Bio-Mass
Anaerobic
Digester Fuel Cell System on Dairy Farms
It is well known that dairy farms are quite capable
of producing self-sufficient power through a remote stand-alone power system
consisting of an anaerobic digester and engine-generator.
However, combustion of fuel has led to environmentally harmful emissions,
and low energy efficiency. This and
other factors have led to a search for an alternative means to meet the energy
needs of dairy farmers, and in so doing, the fuel cell came to mind.
Our main concerns have been the emission of pollutants, maintenance, and
system efficiency. The fact that
energy (electrical and heat) can be obtained from hydrogen-rich gas e.g.
hydrocarbons, promising higher energy efficiency and cleaner emissions, makes
the fuel cell the more attractive energy producing alternative.
Let us consider a dairy farm that currently uses the anaerobic digester
engine-generator system to produce the needed heat and power, and only look at
an alternative (i.e. fuel cells) to the engine-generator component of an
anaerobic digester system on diary farms, then it is fair to say that the
equipment used e.g. plug flow digester, biogas storage equipment, milking
equipment, ventilation, lighting, etc. not directly related to the power
generator, will remain the same (i.e. the need for these equipment and the
electrical demand by these equipment will remain the same).
By implementing a fuel cell system in place of the engine-generator, the
aspects most likely to be affected are changes in energy efficiency
(electrical/heat), the need for maintenance, cleaner emissions and the reduction
of greenhouse gases into the atmosphere, and noise reduction which are the
expected benefits of a fuel cell system when replacing the engine-generator. To
help visualize the energy production process on dairy farms, Figure
1.1 is a flow diagram of an anaerobic digester CHP generating system.
Since the plug-flow digester is the most commonly
used digester on dairy farms; ultimately, the type of fuel cell will play an
important role in determining CHP capabilities, and the need for auxiliary
equipment e.g. reformers. This work
will provide general information on the different anaerobic digester and fuel
cell types, auxiliary equipment (e.g. reformer) if
some other digester fuel cell system is to be considered, as well as grid
interconnection requirements, etc. also included is a fuel cell circuit model.
However, the anaerobic digester fuel cell system this study is mainly concerned
with is the plug-flow digester SOFC (Solid Oxide Fuel Cell) system that
could potentially be used to meet the energy and environmental needs of dairy
farmers.
Benefits
of an Anaerobic Digester Fuel Cell System
Stricter environmental standards have actually
helped push the need for improving energy efficiency, conserving energy, and
reducing energy costs for dairy farm owners.
Implementing an anaerobic digester fuel cell system on dairy farms could
meet these needs and even prove to be beneficial in the years to come.
The expected benefits of such a system would include [1.1]:
-
Energy benefits:
CHP combined heat and power capabilities for high temperature
operating fuel cells, renewable energy production i.e. continuous supply of
fuel from cow manure, and higher energy efficiency
-
Environmental benefits:
Greenhouse gas emissions are reduced and odor control.
With a fuel cell, carbon dioxide emissions may be reduced by up to
49%, nitrogen oxide (NOx) emissions by 91%, carbon monoxide by
68%, and volatile organic compounds by 93% [1.2].
-
Noise reduction, improved reliability, and
lower system maintenance.
However,
the cost of a fuel cell system, ranging anywhere from $3,000-$6,000 per kW of
power generating capacity, is the main disadvantage today when compared to an
engine-generator. Depending on the
type of fuel cell used, reformers may be needed which would further add to the
complexity and cost of the fuel cell system.

REFERENCES
[1.1]
A. Ferguson, V. I. Ugursal. A
Fuel Cell Model For Building Cogeneration Applications. Canadian Residential
Energy End-use Data and Analysis Centre.
[1.2]
D. Scott. Advanced power
generation from fuel cells -implications for coal.
IEA Coal Research, 1993.
[1.3]
Y. Zhu, K.Tomsovic. Development
of models for analyzing the load-following performance of microturbines and fuel
cells. Elsevier, December 2001
[1.4]
C. Nelson, J. Lamb. Final
Report Summary: Haubenschild Farms
Anaerobic Digester. The
Minnesota
Project, August 2002.
