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Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523
www.ijera.com 516 | P a g e
A Simulation of Effects of Compression Ratios on the Combustion
in Engines Fueled With Biogas with Variable CO2 Concentrations
Bui Van Ga, Tran Van Nam, Tran Thanh Hai Tung
The University of Danang
ABSTRACT
The structure of conventional engines is maintained while they are converted to biogas- powered engines so that
they can reuse petroleum as fuel when needed as before conversion. In this case the detonation problem should
be treated. This paper simulates the effects of compression ratio on the combustion in the engines fueled with
biogas containing different CO2 concentrations. The results show that the compression ratio strongly influences
the pressures at the end of combustion processes, but it presents some effect on the final combustion
temperatures and on heat release curves. With a given compression ratio of 12, the temperatures and pressures at
the end of combustion in engines decrease by 473K and 2 MPa respectively; while, the molar concentration of
CO2 in the fuel increases from 20% to 40%.
Keywords – Biogas, Combustion, Compression ratio, Engine, Simulation.
I. Introduction
Biogas is a renewable fuel produced from
organic waste. After being filtered from harmful
impurities such as H2S, biogas can be used as fuel for
engines like natural gas. The use of biogas as fuel
without increasing concentrations of greenhouse
gases in the atmosphere contributes to the limitation
of global warming [1].
The use of biogas as an alternative fuel for
gasoline in electricity generation and in providing
power for production and life in rural areas bring
practical benefits to the economy and environmental
protection. In fact, owing to production requirements,
people use many different types of engines with
widely varying power ranges, so the conversion of
the engines available fueled with biogas is diverse
and their effective operation is also various [2].
The world today has seen the manufacture
and commercialization of specialized engines using
biogas as fuel such as GE Energy Jenbacher,
Australia, with a capacity of 330kW to 3MW, or
Jinan Diesel Engine Co., Ltd. Chinese manufacture
of biogas engines has been used exclusively with a
capacity of 150-660kW. The engine designed for
biogas is usually much more expensive than gasoline
engines using conventional oil. Yanmar Co. (Japan)
has commercialized a generator powered by biogas
(from December 2007) at the price of 106,000 USD
for an engine with a capacity of 25kW [3]. Or at the
Shandong Power Machinery Company of China [4]
commercialization of biogas-powered generators
with the output of 120kW to 500kW costs from
52,000 USD to 137,000 USD, three times more
expensive than diesel generators of the same size
(compared to the price of the site [5], CUMMINS
diesel generators CW 150S, 150 KVA are valued at
16,479 USD each
and a diesel engine costs 43,406 USD 600 KVA).
Biogas used as fuel for these engines must meet
certain conditions such as fuel composition, supply
pressure... One important drawback is that the
engines only work with biogas and can not work with
a liquid fuel.
Some small-sized biogas-powered engines
(capacity of about a few kilowatts) made in China
(such as Feigue Engine with the capacity of 2kW),
imported into our country has a simple structure,
operates on the principles of a spark-ignition engine
and shows many disadvantages in operation. Because
biogas is provided directly to the engine through a
simple carburetor and the load is adjusted by
changing the mixture of supply to the engine
(adjusted for quantity) without the impact of the
biogas rate speed, its engine is not stable, especially
when it shuts down on sudden increased load. On the
other hand, because there is no device to adjust the
quantity of biogas to the engine in order that normal
working pressure of the fuel supply to the engine can
be stabilized. Some small gasoline and biogas
engines manufactured in China (such as Huawei
engines with the capacity of 3kW HW3500) have
similar disadvantages due to the lack of biogas
quantity control systems provided by biogas engine
load.
Through the research on biogas engine
applications above we have discovered that :
- Biogas, a renewable energy source, has been
increasingly used all over the world. Biogas used
as fuel for generators and vehicles has been
applied in developed countries.
- Special motors designed to run on biogas (not
fueled with gasoline or diesel) have higher costs
than similar-sized diesel engines.
- Small engines running on biogas simply do not
RESEARCH ARTICLE OPEN ACCESS
Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523
www.ijera.com 517 | P a g e
work stably because of the lack of the devices
that control the flow rate of biogas.
- The world’s popular biogas-powered engines
that operate on the principles of forced ignition
engines; dual fuel engines -- biogas / diesel -- are
still not popular.
- Universal kits to convert the engines that use
liquid fuel to the engines that use biogas as fuel
have not been commercialized on the market.
The biogas engines available on the world
market as mentioned above are not suitable for use in
Vietnam. Indeed, due to power supply instability, all
the production units must be equipped with backup
generators. Investment in a generator running on
biogas only with a much higher price than diesel
generators as shown above is not economical.
However, with only one backup generator, one can,
on one hand, use biogas to generate electricity for
economical reasons and, on the other hand, can still
run on petroleum fuel when biogas is lacking and
there is loss of grid power. Therefore, a backup
engine is required to run on with both biogas and
petroleum fuel.
To meet the needs for biogas-powered
generators in our country, we need to apply a
technology to convert gasoline engines, diesel
engines used in two biogas fuel/ gas, biogas/ diesel
with different capacities. It is necessary to develop
conversion kits of biogas fuel/ multipurpose oil.
