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Development of a Reduced n-tetradecane-PAH Mechanism for Application on Two-stroke Marine Diesel Engine Xiuxiu Sun, Xingyu Liang, Gequn Shu, Yuesen Wang, Yajun Wang, and Hanzhengnan Yu Energy Fuels, Just Accepted Manuscript • DOI: 10.1021/acs.energyfuels.6b02708 • Publication Date (Web): 29 Nov 2016 Downloaded from http://pubs.acs.org on December 7, 2016
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An article submitted to Energy & Fuels
Development of a Reduced n-tetradecane-PAH Mechanism for Application on Two-stroke Marine Diesel Engine
Xiuxiu Sun1, Xingyu Liang1*, Gequn Shu1, Yuesen Wang1,Yajun Wang1, , Hanzhengnan Yu1,
1.
State key Laboratory of Engines, Tianjin University, Tianjin 300072, China
*Corresponding Author: Xingyu Liang
State Key Laboratory of Engines, Tianjin University, Tianjin, 300072, China
E-mail:
[email protected] Tele: +86 22 2789 1285
Fax: +86 22 2789 1285
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Development of a Reduced n-tetradecane-PAH Mechanism for Application on Two-stroke Marine Diesel Engine
Xiuxiu Sun1, Xingyu Liang1*, Gequn Shu1, Yuesen Wang1, Yajun Wang1,Hanzhengnan Yu1
1.
State key Laboratory of Engines, Tianjin University, Tianjin 300072, China
Abstract
The rigorous regulation requires marine engine decrease emission. It is difficult to test all
technologies for marine engine using experiment method. The alternative fuel is important for the
simulated model. A semi-reduced kinetic mechanism can be constructed to investigate the
performance of the marine diesel engine, which consists of 341 elementary reactions and 74 species.
Then, the Directed Relation Graph with Error Propagation (DRGEP) and the sensitivity analysis
methods were used to reduce this mechanism. The reduced mechanism consists of 279 elementary
reactions and 62 species. The ignition delay times with the semi-detailed and reduced mechanisms
were validated with the experimental data. At the same time, the results were compared with the 2
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data of published mechanism. Good agreements of ignition delay times were obtained. It was also
found that the trends of in-cylinder temperature, pressure and main species mole fractions were
almost same with results of published mechanism in internal combustion engine model. The main
polycyclic aromatic hydrocarbon (PAH) mole fractions are almost the same with experimental data,
especially the species A4. The 62-species mechanism was validated with the experimental data in a
marine diesel engine model. It can be seen that the in-cylinder pressure was in good agreement with
the experimental data. The NOx had a 2.2 % error compared with the experimental data, which is
the minimum error.
Keywords: Marine diesel engine; Alternative fuel; n-tetradecane; reduced mechanism;
1. Introduction
The two-stroke diesel engine has been widely used for marine transport due to the high thermal
efficiency, wide range of power, good reliability and security. However, the increasing of
environmental concern leads to the more stringent regulation for the emission. The IMO
(International Maritime Organization) Tier III requires that the NOx quantity decrease to 3.4 g/kWh
in the Emission Control Area (ECA), which is reduced by 76 % compared with the 14.4 g/kWh in
TierⅡ1. Some available measures can be researched to reduce the marine emission 2, Exhaust Gas
Recirculation (EGR), Direct Water Injection (DWI), humid air motor (HAM) and so on 3-5. 3
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These technologies are based on the regulate combustion process. As we all know, the
combustion is dominated by the fuel chemical kinetics 6. Thus, a detailed model, which can properly
describes fuel oxidation chemistry, is essential to simulated marine diesel combustion. Panagiotis et
al.
7
used the KIVA-3 code as the modeling platform to study the effects of advanced injection
strategies. It has been demonstrated that, by adding a pilot injection, appropriately timed, fuel
savings of the order of 1.7% can be achieved, without increasing NOX emissions. The tetradecane
can be used as alternative fuel. Michele et al. 8 researched the influence of injector diameter (0.2-
1.2 mm range) on diesel spray combustion using Star-CD. The n-dodecane had been used to
represent the liquid thermo-physical fuel properties of the diesel fuel used in the experiment. E.