Anaerobic
Digesters and Energy Production on Dairy Farms
The most common anaerobic digester found on a dairy
farm is the plug-flow type digester system.
Anaerobic (oxygen-free) digesters are designed to digest cow manure where
decomposition releases biogas products. How
this works is, a load of manure moves through the digester, typically it takes
20-25 days (retention time) for the methane producing bacteria to grow and
reproduce in sufficient quantities. During
this retention time, the methane producing bacteria in the organic waste is
allowed to break down the solids while releasing biogas which is comprised of
about 60% CH4, 40% CO2, and the highly corrosive H2S
at approximately 0.2% - 0.4% according to [2.1].
At the end of the retention time, the fully decomposed manure is removed
and replaced by a fresh manure load on a daily basis for continuous biogas
production.
Anaerobic
Digester Design Types
Each of the following digester design type is
capable of trapping biogas but differ in cost, climate suitability, and
concentration of manure solids they can digest as described below.
In general, anaerobic digesters should be kept at a normal operating
temperature of about 100 degrees F in order to function properly.
Although, higher temperature operation can speed up the process and
reduce tank volume; more species of methane producing bacteria exists at the
normal operating temperature. Further
more, higher temperature operation of a digester is more prone to upset and can
lead to further complications if close monitoring is not considered.
-
Covered
Digester consists of a manure storage lagoon with an impermeable
cover. The cover traps gas
produced during decomposition of the manure.
This design can be used for liquid manure having less than 2% solids
and require large lagoon volume and warm climate.
Least expensive.
-
Complete
Mixer Digester suitable
for all climate conditions. Capable
of processing 3% - 10% solids. The
manure is processed in a heated tank above or below ground.
A mechanical mixer keeps the solids in suspension.
This design is expensive to construct and can cost more than the
plug-flow digesters to operate and maintain.
-
Plug-flow
Digester handles solid
concentrations of 11% - 13%. Raw
manure is decomposed as it moves through the tank producing biogas.
An impermeable cover is used to trap the released biogas.
Heating pipes are used to circulate hot water at 25 40 degrees C
(77 104 degrees F) a temperature range suitable for methane producing
bacteria. The hot water can come
from recovered waste heat from an engine generator fueled with digester gas
or from burning digester gas directly in a boiler.
Reasons
for Using Biogas
There are several reasons for considering the use of biogas in fuel cells
to supply energy. First, the methane
(CH4) produced from biogas is of special interest because it is
readily available on dairy farms. Secondly,
usable energy (heat and electricity) can be obtained from biogas (about 60% CH4)
because of its similar composition to natural gas (98% CH4).
And finally, biogas can be purified and/or reformed before it is fed into
a fuel cell which will essentially allow us to have a wider selection of fuel
cell types to choose from.
Energy
Production from Biogas
Energy production will essentially depend on
the amount of biogas produced from the manure fed into the digester.
If we assume the cows are kept in an enclosed area most of the time and
manure collection to be very efficient, then Table 2.1, which provides
information on the amount of manure produced on a daily basis from various farm
animals, can be used to estimate e.g. the amount of manure collected, and
electricity produced from biogas, etc.
Table
2.1 Daily manure production
|
Animal
|
Size
(lbs)
|
Manure
Production Factor per animal
(lbs/day)
(ft3/day)
(gal/day)
|
Density
(lb/ft3)
|
|
Lactating
dairy cow
|
1000
|
110
|
1.774
|
13.27
|
62
|
|
Heifer
|
750
|
65
|
1.000
|
7.48
|
65
|
|
Dry
cow
|
1000
|
82
|
1.323
|
9.89
|
62
|
|
Swine
|
275
|
7.5
|
0.121
|
0.90
|
62
|
|
Sheep
|
100
|
4
|
0.063
|
0.47
|
63
|
|
Turkey
|
20
|
0.9
|
0.014
|
0.11
|
63
|
|
Horse
|
1000
|
50
|
0.794
|
5.94
|
63
|
As can be seen from the above table, a single dairy cow produces about
110 lbs of manure per day having a Total Solids (T.S.) content of about 13%.