The center has researched and experimented
successfully the reform plan of gasoline-powered
engines to run on biogas with the universal kit
GATEC-20 (Fig.1) and GATEC-21 (Fig.2) [6] . Once
the kit is fitted into the engine, the principles and
structure of the original engines have not changed, so
the engine can use the gasoline and oil as necessary
as before the conversion. It can be said that the
converted engines are dual fuel engines powered by
biogas / diesel or biogas/ gasoline.
The GATEC technology [7] to overcome the
above disadvantages of biogas engines is available on
the market. Besides, the universal kit of GATEC
allows the conversion of biogas fuel/ liquid fuel for
most types of widely-used stationary internal
combustion engines (petrol, diesel, a cylinder, multi
cylinders, turbocharged, not supercharged,...) and
changes a wide range of capacities from a few kW to
hundreds of kW.
In terms of economical reasons, The
GATEC technology has brought many practical
benefits for users:
- It is not necessary to equip with an expensive
engine to run on biogas, which has the same
capacity with a backup engine. This will save
money and avoid the trouble of switching the
power system between the two generators.
- It is possible to make use of biogas to generate
electricity with unlimited volume. When the
biogas source runs out, the generator can be
converted to run on gasoline or diesel.
- It does not need to waste on biogas as in the
GATEC technology. In this way we can avoid
the waste of energy and ensure safety and
environmental protection.
- The engines converted to biogas engines can
consume an average of 1 cubic meter of biogas
to generate 1kWh of electricity. This will save
0.4 litre of gasoline and reduce the emission of 1
kg of CO2 into the atmosphere.
As shown above, the GATEC technology
can enable us to convert gasoline or diesel engines
Figure 3. A forced ignition engine running on
biogas was converted from a gasoline engine
Figure 1. GATEC20 Kit
Figure 2. GATEC21 Kit
Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523
www.ijera.com 518 | P a g e
with a wide range of capacities to biogas-powered
engines. Owing to the specific features of biogas fuel
supply in different combined measures, the economic
value of the engine also changes [8]. Biogas forced
ignition engines do not need liquid fuel injection
(Fig.3). Whereas, dual fuel engines running on biogas
converted from diesel engines need a minimum
amount of pilot diesel injection for ignition (Fig.4).
One of the important requirements for
converting a traditional engine to a dual fuel engine --
biogas/ fuel oil -- is that it does not change the
components of the engine so that it can re-use liquid
fuel when needed. This is related to the treatment of
the engine knock when it runs on biogas.
In fact, the fuel of biogas is methane which
has high anti-knock properties. Therefore, when this
fuel is used for biogas engines converted from
gasoline engines, we do not need to apply technical
treatment on detonation. However, for a dual fuel
engine converted from a diesel engine, anti-knock
becomes an important issue which should be handled
to ensure the normal operation of the engine.
The anti-knock properties of the engine
depends on the compression ratio and fuel
composition. In the previous work, we have studied
the effects of biogas composition on continuous
biogas combustion in an open space [9]. In the
following section, we will present the results of a
simulation study of the compression ratio effect on
the combustion engine that runs on the biogas
containing different CH4 concentrations.
II. Simulation of Biogas Combustion in
the Engine Combustion Chamber
In this study, we assume that combustion
occurs in the constant volume combustion cap-
shaped chamber with ignition at the top (Fig.5).
When the combustion occurs in a very short time
compared with the operation of the piston stroke, we
can see that the volume combustion chamber is
constant.
The compression process in the engine is
assumed to be the polytropic compression with the
average polytropic index of n = 1.3. If the
temperatures and pressure at end of the intake
process are Ta and Pa, the temperatures and pressure
at the end of the compression process are
1n
ac TT 
 and
n
ac pp  .
Table 1. Variable temperatures and pressure at the
end of the compression processes in terms of
compression ratio (Ta=325K, pa=0,95 Bar)
Tc(K) pc(Bar)
9 628 17
10 648 19
11 667 21
12 685 24
13 702 27
14 717 29
15 732 32
16 747 35
17 760 38
18 774 41
Table 1 introduces variations of temperatures and
pressure at end of the compression processes versus
the compression ratio of the engine when the intake
is: Ta=325K, pa=0,95Bar.
Simulations are carried out by using the
FLUENT Software, the model of "partial premixed"
combustion in the 3D chamber space. The standard k-
combustion chamber with coefficients: c =0.09,
c1=1.44 and c2=1.92. The speed of layer flame is
assumed to be 2m/s.
The initial mixture is unburnt gas, so the
“variable progress" c = 0 (Fig. 6). On changing
biogas with different CH4 concentrations, we need to
adjust f to have the same ratio of “mixture” . The
biogas fuel used is symbolized MxCy, where x is the
percentage mol of CH4 and y is the percentage of CO2
mol. Table 2 shows the value of f when equals
1.13 with different biogas fuel components.
Figure 5. Cap-Shaped Chamber Used in Simulation Study
Figure 4. A dual fuel engine powered by diesel/
biogas -- converted from a diesel engine
Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523
www.ijera.com 519 | P a g e
The input data of each case include
pressures and temperatures at the end of compression
processes, the mixture components of f. The
thermodynamic parameters of the fuel mixture with
the air-fuel biogas with a different set of
thermodynamics of the PrePDF table before
performing the calculation.
