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Summer Course on Exergy and Its Applications
EXERGY ANALYSIS of
FUEL CELLS
C. Ozgur Colpan
July 2-4, 2012Osmaniye Korkut Ata Üniversitesi
OUTLINE• Introduction to fuel cells• Thermodynamics of fuel cells• Fuel cell irreversibilities and exergy destruction• Ohmic losses• Activation losses• Mass transport or concentration losses• Losses due to fuel crossover
• Efficiency of fuel cells• Exergy analysis of integrated fuel cell systems• Summary
2
Introduction• Fuel cell: An electrochemical device that
converts the energy of fuel into electricity• High efficiency• Low environmental impact
• Main components:• Anode• Cathode• Electrolyte
• Electrochemical reactions occur at the electrodes• Production and consumption of ions
• Ions are conducted from one electrode to the other through electrolyte
• Electrons are cycled via an external load.
Electrode
3
Introduction (Cont’d)• A single cell can produce only a small amount of power• Fuel cell stack: Combination of many single cells to
produce the desired power output• Generally done by connecting single cells in series using
bipolar plates• Bipolar plates forms air and fuel flow channels and conducts
electrons
4
Introduction (Cont’d)
Source: www.fuelcelltechnology.com
5
Introduction (Cont’d)
Source: Larminie and Dicks (2002)
6
Thermodynamics of Fuel Cells
V=Cell Voltage (V)I=Current Density (A/cm2)
Work is obtained from the transport of electrons across a potential difference and not from mechanical means.
7
Thermodynamics of Fuel Cells (Cont’d)Reversible Process1st Law:
Faraday constant=96485 CElectromotive force (EMF) or Reversible open circuit voltage (OCV)
Number of electrons transferred
2nd Law:
Combining 1st and 2nd Laws:
If we divide both sides with the number of moles of fuel utilized
Molar specific Gibbs free energy change of the reaction
8
How to find n?Example: PEMFC
Example: DMFC
Example: SOFC
Thermodynamics of Fuel Cells (Cont’d)
eHCOOHOHCH 66223
OHeHO 22 3665.1
OHCOOOHCH 2223 25.1
e2H2H 2
OHe2H2O5.0 22
OHOH 222 5.0
e2OHOH 22
2
22 Oe2O5.0
OHOH 222 5.0
Anode
Anode
Anode
Cathode
Cathode
Cathode
Overall
Overall
Overall
9
How to calculate ∆g?• Gibbs free energy depends on temperature, pressure,
and concentration
Thermodynamics of Fuel Cells (Cont’d)
Change in the molar specific Gibbs free energy of the reaction
Where
Chemical potential
Chemical potential in the standard state
ActivityFor ideal gases
For pure liquid
For example:
WhereChange in the molar specific Gibbs free energy of the reaction in the standard state
10
• EMF in terms of product and/or reactant activity is called Nernst Voltage. • It is the reversible cell voltage that would exist at a given
temperature and pressure
Thermodynamics of Fuel Cells (Cont’d)
Combine and
Nernst Voltage
11
Thermodynamics of Fuel Cells (Cont’d)
If all the pressures are given in bar, then
Example: Derivation of Nernst Voltage for SOFC
)(222 5.0 vOHOH
12
• We can also show Nernst voltage of the SOFC in terms of fuel utilization ratio and air utilization ratio.
• Fuel utilization ratio:
• Air utilization ratio:
Thermodynamics of Fuel Cells (Cont’d)
Nernst voltage becomes (Colpan et al., 2009):
13
Thermodynamics of Fuel Cells (Cont’d)
14
Fuel Cell Irreversibilities and Exergy Destruction• Entropy is generated due to irreversibilities in fuel cells. • Entropy generation rate may be written as follows after
combining first and second laws of thermodynamics.
• For a hydrogen fuel cell, entropy generation rate per molar flow rate of hydrogen utilized can be shown as (for 0D modeling):
For 1 mol of H2 utilized, 2F current is produced.
15
Fuel Cell Irreversibilities and Exergy Destruction (Cont’d)• The difference between Nernst voltage (reversible cell
voltage) and operating cell voltage is known as polarization or overpotential or voltage loss or irreversibility.
• There are four major irreversibilities in fuel cells.• Ohmic losses• Activation losses• Mass transport and concentration losses• Losses due to fuel crossover (e.g. in DMFCs)
• If we neglect the fuel crossover losses
16
Fuel Cell Irreversibilities and Exergy Destruction (Cont’d)• Using Guoy-Stodola theorem, specific exergy destruction
in a process may be shown as
• Hence, combining equations
• For high temperature fuel cells (e.g. SOFC), the operating cell voltage is generally higher than low temperature fuel cells (e.g. PEMFC), because the irreversibilities are smaller.
17
Fuel Cell Irreversibilities and Exergy Destruction (Cont’d)
A typical low temperature fuel cell A typical high temperature fuel cell
Source: Larminie and Dicks (2002)
18
Ohmic Losses• Caused by the resistance to the flow of ions through the
electrolyte and resistance to the flow of electrons. • Ohm’s law describes that there is a linear relationship
between voltage drop and current density.