About 80% of the 13% of Total Solids is Volatile Solids (V.S.) that can
potentially produce energy. It is
estimated that for each 100 lbs of manure fed to a digester about 4 lbs of
manure is converted into biogas and the rest leaves the digester as effluent
[2.2]. We can estimate the amount of
manure collected per day from dairy cows by:
(2.1)
where:
hp = proportion of
manure collected (%)
MPF = manure production factor (ft3/day/cow)
From
this, we can find the daily amount of biogas produced and thus the heating
value. From the heating value, the amount of electrical and heat energy that is
available for use, depending on the energy system used (i.e. engine-generator or
fuel cell system), can be calculated. With
the help of Tables 2.2 and 2.3 these quantities can be obtained through the
following:
(2.2)
where:
GPF = gas production factor
DGP = daily gas produced
Table
2.2 Retention time and Gas
Production Factor provided by [2.2]
|
HRT
(Retention time)
|
Gas
Production Factor
|
|
15
days
|
30
|
|
20
days
|
34
|
|
25
days
|
37
|
|
30
days
|
39
|
The
gas production factors listed in Table 2.2 depend on the retention time of the
collected manure. A retention time
of 25 days or up to one month is not unusual.
To a certain extent, the longer the retention time, the more biogas that
can be produced. From the daily gas
production, the following can be calculated:
(2.3)
Daily Heat Value (Btu/day) = DGP x heat value of
gas
(2.4)
(2.5)
(2.6)
where:
heat value of gas = the amount of heat energy available in Btu
t = on-line
time (%)
hengine
= electrical efficiency of engine-generator
hcell
= electrical efficiency of fuel cell type
eengine
= electrical energy produced from engine-generator (kWh/day)
ecell
= electrical energy produced from the fuel cell type (kWh/day)
A
list of heating values of gaseous fuels at various temperatures is given in
Table 2.3.
Table 2.3 Heating value of
different fuels at various temperatures in (Btu/ft3)
|
Fuel
|
25°C
|
80°C
|
150°C
|
200°C
|
650°C
|
1000°C
|
|
Methane
|
915.65
|
900.76
|
895.85
|
895.72
|
894.26
|
890.93
|
|
Biogas
(60% CH4)
|
549.39
|
540.46
|
537.51
|
537.43
|
536.55
|
534.56
|
|
Hydrogen
(2H2)
|
531.07
|
510.88
|
498.82
|
493.40
|
440.59
|
396.54
|
Table 2.4 Heating
value converted into (kWh/ft3) where 1 Btu = 2.9287x10-4
kWh
|
Fuel
|
25°C
|
80°C
|
150°C
|
200°C
|
650°C
|
1000°C
|
|
Methane
|
0.2682
|
0.2638
|
0.2624
|
0.2623
|
0.2619
|
0.2609
|
|
Biogas
(60% CH4)
|
0.1641
|
0.1614
|
0.1606
|
0.1605
|
0.1603
|
0.1597
|
|
Hydrogen
(2H2)
|
0.1555
|
0.1496
|
0.1461
|
0.1445
|
0.1290
|
0.1161
|
The heating values listed in Table 2.3 were
computed by using a Matlab script (energy_density.m) that found the available
free energy at various temperatures for the reactions below.
The available free energy was then converted into a heating value.
Hydrogen: 2H2
+ O2 "
2H2O (2.7)
Methane: CH4
+ 2O2 "
2H2O + CO2
(2.8)
We can use the information above to estimate energy
production, e.g. if a single dairy cow were to produce 110 lbs of manure this
would in turn produce about 65.6 ft3/day of biogas or 39.4 ft3/day
of methane with a retention time of 25 days.