Table 2. The value of f when
to the biogas fuel with different components
Types of fuel M60C40 M70C30 M80C20
f 0,156 0,125 0,100
Combustion is started by assumed sparks with the
energy Eig = 0.1 J. After ignition, the flame spreads
slowly from the spark center to the farthest point of
ignition of the combustion chamber. Computation
time step is chosen dt = 0.001s. At each calculation,
we determine the temperature, average pressure
throughout the combustion chamber, the
concentration of CH4 and O2 and the products of
combustion as well as the speed of air movement in
the combustion chamber. Fig.7 introduces the results
of a combustion mixture of air and biogas engine
M70C30 with
the section apart 2ms axis passing through the
combustion chamber. The data include the mass
concentration of CH4, CO2, the temperature of the
mixture and the movement speed of air in the
combustion chamber. This result shows that, after
catching fire, the flame quickly spreads to the
membrane from the ignition center. The
concentration of CH4 in the fire area reduces
quickly, while the CO2 generated increases rapidly.
The combustion chamber is divided into two
sections: The burnt gas section and the unburnt gas
section, which are separated from each other by the
surface of the flame. The high-temperature zone of
Figure 6. Adjustment of average mixture
component of f to get an equivalent
coefficient of the given mixture 
3ms
5ms
7ms
9ms
11ms
13ms
15ms
17ms
19ms
CH4 CO2 T(K) V(m/s)
Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523
www.ijera.com 520 | P a g e
the burnt mixture spreads gradually corresponding to
the shift of the flame.
As temperatures in the combustion zone
rise, combustion products expand and compress
unburnt gas mixture toward the front, forming a
high-speed zone around the fire flame.
III. Results and Discussion
Fig.8 and Fig.9 introduce variable average
concentrations of CH4 and O2 in the engine
combustion chamber corresponding to the engines
with compression ratios of 9, 12 and 15. When the
engine compression ratios increase, the density of
the mixture in the combustion chamber increases
accordingly. This makes the speed of combustion
(mixture consumption rate) decrease. This represents
a change in the slope of the curve of varying
concentrations of CH4 and O2 over the time.
0
1
2
3
4
5
6
0 5 10 15 20 25 30
CH4(%)
t (ms)
=15
=12
=9
Figure 8. The effect of the compression ratio on the
concentration of CH4 in the combustion chamber
(fuel:M80C20)
0
4
8
12
16
20
24
0 5 10 15 20 25 30
O2(%)
t (ms)
=15
=12
=9
Figure 9. The effect of the compression ratio on the
concentration of O2 in the combustion chamber
(fuel:M80C20)
500
1000
1500
2000
2500
3000
0 5 10 15 20 25 30
t (ms)
=15
=9
=12
T (K)
Figure 10. The effect of the compression ratio on the
average temperature of the mixture in the
combustion chamber (fuel:M80C20)
0
2
4
6
8
10
12
0 5 10 15 20 25 30
t (ms)
P (MPa) =15
=12
=9
Figure 11. The effect of the compression ratio on the
average pressure variations in the combustion
chamber (fuel: M80C20)
The change of combustion speed in
accordance with the compression ratio leads to
change in the speed of heat release, so the contour
curves of temperature variation may also be slightly
changed with the engine compression ratios (Fig.10).
The effect of the compression ratios on the
combustion processes of internal combustion
engines is clearly shown in the curve of average
6
2
4
3
5
CH4(%) CO2(%)
12
9,5
7,0
4,5
2,0
T(K)
2700
2200
1700
1200
700
V(m/s)
2,0
1,5
1,0
0,5
0,0
Figure 7. Variations of average concentrations
of CH4, CO2, temperature and speed of the
mixture in the combustion chamber with =12
and M70C30 fuel
Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523
www.ijera.com 521 | P a g e
pressure variations in the combustion chamber.
Figure11shows that the maximum pressure at the
end of combustion processes changes vehemently in
accordance with the compression ratio. According to
the equation of the ideal gas state PV = NRT, when
the volume V and temperature T are unchanged, the
pressure relies on the number of moles of gas n. In
other words, it depends on the density of the mixture
in the combustion chamber before ignition. Since the
temperature at the end of the combustion processes
corresponds to the engines of same combustion
chamber volumes and different compression ratios
slightly change, the pressure at the end of
combustion processes is in proportion to engine
compression ratios.
The temperature of the mixture before
combustion significantly affects the pressure
variations in the engine combustion chamber. Fig.12
compares the variable pressure chamber in the
engine compression ratio =9 and =12 in both the
initial temperature Tc = 628K and Tc = 685K.
Together with the engine compression ratio, the
higher initial temperatures are, the lower the
pressures at the end of the combustion become.