Sigurdsson et al. 9 have been studied the scavenge flow and convective heat transfer in large two-
stroke marine diesel engines. The model predictions are in good agreement with the experimentally
determined mass of scavenged gases and scavenging efficiency. The convective contribution to the
in-cylinder heat loss is predicted to be 3.2% of the fuel energy flow to the cylinder. Pang et al. 10
investigate soot formation and oxidation processes under large two-stroke marine diesel engine-like
conditions using integrated CFD (computational fluid dynamics) -chemical kinetics. The n-heptane
was used as alternative fuel in the simulated model. The results show that the averaged nitrogen
monoxide concentration is 7.7 % lower when both convective and soot radiative heat losses are
accounted, but the net soot mass production is less sensitive to soot radiation. Raptotasios et al. 4
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investigate the NOx reduction potential of two-stroke marine diesel engines using EGR. The n-
tetradecane was used as fuels in their simulated model. The results show that the NOx can reduce
to the value of the Tier III requirement, when the EGR rate exceeded 35 % for the 4T50ME-X tested
engine. The commercial diesel is a complex mixture, which consists of hundreds of medium-high-
molecular-weight hydrocarbons. It is not feasible to consider the oxidation chemistry of all
hydrocarbons 12. So the different alkanes can be used as alternative fuel in the simulated marine
diesel engine model.
It is very important to choose a surrogate fuel to ensure the accuracy of a simulated model, due
to the diverse performance of surrogate fuels. Alkanes has been used as surrogate fuel frequently,
such as n-heptane 10, 13, 14, n-tetradecane 7, 8, 11, 15. Researchers can have studied the characteristics of
alkanes. Westbrook et al. 16analyze the detailed chemical kinetic reaction mechanism for combustion
of n-alkane hydrocarbons from n-octane to n-hexadecane. These mechanisms include both high
temperature and low temperature reaction pathways. The paper describes the pyrolysis and
oxidation of alkanes. His-Ping et al. 17 have studied the ignition delay time of n-heptane, n-decane,
n-dodecane, and n-tetradecane at elevated pressures in a shock tube. It indicates that the ignition
delay times for n-alkanes are influenced little by n-alkane chain length for C7 and longer n-alkanes
and for mixtures with common carbon content. The mechanisms of Curran et al. 18 and Westbrook
et al. (Lawrence Livermore National Laboratory (LLNL)) 16 are in agreement with this finding. John 5
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et al. 19 studied the combustion characterization and ignition delay modeling of low and high-cetane
alternative diesel fuels in a marine diesel engine. The modeled chemistry could capture relative
changes in the experimentally observed ignition delay, suggesting that the measured differences in
physical properties, which will affect spray development, do not contribute as significantly to
differences in ignition delay. The experiment and modeling study of the low-temperature oxidation
of large alkanes have been studied by Biet et al. 20. These simulations should help users of kinetic
mechanisms to know if it is necessary to consider heavier model molecules knowing that the number
of included species and reactions will then be considerably increased. Although, the detailed
chemical reaction mechanisms were developed by researchers, the reduced chemical reaction
mechanism is necessary, due to the complex chemical mechanism and the limited capacity of
computer.
Keyvan et al. 21 reduced n-heptane fuel using combined reduction methods. This combination
of methods successfully reduced the comprehensive Curran’s n-heptane mechanism (561 species
and 2539 reactions)
22, 23
to a reduced mechanism with only 118 species and 330 reactions. The
simulation time is decreased from 601 min to 8 min. Wang et al. 12developed chemical kinetics of
diesel surrogate fuel oxidation. The complete kinetic mechanism, which comprised 697 reactions
and 153 species, was reduced to a minor mechanism that included only 141 reactions and 75 species
using the sensitivity and reaction path analyses. The cetane number of n-heptane is close to the value 6
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of diesel fuel, however the n-tetradecane is an optimal choice for the character of diesel fuel. Su et
al.
24
developed a reduced model of n-heptane including 40 species and 62 reactions. The results
showed the well-known two-stage ignition characteristics of n-heptane. The optimized reduced
model generally agrees well with those of the detailed chemical kinetic model
tetradecane, which can be found in reference
23
. For the n-
25
, the simulations show good agreement with the
measurements including the laminar flame speed and extinction strain rate in premixed laminar
flame and counter flow flame, ignition delay and major species. Even though the n-tetradecane is
popular as a marine diesel alternative fuel, the chemical reaction mechanism of n-tetradecane is
insufficient yet.
On the basis of previous studies, this paper constructed a semi-reduced kinetic model to
investigate the performance of marine diesel engine, which comprised 341 elementary reactions and
74 species. Then, the Directed Relation Graph with Error Propagation (DRGEP) and the sensitivity
analysis were used to reduce this model. The reduce model consists of 279 elementary reactions and
62 species. The semi-reduced model and the reduced model are validated against the experimental
data. The three-dimensional-CFD of marine diesel engine was used to validate the reduced model.