At 25°C, using an engine generator with
an electrical efficiency of 25%, this would mean an electrical production of
about 2.64 kWh per day per cow from biogas having an energy density of 549.39
Btu/ft3. With a
constant flow of fuel and oxidant to a fuel cell, it would be ideal for all the
energy from the chemical reaction involving hydrogen, Equation (2.7), to be
available for use. Unfortunately,
this has yet to be obtained because of certain factors that affect the
performance of the fuel cell. However,
we can estimate the electrical production from a fuel cell by using the
electrical efficiency of the cell type used when fed with a constant flow of
hydrogen (from reformed biogas) and oxidant.
With that being said, the following Matlab script (electrical_production.m)
was created to do the following:
§
Computes the daily biogas production from
dairy cows dependent on the farm size and generates a plot.
Assumes a 30 day retention time and a 90% manure collection efficiency.
Figure 2.1.
§
Generates a plot of daily electrical
production from an engine-generator (
) using the daily biogas produced. Assumes
a 20% electrical efficiency, and 90% on-line time.
Figure 2.2.
§
Generates a plot to estimate the daily
energy production from different fuel cell types (
) and hydrogen gas. The energy
production shown in the plot is dependent on the operating temperature, and
electrical efficiency of the fuel cell type as noted in the figure.
Figure 2.3.
§
Generates a plot to estimate the daily
energy production using MCFC and SOFC from biogas.
Figure 2.4.
§
Generates a plot to estimate the daily
electrical energy production using MCFC and SOFC from methane (60% of biogas).
Figure 2.5
The
plots generated from electrical_production.m will allow us to estimate biogas
production, and make comparisons between the engine-generator and fuel cells in
terms of electrical production.
Efficiency
Comparison of Fuel Cells to Engine-Generators
In fuel cells, the electrochemical reaction
converts the chemical energy of the fuel into electrical and thermal energy to
achieve high efficiencies. In other
words, fuel cells generate electricity without burning
the fuel. This process, in
terms of energy efficiency, is not limited by temperature or what is called the
Carnot efficiency as in the engine-generator [2.3], see Appendix A.
Conventional power generation converts the chemical energy of the fuel
(e.g. natural gas) into thermal energy by combustion.
This thermal energy is transferred to a working fluid (e.g. water) that
will convert the thermal energy to mechanical energy with the help of special
engines (turbines). Finally, a
generator converts the mechanical energy to electrical energy.
This whole process is linked to and limited by the so-called Carnot
efficiency. Table 2.5 compares
typical fuel-to-power efficiencies of various types of prime movers.
These efficiency figures do not account for increases due to the use of
cogenerated heat.
|
Table
2.5 Typical fuel-to-power efficiency values provided by [2.1]
|
|
|
|
|
|
Power
Generator
|
|
Electrical
Efficiency
|
|
Spark ignition engine
|
|
18-25%
|
|
Compression ignition
engine (Diesel)
|
|
30-35% above 1 MW
25-30%
below 1 MW
|
|
Gas turbine
|
|
18-40% above 10 MW
|
|
Microturbine
|
|
25-35% below 1 MW
|
|
Steam boiler and turbine
|
|
6-35% above 20 MW
|
|
Fuel Cell
|
|
40-60% depending on the type used
|





Theoretically, fuel cells promise much higher energy efficiency (~ 60%
fuel-to-power efficiency, approximately 40% of energy produced is wasted as
heat) than the engine generator (~ 25% fuel-to-power efficiency, approximately
75% wasted as heat) as seen in Table 2.5. If
half of the wasted heat is recovered and used, we can say that using the
engine-generator considering cogeneration has an efficiency of about 62.5% and
the fuel cell would have a cogeneration efficiency of about 80%.
Determining the Efficiency of Fuel Cells
One of the primary reasons for considering the use
of the fuel cell is the capability of high energy conversion efficiency.