0
1
2
3
4
5
6
0 5 10 15 20 25 30
CH4(%)
t (ms)
M80C20
M70C30
M60C40
Figure 13. Influences of biogas on average fuel
composition pressure variations of the mixture in the
2
4
6
8
10
12
14
16
18
20
0 5 10 15 20 25 30
CO2(%)
t (ms)
M80C20
M70C30
M60C40
Figure 14. Influences of biogas on average fuel
composition pressure variations of the mixture in the
combustion chamber
500
1000
1500
2000
2500
3000
0 5 10 15 20 25 30
t (ms)
T (K) M80C20
M70C30
M60C40
Figure 15. Influences of biogas components on the
average temperature variations of the mixture in the
t (ms)
P (MPa) M80C20
M70C30
M60C40
2
4
6
8
10
0 5 10 15 20 25 30
Figure 16. Influences of biogas components on the
average fuel composition pressure variations of the
mixture in the combustion chamber (compression ratio
The same compression ratio engines, biogas
fuel components strongly influence the combustion
of the engine. Fig.13 and Fig.14 introduces
variations of the average concentrations of CH4 and
0
2
4
6
8
10
12
0 5 10 15 20 25 30
t (ms)
=12
P (MPa)
=9
Ti=685K
Ti=628K
Ti=685K
Ti=628K
Figure 12. Influence of initial temperature on the
variation of pressure in the combustion chamber with
different compression ratios (fuel M80C20)
Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523
www.ijera.com 522 | P a g e
CO2 in the combustion chamber with fuel types such
as M60C40 and M70C30 and M80C20. For rich
biogas, CH4 burns almost completely at the end of
the combustion processes. When the CO2
components in the fuel increase, CH4 concentration
remaining in the mixture also increases. Although
the amount of fuel burnt is reduced, the amount of
CO2 in the mixture is initially high for poor fuel and
CO2 in the mixture significantly increases. This
shows that the concentration of CO2 in a strong
influence on combustion processes, thus affecting
the heat release in the combustion chamber.
Fig.15 and Fig.16 introduces the effect of
biogas on fuel composition variations in the
temperatures and pressures in the engine combustion
chamber with a compression ratio of
biogas, CO2 in the fuel component hinders the
exposure of oxygen and CH4 as bad combustion
processes resulting in the amount of unburned CH4
in emissions increased. Consequently, the
temperatures and pressures at the end of the
combustion processes decline. Fig.17 shows that the
average maximum temperatures of the mixture at the
end of the combustion processes decrease from
2565K down to 2092K (down by 473K) when the
moles of CO2 in biogas increase from 20% to 40%.
Corresponding to the increase in the concentration of
moles of CO2, the maximum pressure at the end of
the combustion mixture decreases from 9.3 MPa to
7.3 MPa (lower 2MPa) (Fig.18).
Simulation results show that the
concentration of CO2 in the biogas fuel has a strong
influence on the combustion engine, especially the
speed of heat release. This affects the anti-knock
properties of the mixture. Therefore, when
converting a conventional engine to use biogas
without changing the compression ratio of the
engine, we can adjust the concentration of CO2 in
the fuel to control the phenomenon of detonation.
2000
2200
2400
2600
20 24 28 32 36 40
Tmax (K)
% CO2 (mol/mol)
Figure 17. The effect of CO2 component in biogas
fuel on temperatures at the end of combustion
processes
7
7,5
8
8,5
9
9,5
20 24 28 32 36 40
pmax (MPa)
% CO2 (mol/mol)
Figure 18. The effect of CO2 component in biogas
fuel on pressures at the end of combustion
1. Conclusion
The results of this study enable us to draw the
following conclusions:
1. When the compression ratio engine powered
by biogas ranges from 9 to 15, the end of the
combustion pressure increases in proportion
to the compression ratio, but the heat release
curve at the end of the combustion
temperatures in this case is less affected by
the compression ratio.
2. With the same engine compression ratio
given, the biogas fuel components affect the
speed of combustion, temperatures as well as
pressure at the end of the combustion process.
The concentration of CH4 at end of the
combustion processes increases the
concentration of CO2 in the fuel.
The CO2 components in the biogas fuel are
adjustable to control the detonation in the conversion
of conventional engines of high compression ratios
to the engines fueled with biogas.
REFERENCES
[1] B.V. Ga, L.M Tien, T.L.B Tram, N.V.
Dong, Limitation of Emissions of
Greenhouse Gases with the Application of
Biogas Technology to Internal Combustion
Engines, Proceedings of Scientific
Researches at the Eight National
Conference on Mechanics, Volume 1,
Hanoi, 2009, 383-392.
[2] B.V. Ga, T.V. Nam, N.T.T Xuan,
Utilization of Biogas Engines in Rural
Areas: A Contribution to Climate Change
Mitigation, Colloque International
RUNSUD 2010, Universite Nice-Sophia
Antipolis, France, 2010, 19-31.
[3] (http://vietbao.vn/Khoa-hoc/May-phat-
dien-sach/45265746/188/)
[4] (http://www.sdxsgs.com)
[5] http://www.vatgia.com
[6] B.V. Ga, T.V. Nam, L.X Thach, A
Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523
www.ijera.com 523 | P a g e
Simulation of the Flow through the Mixture
Creation Kit for Forced Ignition Biogas-
Powered Engines by Fluent Software,
Journal of Science and Technology,
Universities of Technology, Issue 80,2011,
134-138.
[7] B.V. Ga, Patent for an Invention No 9433,
The Variable Speed Adjuster for Biogas
Stationary Motors Converted from Diesel
Motors, Issued by Intellectual Property
Department on July 11th
, 2011.