This model can provide direction to choosing the marine diesel engine alternative fuel.
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2. Kinetic Mechanism Model 2.1 Model Development The skeletal mechanism was built upon a decoupling methodology 26. The oxidation of alkanes
was divided into two parts: a detailed mechanism for H2/CO/C1, which were detailed studied by
Klippenstein et al. 27 and the oxidation process of small molecule C2-C3, which can be gotten from
the GRI-3.0. The oxidation process of alkanes was analyzed by researchers 14, 16. The oxidation of
n-tetradecane can be built by the reaction path analysis 25, 28. These can be comprised the oxidation
process of n-tetradecane.
The polycyclic aromatic hydrocarbon was used as the precursor of soot. It is important to
predict the soot mass
29.
The reduced PAH mechanism to added into the base n-tetradecane
mechanism, which includes 20 species and 139 reactions 30. The n-tetradecane and PAH mechanism
can connect with the soot model to predict the marine engine soot mass.
The semi-reduced kinetic model investigates the performance of a marine diesel engine, which
comprised 341 elementary reactions and 74 species. Due to the marine engine model has million
cells, the mechanism needs to be simplified to save the calculated time. The DRGEP method can
delete the useless species for the oxidation of n-tetradecane, as studied by the other researchers 21,
31.
So detail information about this method will not be introduced. The CO2 is the important product
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species for the fuel combustion, the related species need to be kept during the simply process. The
produce process of CO2 is shown in Fig.1.
Fig.1 the CO2 reaction paths: the blue lines represent paths of HO2 in reaction, the red lines represent paths of OH in reaction
From the Fig.1, we can see that HCO, C2H2 and CH3O also have directly relationship with the
CO2 produce process. The species CO is the dominant species for the CO2 process. The OH and
HO2 are the important small species for the reactions. The Fig.2 shows the important species for A4
produce process. CH2CO is the important species for the A4, except C2H2. So, the HCO, CO, CH3O,
C2H2 and CH2CO will be retained in the simplified model.
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Fig.2 the A4 reaction paths the blue lines represent paths of HO2 in reaction, the pink lines represent paths of OH in reaction species reaction
74
60
345
CO CO2 H2O Ignition delay time
50
72 330
315
68 66
300
40
Tolerance/ %
Species
70
Reactions number
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30
20
64 285 62 60 0
2
4
6
8
10
12
14
16
18
270 20
10
0 0
2
Simplify the number of times
4
6 8 10 12 14 Simplify the number of times
16
18
(b) Tolerance
(a) Species and reactions
Fig.3 the simplify process for the semi-detailed chemical mechanism: (a) the vary of species and reactions with the simplify number (b) the vary of tolerance with the simplify number
Fig.3 shows the simplify process using DRGEP method. The absolute tolerance set to1e-04,
the relative tolerance set to 10 %. The numbers of species and reactions decrease with increasing
number of simplifies, which can be shown in Fig.3 (a). The tolerances of species and ignition delay
time increases. The percentage of target tolerance is calculated using the following formula: the
absolute different value of master and skeletal / (the value of master * relative tolerance + absolute
tolerance). As the size of the skeletal mechanism decrease, the error value increases. The optimal 10
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skeletal mechanism has the smallest size possible with an error value less than 100 %. 0.5,13
R140 R139 R135 R133 R132 R114 R109 R102 R9 R8 R4 R1 -1.0
0.5,40atm
R140 R139 R135 R133 R132 R109 R102 R9 R8 R4 R3 R1
1100 1000 900
-0.8
-0.6
-0.4
-0.2
0.0
0.2
0.4
0.6
0.8
1.0
1100 1000 900
-1.0
-0.8
-0.6
Temperature sensitivity coefficient
-0.4
-0.2
0.0
0.2
0.4
0.6
0.8
1.0
Temperature sensitivity coefficient
Temperature densitivity coefficient
Temperature densitivity coefficient
(a) Equivalence Ratio = 0.5, Pressure = 13 atm
(b) Equivalence Ratio =1,40 0.5, Pressure = 40 atm
1,14
R140 R139 R135 R133 R132 R109 R107 R102 R11 R9 R8 R4 R1 -1.0
R140 R139 R135 R133 R132 R109 R102 R10 R9 R8 R4 R3 R1
1100 1000 900
-0.8
-0.6
-0.4
-0.2
0.0
0.2
0.4
0.6
0.8
1.0
-1.0
1100 1000 900
-0.8
Temperature sensitivity coefficient
-0.6
-0.4
-0.2
0.0
0.2
0.4
0.6
0.8
Temperature sensitivity Temperature densitivitycoefficient coefficient
Temperature densitivity coefficient
(c) Equivalence Ratio = 1, Pressure = 14 atm
(d) Equivalence Ratio = 1, Pressure = 40 atm
Fig.4 the temperature sensitivity analysis at different conditions
The sensitivity analysis represents the ensemble response to small disturbances by calculating
the ensemble property parameters (species concentration, temperature, and produce rate of species)
variation caused by small changes in the value of a reaction constant. The sensitivity analysis can
make us find some reactions that having influence on the special species or parameters. This method
also be used in some paper, so, it is not necessary to introduce 12, 32. Because the temperature is very
sensitive to ignition of the combustion engine, the important reactions can be kept using this method.