There are four aspects of efficiency that must be considered when
determining the efficiency of a fuel cell:
-
Voltage efficiency
-
Current efficiency
-
Free energy efficiency and
-
Comparative thermal efficiency
1. If a hydrogen-oxygen fuel
cell were to give a potential of 1.23 volts at 25°C
when producing current, then all the free energy of the reaction would be
completely converted to electrical energy and the cell would be running at a
voltage efficiency of 100%. However,
in practice, most hydrogen-oxygen fuel cells operating at 25°C
run at potentials in the range of 0.6-0.8V and if efficiency is defined by:
Such
cells are running at about 50-65% efficiency.
The operating voltage is simply measured during the operation of a cell.
The lower operating voltage is the result of activation, concentration,
and impedance losses.
2.
Current efficiency is based on an assumed stoichiometric equation and is
defined in several ways:
To
illustrate what is meant by current efficiency, consider the following balanced
reaction:
Anode: 2H2 D
4H+ + 4e-
Cathode: O2 + 4H+ +
4e- D
2H2O
Overall: 2H2(g) + O2(g)
g
2H2O
If
the sole product is to be H2O, then all the current produced from the
fuel cell consuming hydrogen should be used in forming H2O and the
current efficiency is 100%. If e.g.
any side products or intermediates are formed, then the end product is formed at
a lower efficiency. The following
are several reasons that result in a lower current efficiency:
-
Side reactions may occur which yield fewer
electrons
-
The reaction proceeds through a series of
consecutive reactions to the final end product, where some loss or build-up
of intermediates occurs.
-
Crossover reaction occurs between the fuel
and oxidant or the fuel is dissolved in the electrolyte.
-
Impurities in the fuel and/or oxidant stream
Most
practical fuel cells however are likely to use air as the oxidant and so having
a high current efficiency becomes a secondary need.
3. The free energy efficiency
(eG) compared to the voltage
efficiency offers a better measure of the chemical energy that is being
converted to electrical energy and can be defined as the fraction of the
available free energy that is converted to electric power.
To calculate free energy efficiency where DG
= -nFEand DG = -nFE it follows that:
4.
The comparative thermal efficiency (eT)
makes it possible to make the comparison of fuel cells to heat engines.
This is defined as:
Observe
that even when eG = 100%, the
comparative thermal efficiency of the fuel cell may still be less than 100%.
The following example is used to make a comparison of a fuel cell to heat
engine. Consider the reaction:
H2(g) + ½ O2(g) g
H2O(l)
For
which DG = -56.69 kcal and DH
= -68.32 kcal at 298°K,
it follows that a fuel cell with a free energy efficiency of 60% is as efficient
as a heat engine burning hydrogen at a thermal efficiency of
.
However, when electrical energy is required from a particular fuel, then
the efficiency of the fuel cell should be compared with the overall efficiency
of the heat engine burning the fuel and the generator converting mechanical
energy to electricity.
Heat
Recovery Utilization
Usable heat should be recovered from high
temperature operating fuel cells. About
40% of fuel energy from high temperature operating fuel cells is rejected as
waste heat. Recovery of this heat
for heating the digester, and space heating and hot water needs on the dairy
farm are essential. Properly sized
heat exchangers can recover about 7,000 Btus of heat per hour for each kilowatt
of generator load [2.2]. For
example, 140,000 Btu/hr of heat could be recovered from a cogenerator operating
at 20 kilowatts (7000 Btu/hr-kW x 20kW = 140,000 Btu/hr) using a heat exchanger.
Figure
2.6 is a diagram of a fuel cell cogeneration system.

Figure 2.6
Components of a fuel cell cogeneration system
Typical Energy Usage and Load Demand on a
Dairy Farm
The
equipment used is an important aspect to be considered for proper sizing of a
fuel cell system and the energy usage on a dairy farm will certainly depend on
the farm size. The energy usage
(electricity and heat) by a typical dairy farm can be categorized by the
equipment used and is summarized here. This
will provide baseline information on the types of equipment used that contribute
to the dairy farm electrical load. The
NYSERDA audit shows that the majority of the energy used by dairy farms is due
to milk production equipment that consists of milk cooling, water heating
equipment, and vacuum pumps, other sources of energy usage are due to lighting
and ventilation. All together, these
equipment, account for 92% of the total energy used on a dairy farm.