[8] B.V. Ga, L.M. Tien, L.X Thach,
Comparison of the Effectiveness of
Measures to Provide Biogas for Internal
Combustion Engines, Journal of Science
and Technology, University of Danang,
No. 2 (37), 2010, 65-72.
[9] B.V. Ga, T.V. Nam, L.M. Tien, An
Investigation into the Effect of CO2 on the
Combustion Process in Dual Fuel Biogas-
Propane Combustion Chamber 3-D,
Journal of Science and Technology,
Universities of Technology, Issue 81, 2011,
96-102.

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Cq35516523

  • 1. Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523 www.ijera.com 516 | P a g e A Simulation of Effects of Compression Ratios on the Combustion in Engines Fueled With Biogas with Variable CO2 Concentrations Bui Van Ga, Tran Van Nam, Tran Thanh Hai Tung The University of Danang ABSTRACT The structure of conventional engines is maintained while they are converted to biogas- powered engines so that they can reuse petroleum as fuel when needed as before conversion. In this case the detonation problem should be treated. This paper simulates the effects of compression ratio on the combustion in the engines fueled with biogas containing different CO2 concentrations. The results show that the compression ratio strongly influences the pressures at the end of combustion processes, but it presents some effect on the final combustion temperatures and on heat release curves. With a given compression ratio of 12, the temperatures and pressures at the end of combustion in engines decrease by 473K and 2 MPa respectively; while, the molar concentration of CO2 in the fuel increases from 20% to 40%. Keywords – Biogas, Combustion, Compression ratio, Engine, Simulation. I. Introduction Biogas is a renewable fuel produced from organic waste. After being filtered from harmful impurities such as H2S, biogas can be used as fuel for engines like natural gas. The use of biogas as fuel without increasing concentrations of greenhouse gases in the atmosphere contributes to the limitation of global warming [1]. The use of biogas as an alternative fuel for gasoline in electricity generation and in providing power for production and life in rural areas bring practical benefits to the economy and environmental protection. In fact, owing to production requirements, people use many different types of engines with widely varying power ranges, so the conversion of the engines available fueled with biogas is diverse and their effective operation is also various [2]. The world today has seen the manufacture and commercialization of specialized engines using biogas as fuel such as GE Energy Jenbacher, Australia, with a capacity of 330kW to 3MW, or Jinan Diesel Engine Co., Ltd. Chinese manufacture of biogas engines has been used exclusively with a capacity of 150-660kW. The engine designed for biogas is usually much more expensive than gasoline engines using conventional oil. Yanmar Co. (Japan) has commercialized a generator powered by biogas (from December 2007) at the price of 106,000 USD for an engine with a capacity of 25kW [3]. Or at the Shandong Power Machinery Company of China [4] commercialization of biogas-powered generators with the output of 120kW to 500kW costs from 52,000 USD to 137,000 USD, three times more expensive than diesel generators of the same size (compared to the price of the site [5], CUMMINS diesel generators CW 150S, 150 KVA are valued at 16,479 USD each and a diesel engine costs 43,406 USD 600 KVA). Biogas used as fuel for these engines must meet certain conditions such as fuel composition, supply pressure... One important drawback is that the engines only work with biogas and can not work with a liquid fuel. Some small-sized biogas-powered engines (capacity of about a few kilowatts) made in China (such as Feigue Engine with the capacity of 2kW), imported into our country has a simple structure, operates on the principles of a spark-ignition engine and shows many disadvantages in operation. Because biogas is provided directly to the engine through a simple carburetor and the load is adjusted by changing the mixture of supply to the engine (adjusted for quantity) without the impact of the biogas rate speed, its engine is not stable, especially when it shuts down on sudden increased load. On the other hand, because there is no device to adjust the quantity of biogas to the engine in order that normal working pressure of the fuel supply to the engine can be stabilized. Some small gasoline and biogas engines manufactured in China (such as Huawei engines with the capacity of 3kW HW3500) have similar disadvantages due to the lack of biogas quantity control systems provided by biogas engine load. Through the research on biogas engine applications above we have discovered that : - Biogas, a renewable energy source, has been increasingly used all over the world. Biogas used as fuel for generators and vehicles has been applied in developed countries. - Special motors designed to run on biogas (not fueled with gasoline or diesel) have higher costs than similar-sized diesel engines. - Small engines running on biogas simply do not RESEARCH ARTICLE OPEN ACCESS