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Fig.4 shows the results of the temperature sensitivity analysis for four different conditions. These
reactions have a significant effect on the system temperature change, especially for the R4, R8, R9
and R135. The corresponding reactions can be found in accessory. These reactions were retained in
reduced chemical mechanism. The final reduced mechanism consists of 279 elementary reactions
and 62 species.
2.2 Marine Diesel Engine Model
The 3-D model is conducted based on the 6S35ME-B9. The structure parameters can be found
in table 1. The engine speed is 142 r/min, and the power is 3575 kW, which can be operated in 100 %
load.
Table. 1 6S35ME-B9 test engine specifications
cylinder number
6
Bore (mm)
350
Stroke (mm)
1550
Displacement (L)
149
connecting rod length (mm)
1550
Speed (r/min)
142
Power (kWh)
3575
The simulated model was performed using the commercial CFD code CONVERGE 2.3. Fig.
5 shows the 3-D geometric structure of the marine engine (6S35ME-B9). The model includes
scavenge box, cylinder and exhaust port. The k-ε RAN model is used for turbulence model. Kelvin 12
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Helmholtz-Rayleigh Taylor (KH-RT) is applied to spray breakup model. The breakup time and size
were set as 1.0 and 0.1respectively. The injected liquid temperature was set as 345 K. The NTC
collision is implemented to simulated fuel collision. The splash model can be used in the wall
interaction. The rebound weber number was set 5.0. The injection duration is 15.3628°CA and the
total injection mass is 0.0125915 Kg, which can be gotten from the experiment. The Extend
Zeldovich NOx model is applied to simulate the NOx product process.
Fig 5.The 3-D geometric structure of the tested marine engine
3. The Semi-detailed Chemical Mechanism Validation 3.1 Comparison to Experimental Data of Ignition Delay Times in Shock Tubes
The ignition delay time is an important parameter for the chemical mechanism, which shows
the accuracy of mechanism. All calculated data for ignition delay time were obtained using closed
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homogeneous constant volume reactor model from the CHEMKIN. The ignition delay time is
defined as the time needed for the mixture to reach a temperature of 400 K from the initial
temperature. Fig.6 shows the comparisons of ignition delay times for new mechanism, experimental
data
17
, detailed n-tetradecane mechanism16 and the mechanism developed by Chang et al.
25
at
different equivalence ratios and pressure. 10000
P=40atm EXP Chang et al Detailed mod 74-species
P=14 atm EXP Chang et al Detailed mod 74-species
Ignition delay time/us
Ignition delay time/us
10000
1000
1000
100
100 0.80
0.85
0.90
0.95
1.00
1.05
1.10
1.15
10 0.80
0.85
0.90
0.95
1000/T (1/K)
1.05
1.10
(b) Φ= 1 P= 40 atm 10000
P=13atm EXP Chang et al Detailed mod 74-species
Ignition delay time/us
10000
1.00
1000/T (1/K)
(a) Φ= 1 P= 14 atm
Ignition delay time/us
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1000
P=40atm EXP Chang et al Detailed mod 74-species
1000
100
100
0.70
0.75
0.80
0.85
0.90
0.95
1.00
1.05
1.10
1.15
10 0.80
0.85
1000/T (1/K)
0.90
0.95
1.00
1.05
1.10
1.15
1000/T (1/K) (d) Φ= 0.5 P= 40 atm
(c) Φ= 0.5 P= 13 atm
Fig. 6 Comparison ignition delay time of new mechanism, experimental data 17, detailed chemical mechanism 16 and published mechanism by Chang et al 25 at different equivalence ratios and pressure
The ignition delay times predicted by the new mechanism are in agreement with the
experimental data. The maximum errors are found in Figs.6 (a) and (c), at low pressure and the
temperature range from 900 K to 1100 K. However, the ignition delay times of new mechanism are
in agreement with of the data that published by Chang et al.. The new mechanism predicts good
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ignition delay times at high pressure, which can be got from Figs. 6 (b) and (d). The reason of
different ignition delay times is that the pre-exponential factors are different for significant reactions.