The remaining 8% will consist of feeding and manure handling equipment,
and miscellaneous uses. Generally,
the electrical energy consumption on a typical dairy farm ranges from 800 to
1200 kWh of electricity per cow annually, and averaging about 100 dairy cows in
size according to an energy audit for dairy farms across central and northern
New York. Figure 2.7 provided by
[2.1] shows the energy needs of a 100 cow dairy farm and the potential energy
that can be delivered by this farm size using a generator.
Also shown is the energy profile of a 600 cow dairy and the energy a farm
this size could potentially deliver.
Figure 2.7 Electricity use profile
for 100 and 600 cow dairies
Referring
back to the example we had earlier, the electrical production from the manure of
a cow is approximately 2.64 kWh per day, then 100 cows would have the potential
to deliver 11 kW of energy per day (
). This is close to what the energy
profile shows us as a dotted line at 17kW-18kW.
For a farm size of 600 cows, the potential energy that could be delivered
was calculated to be 66kW, a 44kW difference from the 110kW that is seen from
the profile. Nonetheless, the
profile does give us an idea of the daily energy demand needed by dairy farmers
for this study.
Fuel
Cell Sizing
To size a fuel cell one could use a load profile of
a dairy farm to determine sizing or if potential gas production has been
estimated, using the same idea for sizing an engine-generator the cogenerator
fuel cell should have one kilowatt of capacity per 600-650 cubic foot of daily
biogas production. For a 250-cow
dairy farm with a digester producing 15,000 ft3 of biogas per day, a
25 kilowatt fuel cell generator is suggested.
For continuously operated cogenerators, 1 kW of cogenerator capacity per
10 cow equivalents is also reasonable starting point.
Fuel
Cell System Components
A power generation fuel cell system may incorporate
several auxiliary devices required for operation and are listed below:
-
Auxiliary burner is used to provide
supplementary heat to the fuel processor for process heating if sufficient
thermal energy cannot be recovered from hot process streams.
-
Heat extraction equipment and exchangers
during operation, the fuel cell produces heat that must be extracted to
ensure that the stack remains at optimal temperature.
Extracted heat can be used for heating and domestic hot water
purposes. Heat exchangers will
transfer heat from streams requiring cooling to streams requiring heating.
-
Compressors and pumps some fuel cell
types may operate at pressures several times that of the ambient,
necessitating compressors and pumps.
-
Reformers converts hydrocarbons such as
methane into a mixture of hydrogen and carbon dioxide gases before fed to a
fuel cell
-
Gas flow controller the controller would
automatically adjust the gas flow rate when changes in biogas production
occur or when load demand changes.
REFERENCES
[2.1] P. Wright.
Overview of Anaerobic Digestion Systems for Dairy Farms.
Agricultural and Biological Engineering Department,
Cornell
University
.
[2.2] R.K. Koelsh, E.E.
Fabian, R.W. Guest, J.K. Campbell. Anaerobic
Digesters for Dairy Farms. Agricultural
and Biological Engineering Department,
Cornell
University
.
[2.3] W.J.
Jewell, P.E. Wright, N.P. Fleszar, G.Green, A. Safinski, A. Zucker.
Evaluation of Anaerobic Digestion Options for Groups of Dairy Farms in
Upstate
New York
. Department of Agricultural and
Biological Engineering,
Cornell
University
, June 1997.
[2.4]
renewable Energy World.
Renewable fuel cell power from biogas. http://www.jxj.com/magsandj/rew/2001_06/renewable_fuel_cell.html.
Nov-Dec 2001.
[2.5] C. Collar, T. Shultz, N.
Peterson, A. Wubishet, G. Higginbotham. Dairy
and Livestock Research Report.
California
Dairy Energy Project.
[2.6]
National
Fuel
Cell
Research
Center
. Fuel Cell Benefits. http://www.nfcrc.uci.edu/fcresources/FCexplained/FC_benefits.htm.
[2.7] K. R. Williams.
An Introduction to Fuel Cells. Elsevier
Publishing Company, 1966.
|