Where
Resistivity of the materials (determined by experiments)
Length of the electron and ion paths (generally taken as the thickness of the conducting layer)
Area Specific ohmic Resistance
19
Ohmic Losses (Cont’d)Example: The electrolyte of the SOFC (YSZ)
Source: Colpan et al. (2009)
20
Activation Losses• Caused by the slowness of the reactions taking place on
the surface of the electrodes.• Different equations in literature
• From the most simple to the complex: a linear equation with constant coefficients, Tafel equation, and Butler-Volmer equation.
• Tafel Equation
• For a hydrogen fuel cell with two electrons transferred per mole
Tafel slope (Higher for a slower reaction)
Exchange current density (Higher for a faster reaction)
Charge transfer coefficient 21
Activation Losses (Cont’d)
Source: Larminie and Dicks (2002)
Tafel Plots for slow and fast electrochemical reactions
22
Activation Losses (Cont’d)Exchange Current Density• There is a continual backwards and forwards flow of
electrons from and to the electrolyte• At exchange current density, there is an equilibrium
between forward and backward reactions
• Higher the exchange current density, better the performance
Example: Cathode reaction of PEMFC
23
Activation Losses (Cont’d)• For a low temperature, hydrogen fed fuel cell, a typical
value for exchange current density is 0.1 mA cm-2 at the cathode and about 200 mA cm-2 at the anode.
• For SOFC• Butler-Volmer Equation• Assuming charge transfer coefficient for anode and
cathode as 0.5
• e.g. Exchange current density of anode: ~650 mA cm-2 Exchange current density of cathode: ~250 mA cm-
2 24
Mass Transport or Concentration Losses• When gases at the channels diffuse through the porous
electrodes, the gas partial pressure at the electrochemically reactive sites becomes less than that in the bulk of the gas stream. • Hence, a voltage drop occurs which is called concentration
polarization.
Limiting current density• The current density at which the fuel is used up at a rate equal to its maximum supply.• Can be found solving diffusion equations (e.g. Fick’s law)
25
Mass Transport or Concentration LossesExample: For SOFC
Where
26
Losses due to Fuel Crossover• Fuel crossover occurs when some fuel diffuses from the
anode through the electrolyte to the cathode.• This fuel reacts directly with the oxygen, producing no
current. • The term ‘mixed potential’ is often used to describe the
situation that arises with fuel crossover.• For example, for DMFC, it affects the cathodic activation
polarization.
Where Crossover current density
27
Case StudyPolarizations and specific exergy destruction for a SOFC
28
Efficiency of Fuel Cells• Electrical efficiency of a fuel cell
• Exergetic efficiency of a fuel cell
• Maximum electrical efficiency of a fuel cell
• Fuel cells are not subject to Carnot efficiency.
29
Efficiency of Fuel Cells (Cont’d)
Source: Larminie and Dicks (2002)
Note: Fuel cell efficiency shown is relative to HHV.30
Exergy Analysis of Integrated Fuel Cell SystemsAPPROACH• Draw the control volumes enclosing a component or several
components of the system • Calculate the flow exergies of each state (Physical+Chemical
exergies if other exergy components are negligible)• Apply exergy balances around the control volumes to find
the exergy destruction in those control volumes• Compare the exergy destruction in a control volume to the
total exergy destructions within the overall system• Compare the exergy destructions and losses to the chemical
exergy of the fuel• Calculate the exergy efficiency of the integrated system
31
Exergy Analysis of Integrated Fuel Cell Systems (Cont’d)Case Study: Integrated SOFC and Biomass Gasification
System
Source: Colpan et al. (2010) 32
Exergy Analysis of Integrated Fuel Cell Systems (Cont’d)
The physical and chemical exergy flow rates:
The exergy balance:
The exergetic efficiency of the system:
De
eei
iicvj
jj
o xEexnexnWQTT
10
)s(sT)h(hex oooPH
kkoCHkk
CH xxTRxexex ln
)(,15, 2 lOHchOHCch
processnet
enxE
xEW
zyx
fgCH hmLHVex 1
CO
CNCHCOCH/4124.01
/0493.0/0531.01/3493.0/016.0044.1
(for all substances)
(for ideal gas mixtures)
(for CxHyOz)
(for O/C<2)(Szargut, 2005)
33
Exergy Analysis of Integrated Fuel Cell Systems (Cont’d)
Exergy loss ratios
Performance assessment parametersFUE PHR
Case1: Air 18.5% 63.9% 0.409 30.9%Case2: Enriched O2 19.9% 60.9% 0.487 30.7%Case3: Steam 41.8% 50.8% 4.649 39.1%
Exergy destruction ratios
34
Summary• Reversible open circuit voltage (OCV) or Electromotive force
(EMF) depends on the change in the Gibbs free energy of the overall reaction and the number of electrons transferred.
• Nernst voltage is the EMF written in terms of product and/or reactant activity.
• The difference between the reversible OCV and operating cell voltage is known as polarization or overpotential or voltage loss or irreversibility.
• Four major irreversibilities in fuel cells are: ohmic losses, activation losses, mass transport or concentration losses, and fuel crossover losses.
• For high temperature fuel cells, the maximum theoretical efficiency can be lower than the Carnot efficiency.
• Exergy analysis is an useful tool to find the exergy destructions and losses, and exergetic efficiency of integrated fuel cell systems.35