  • 2. Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523 www.ijera.com 517 | P a g e work stably because of the lack of the devices that control the flow rate of biogas. - The world’s popular biogas-powered engines that operate on the principles of forced ignition engines; dual fuel engines -- biogas / diesel -- are still not popular. - Universal kits to convert the engines that use liquid fuel to the engines that use biogas as fuel have not been commercialized on the market. The biogas engines available on the world market as mentioned above are not suitable for use in Vietnam. Indeed, due to power supply instability, all the production units must be equipped with backup generators. Investment in a generator running on biogas only with a much higher price than diesel generators as shown above is not economical. However, with only one backup generator, one can, on one hand, use biogas to generate electricity for economical reasons and, on the other hand, can still run on petroleum fuel when biogas is lacking and there is loss of grid power. Therefore, a backup engine is required to run on with both biogas and petroleum fuel. To meet the needs for biogas-powered generators in our country, we need to apply a technology to convert gasoline engines, diesel engines used in two biogas fuel/ gas, biogas/ diesel with different capacities. It is necessary to develop conversion kits of biogas fuel/ multipurpose oil. The center has researched and experimented successfully the reform plan of gasoline-powered engines to run on biogas with the universal kit GATEC-20 (Fig.1) and GATEC-21 (Fig.2) [6] . Once the kit is fitted into the engine, the principles and structure of the original engines have not changed, so the engine can use the gasoline and oil as necessary as before the conversion. It can be said that the converted engines are dual fuel engines powered by biogas / diesel or biogas/ gasoline. The GATEC technology [7] to overcome the above disadvantages of biogas engines is available on the market. Besides, the universal kit of GATEC allows the conversion of biogas fuel/ liquid fuel for most types of widely-used stationary internal combustion engines (petrol, diesel, a cylinder, multi cylinders, turbocharged, not supercharged,...) and changes a wide range of capacities from a few kW to hundreds of kW. In terms of economical reasons, The GATEC technology has brought many practical benefits for users: - It is not necessary to equip with an expensive engine to run on biogas, which has the same capacity with a backup engine. This will save money and avoid the trouble of switching the power system between the two generators. - It is possible to make use of biogas to generate electricity with unlimited volume. When the biogas source runs out, the generator can be converted to run on gasoline or diesel. - It does not need to waste on biogas as in the GATEC technology. In this way we can avoid the waste of energy and ensure safety and environmental protection. - The engines converted to biogas engines can consume an average of 1 cubic meter of biogas to generate 1kWh of electricity. This will save 0.4 litre of gasoline and reduce the emission of 1 kg of CO2 into the atmosphere. As shown above, the GATEC technology can enable us to convert gasoline or diesel engines Figure 3. A forced ignition engine running on biogas was converted from a gasoline engine Figure 1. GATEC20 Kit Figure 2. GATEC21 Kit
  • 3. Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523 www.ijera.com 518 | P a g e with a wide range of capacities to biogas-powered engines. Owing to the specific features of biogas fuel supply in different combined measures, the economic value of the engine also changes [8]. Biogas forced ignition engines do not need liquid fuel injection (Fig.3). Whereas, dual fuel engines running on biogas converted from diesel engines need a minimum amount of pilot diesel injection for ignition (Fig.4). One of the important requirements for converting a traditional engine to a dual fuel engine -- biogas/ fuel oil -- is that it does not change the components of the engine so that it can re-use liquid fuel when needed. This is related to the treatment of the engine knock when it runs on biogas. In fact, the fuel of biogas is methane which has high anti-knock properties. Therefore, when this fuel is used for biogas engines converted from gasoline engines, we do not need to apply technical treatment on detonation. However, for a dual fuel engine converted from a diesel engine, anti-knock becomes an important issue which should be handled to ensure the normal operation of the engine. The anti-knock properties of the engine depends on the compression ratio and fuel composition. In the previous work, we have studied the effects of biogas composition on continuous biogas combustion in an open space [9]. In the following section, we will present the results of a simulation study of the compression ratio effect on the combustion engine that runs on the biogas containing different CH4 concentrations. II. Simulation of Biogas Combustion in the Engine Combustion Chamber In this study, we assume that combustion occurs in the constant volume combustion cap- shaped chamber with ignition at the top (Fig.5). When the combustion occurs in a very short time compared with the operation of the piston stroke, we can see that the volume combustion chamber is constant. The compression process in the engine is assumed to be the polytropic compression with the average polytropic index of n = 1.3. If the temperatures and pressure at end of the intake process are Ta and Pa, the temperatures and pressure at the end of the compression process are 1n ac TT   and n ac pp  . Table 1. Variable temperatures and pressure at the end of the compression processes in terms of compression ratio (Ta=325K, pa=0,95 Bar) Tc(K) pc(Bar) 9 628 17 10 648 19 11 667 21 12 685 24 13 702 27 14 717 29 15 732 32 16 747 35 17 760 38 18 774 41 Table 1 introduces variations of temperatures and pressure at end of the compression processes versus the compression ratio of the engine when the intake is: Ta=325K, pa=0,95Bar. Simulations are carried out by using the FLUENT Software, the model of "partial premixed" combustion in the 3D chamber space. The standard k- combustion chamber with coefficients: c =0.09, c1=1.44 and c2=1.92. The speed of layer flame is assumed to be 2m/s. The initial mixture is unburnt gas, so the “variable progress" c = 0 (Fig. 6). On changing biogas with different CH4 concentrations, we need to adjust f to have the same ratio of “mixture” . The biogas fuel used is symbolized MxCy, where x is the percentage mol of CH4 and y is the percentage of CO2 mol. Table 2 shows the value of f when equals 1.13 with different biogas fuel components. Figure 5. Cap-Shaped Chamber Used in Simulation Study Figure 4. A dual fuel engine powered by diesel/ biogas -- converted from a diesel engine
