SOFC R&D directions: lower operating temperatures, and internal reforming of HC fuel, especially CH4

• O2- ion conductivity is low. • Larger temperature distribution in through-

plane direction • Water is needed for reforming, WGS and

avoiding carbon deposition, but water is produced from H2 electro-oxidation.

Reforming reaction (endothermic) CH4 + H2O -> CO + 3H2 (steam reforming) CO + H2O -> CO2 + H2 (water gas shift)

CH4+H2O

H2O

H2

CH4

SOFC Anode

Steam reforming; WGSendothermic

Electro-oxidation

Page 15: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

15

• State-of-the-Art (SOFC)– CFD-based modeling of species, heat and charge transport on

cell level – Micro-models of transport phenomena in porous electrodes – Limited experimental characterization, especially distribution

data of current, species and temperature – Few studies on water and heat transport in the anode with

direct feed of HC fuel• Water is reactant of reforming reaction but product of

electrochemical reaction• Heat is consumed in reforming reaction but produced from

electrochemical reaction• Heat/water sink and source co-exist in HC fueled SOFC

Page 16: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

16

• Barriers (SOFC)– Multi-component transport models accounting for

competitive reactions in anode– Measurements of current, species and temperature

distributions, especially water vapor and temperature distributions in the anode

– Effective water and heat management– Understand and develop electrode microstructure-

performance relationship

Page 17: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

17

• Recommendations1. Novel concepts of water management for automotive fuel cells2. Understanding pore-level physics of water transport3. Multiscale models to predict electrode flooding and mass transport loss4. In-situ characterization techniques with micron-resolution5. Dynamic behavior of polymer electrolyte fuel cells6. Subzero startup of polymer electrolyte fuel cells7. Basic understanding of water, methanol and heat transport in direct

methanol fuel cells8. More compact, efficient DMFC designs9. Transport phenomena in direct ethanol fuel cells10. Models and experimental data of water and heat transport in SOFC 11. Understanding electrode microstructure-performance relationship

Page 18: Transport Phenomena in Fuel Cells - Thermal-Fluids Central

18

• References1. C.Y. Wang, Chemical Reviews, 104, 4727 (2004)2. K.D. Kreuer et al., Chemical Reviews, 104, 4637 (2004).3. J.H. Nam and M. Kaviany, Int J Heat Mass Trans., 46, 4595 (2003)4. U. Pasaogullari and C.Y. Wang, J Electrochem Soc., 151, A399 (2004)5. S.A. Freunberger et al., J Electrochem Soc, 153, A1258 (2006)6. X.G. Yang et al., Electrochem & Solid-State Lett., 7, A408 (2004)7. S. Ge and C.Y. Wang, Electrochim. Acta, 52, 4825 (2007)8. Y. Wang and C.Y. Wang, Electrochim. Acta, 50, 1307 (2005).9. P.K. Sinha et al., J Mater. Chem., in press, 2007.10. G.Q. Lu et al., Electrochem & Solid-State Lett, 8, A1 (2005)11. C.Y. Wang and F.Q. Liu, Chapter 10 in 2006 Small Fuel Cell Symp., Knowledge

Foundation, 2006.12. Gurau et al., AIChE J, 44, 2410 (1998)13. S. Um et al., J Electrochem Soc, 147, 4485 (2000)14. A.V. Virkar et al., Solid State Ionics, 131, 189 (2000)15. T. Thampan et al., J Electrochem Soc., 147, 3242 (2000)


Recommended