  • 4. Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523 www.ijera.com 519 | P a g e The input data of each case include pressures and temperatures at the end of compression processes, the mixture components of f. The thermodynamic parameters of the fuel mixture with the air-fuel biogas with a different set of thermodynamics of the PrePDF table before performing the calculation. Table 2. The value of f when to the biogas fuel with different components Types of fuel M60C40 M70C30 M80C20 f 0,156 0,125 0,100 Combustion is started by assumed sparks with the energy Eig = 0.1 J. After ignition, the flame spreads slowly from the spark center to the farthest point of ignition of the combustion chamber. Computation time step is chosen dt = 0.001s. At each calculation, we determine the temperature, average pressure throughout the combustion chamber, the concentration of CH4 and O2 and the products of combustion as well as the speed of air movement in the combustion chamber. Fig.7 introduces the results of a combustion mixture of air and biogas engine M70C30 with the section apart 2ms axis passing through the combustion chamber. The data include the mass concentration of CH4, CO2, the temperature of the mixture and the movement speed of air in the combustion chamber. This result shows that, after catching fire, the flame quickly spreads to the membrane from the ignition center. The concentration of CH4 in the fire area reduces quickly, while the CO2 generated increases rapidly. The combustion chamber is divided into two sections: The burnt gas section and the unburnt gas section, which are separated from each other by the surface of the flame. The high-temperature zone of Figure 6. Adjustment of average mixture component of f to get an equivalent coefficient of the given mixture  3ms 5ms 7ms 9ms 11ms 13ms 15ms 17ms 19ms CH4 CO2 T(K) V(m/s)
  • 5. Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523 www.ijera.com 520 | P a g e the burnt mixture spreads gradually corresponding to the shift of the flame. As temperatures in the combustion zone rise, combustion products expand and compress unburnt gas mixture toward the front, forming a high-speed zone around the fire flame. III. Results and Discussion Fig.8 and Fig.9 introduce variable average concentrations of CH4 and O2 in the engine combustion chamber corresponding to the engines with compression ratios of 9, 12 and 15. When the engine compression ratios increase, the density of the mixture in the combustion chamber increases accordingly. This makes the speed of combustion (mixture consumption rate) decrease. This represents a change in the slope of the curve of varying concentrations of CH4 and O2 over the time. 0 1 2 3 4 5 6 0 5 10 15 20 25 30 CH4(%) t (ms) =15 =12 =9 Figure 8. The effect of the compression ratio on the concentration of CH4 in the combustion chamber (fuel:M80C20) 0 4 8 12 16 20 24 0 5 10 15 20 25 30 O2(%) t (ms) =15 =12 =9 Figure 9. The effect of the compression ratio on the concentration of O2 in the combustion chamber (fuel:M80C20) 500 1000 1500 2000 2500 3000 0 5 10 15 20 25 30 t (ms) =15 =9 =12 T (K) Figure 10. The effect of the compression ratio on the average temperature of the mixture in the combustion chamber (fuel:M80C20) 0 2 4 6 8 10 12 0 5 10 15 20 25 30 t (ms) P (MPa) =15 =12 =9 Figure 11. The effect of the compression ratio on the average pressure variations in the combustion chamber (fuel: M80C20) The change of combustion speed in accordance with the compression ratio leads to change in the speed of heat release, so the contour curves of temperature variation may also be slightly changed with the engine compression ratios (Fig.10). The effect of the compression ratios on the combustion processes of internal combustion engines is clearly shown in the curve of average 6 2 4 3 5 CH4(%) CO2(%) 12 9,5 7,0 4,5 2,0 T(K) 2700 2200 1700 1200 700 V(m/s) 2,0 1,5 1,0 0,5 0,0 Figure 7. Variations of average concentrations of CH4, CO2, temperature and speed of the mixture in the combustion chamber with =12 and M70C30 fuel
  • 6. Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523 www.ijera.com 521 | P a g e pressure variations in the combustion chamber. Figure11shows that the maximum pressure at the end of combustion processes changes vehemently in accordance with the compression ratio. According to the equation of the ideal gas state PV = NRT, when the volume V and temperature T are unchanged, the pressure relies on the number of moles of gas n. In other words, it depends on the density of the mixture in the combustion chamber before ignition. Since the temperature at the end of the combustion processes corresponds to the engines of same combustion chamber volumes and different compression ratios slightly change, the pressure at the end of combustion processes is in proportion to engine compression ratios. The temperature of the mixture before combustion significantly affects the pressure variations in the engine combustion chamber. Fig.12 compares the variable pressure chamber in the engine compression ratio =9 and =12 in both the initial temperature Tc = 628K and Tc = 685K. Together with the engine compression ratio, the higher initial temperatures are, the lower the pressures at the end of the combustion become. 0 1 2 3 4 5 6 0 5 10 15 20 25 30 CH4(%) t (ms) M80C20 M70C30 M60C40 Figure 13. Influences of biogas on average fuel composition pressure variations of the mixture in the 2 4 6 8 10 12 14 16 18 20 0 5 10 15 20 25 30 CO2(%) t (ms) M80C20 M70C30 M60C40 Figure 14. Influences of biogas on average fuel composition pressure variations of the mixture in the combustion chamber 500 1000 1500 2000 2500 3000 0 5 10 15 20 25 30 t (ms) T (K) M80C20 M70C30 M60C40 Figure 15. Influences of biogas components on the average temperature variations of the mixture in the t (ms) P (MPa) M80C20 M70C30 M60C40 2 4 6 8 10 0 5 10 15 20 25 30 Figure 16. Influences of biogas components on the average fuel composition pressure variations of the mixture in the combustion chamber (compression ratio The same compression ratio engines, biogas fuel components strongly influence the combustion of the engine. Fig.13 and Fig.14 introduces variations of the average concentrations of CH4 and 0 2 4 6 8 10 12 0 5 10 15 20 25 30 t (ms) =12 P (MPa) =9 Ti=685K Ti=628K Ti=685K Ti=628K Figure 12. Influence of initial temperature on the variation of pressure in the combustion chamber with different compression ratios (fuel M80C20)
  • 7. Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523 www.ijera.com 522 | P a g e CO2 in the combustion chamber with fuel types such as M60C40 and M70C30 and M80C20. For rich biogas, CH4 burns almost completely at the end of the combustion processes. When the CO2 components in the fuel increase, CH4 concentration remaining in the mixture also increases. Although the amount of fuel burnt is reduced, the amount of CO2 in the mixture is initially high for poor fuel and CO2 in the mixture significantly increases. This shows that the concentration of CO2 in a strong influence on combustion processes, thus affecting the heat release in the combustion chamber. Fig.15 and Fig.16 introduces the effect of biogas on fuel composition variations in the temperatures and pressures in the engine combustion chamber with a compression ratio of biogas, CO2 in the fuel component hinders the exposure of oxygen and CH4 as bad combustion processes resulting in the amount of unburned CH4 in emissions increased. Consequently, the temperatures and pressures at the end of the combustion processes decline. Fig.17 shows that the average maximum temperatures of the mixture at the end of the combustion processes decrease from 2565K down to 2092K (down by 473K) when the moles of CO2 in biogas increase from 20% to 40%. Corresponding to the increase in the concentration of moles of CO2, the maximum pressure at the end of the combustion mixture decreases from 9.3 MPa to 7.3 MPa (lower 2MPa) (Fig.18). Simulation results show that the concentration of CO2 in the biogas fuel has a strong influence on the combustion engine, especially the speed of heat release. This affects the anti-knock properties of the mixture. Therefore, when converting a conventional engine to use biogas without changing the compression ratio of the engine, we can adjust the concentration of CO2 in the fuel to control the phenomenon of detonation. 2000 2200 2400 2600 20 24 28 32 36 40 Tmax (K) % CO2 (mol/mol) Figure 17. The effect of CO2 component in biogas fuel on temperatures at the end of combustion processes 7 7,5 8 8,5 9 9,5 20 24 28 32 36 40 pmax (MPa) % CO2 (mol/mol) Figure 18. The effect of CO2 component in biogas fuel on pressures at the end of combustion 1. Conclusion The results of this study enable us to draw the following conclusions: 1. When the compression ratio engine powered by biogas ranges from 9 to 15, the end of the combustion pressure increases in proportion to the compression ratio, but the heat release curve at the end of the combustion temperatures in this case is less affected by the compression ratio. 2. With the same engine compression ratio given, the biogas fuel components affect the speed of combustion, temperatures as well as pressure at the end of the combustion process. The concentration of CH4 at end of the combustion processes increases the concentration of CO2 in the fuel. The CO2 components in the biogas fuel are adjustable to control the detonation in the conversion of conventional engines of high compression ratios to the engines fueled with biogas. REFERENCES [1] B.V. Ga, L.M Tien, T.L.B Tram, N.V. Dong, Limitation of Emissions of Greenhouse Gases with the Application of Biogas Technology to Internal Combustion Engines, Proceedings of Scientific Researches at the Eight National Conference on Mechanics, Volume 1, Hanoi, 2009, 383-392. [2] B.V. Ga, T.V. Nam, N.T.T Xuan, Utilization of Biogas Engines in Rural Areas: A Contribution to Climate Change Mitigation, Colloque International RUNSUD 2010, Universite Nice-Sophia Antipolis, France, 2010, 19-31. [3] (http://vietbao.vn/Khoa-hoc/May-phat- dien-sach/45265746/188/) [4] (http://www.sdxsgs.com) [5] http://www.vatgia.com [6] B.V. Ga, T.V. Nam, L.X Thach, A
  • 8. Tran Van Nam et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.516-523 www.ijera.com 523 | P a g e Simulation of the Flow through the Mixture Creation Kit for Forced Ignition Biogas- Powered Engines by Fluent Software, Journal of Science and Technology, Universities of Technology, Issue 80,2011, 134-138. [7] B.V. Ga, Patent for an Invention No 9433, The Variable Speed Adjuster for Biogas Stationary Motors Converted from Diesel Motors, Issued by Intellectual Property Department on July 11th , 2011. [8] B.V. Ga, L.M. Tien, L.X Thach, Comparison of the Effectiveness of Measures to Provide Biogas for Internal Combustion Engines, Journal of Science and Technology, University of Danang, No. 2 (37), 2010, 65-72. [9] B.V. Ga, T.V. Nam, L.M. Tien, An Investigation into the Effect of CO2 on the Combustion Process in Dual Fuel Biogas- Propane Combustion Chamber 3-D, Journal of Science and Technology, Universities of Technology, Issue 81, 2011, 96-102.