The ignition delay times of n-tetradecane are acceptable for this new mechanism based on the
comparisons.
3.2 Comparison to Results in Internal Combustion Engine
The semi-detailed reaction mechanism will be used as alternative fuel for internal combustion
engine. It is necessary to predict the accuracy of new mechanism. The in-cylinder pressure and
temperature, the main species mole fractions can be compared with the results from detailed
mechanism, and the developed mechanism by Chang et al.. All computer data have been obtained
by applying the closed internal combustion simulator model from the CHEMKIN. The internal
combustion engine specifications are listed here based on former study12: the bore 115 mm, the
stroke 115 mm, the connect rod length 210 mm, the clearance volume 74.656 cm3 and the engine
speed 1400 r/min.
Fig. 7 displays the comparison of the in-cylinder pressure at four different operating conditions,
which can be shown in Table.2. It can be seen that the trends of in-cylinder pressure obtained by the
74 species mechanism are in acceptable agreement with those of the published mechanism by Chang
et al.. However, the time of break pressure delay 2 °CA for condition 2 (Fig. 7(c)). The maximum
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error was found in Fig.7 (b) by comparing the time of break pressure, which is about 4 °CA delay.
The ignition delay times directly lead to different times of break pressure. Fig.8 displays the
comparison of in-cylinder temperature at four different conditions. The in-cylinder pressure and
temperature have relationship with combustion, the same trends were also found for the in-cylinder
temperature. Therefore, the new mechanism can predict the pressure and temperature for the internal
combustion engine. 180
180 160
Chang et al Detailed mod 74-species
160
Chang et al Detailed mod 74-species
140
140 120
Pressure/atm
Pressure/atm
120 100 80 60
100 80 60
40
40
20
20
0 -40
-30
-20
-10
0
10
20
30
40
0 -40
-30
-20
-10
Crank angle/℃ A
0
10
20
30
40
Crank angle/℃ A
(a) Φ= 1 T= 325 K P= 1 atm
(b) Φ= 1 T= 350 K P= 1 atm
180 160
200
Chang et al Detailed mod 74-species
180
140
160
120
140
Pressure/atm
Pressure/atm
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100 80 60
Chang et al Detailed mod 74-species
120 100 80 60
40
40
20 0 -40
20
-30
-20
-10
0
10
20
30
40
0 -40
-30
Crank angle/℃ A
-20
-10
0
10
20
Crank angle/℃ A (d) Φ= 1.2 T= 350 K P= 1.2 atm
(c) Φ= 1.2 T= 325 K P= 1 atm
Fig.7 Comparison of the in-cylinder pressure at different conditions.
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40
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3500 3000
Chang et al Detailed mod 74-species
Chang et al Detailed mod 74-species
3000
2500
Temperature/K
Temperature/K
2500 2000
1500
2000
1500
1000
1000 500 -40
-30
-20
-10
0
10
20
30
500 -40
40
-30
-20
-10
Crank angle/℃ A
0
10
20
30
40
Crank angle/℃ A
(a) Φ= 1 T= 325 K P= 1 atm
(b) Φ= 1 T= 350 K P= 1 atm 3500
3000
Chang et al Detailed mod 74-species
3000
Chang et al Detailed mod 74-species
2500
Temperature/K
2500
Temperature/K
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2000
1500
1000
1500
1000
500 -40
2000
500 -30
-20
-10
0
10
20
30
40
-40
-30
-20
-10
0
10
Crank angle/℃ A
Crank angle/℃ A
(c) Φ= 1.2 T= 325 K P= 1 atm
(d) Φ= 1.2 T= 350 K P= 1.2 atm
20
30
Fig.8 Comparison of the in-cylinder temperature at different conditions. Table. 2 The combustion engine operating conditions
Equivalence ratio
Intake temperature (K)
Intake pressure (atm)
Condition 1
1
325
1
Condition 2
1
350
1
Condition 3
1.2
325
1
Condition 4
1.2
350
1.2
CO2 and H2O are important species for combustion. OH takes part in many reactions, which
can be found in Fig.1. At the same time, the OH is one kind of H2O2 pyrolysis products. The
comparison of these species can increase the accuracy of mechanism. Fig. 9 shows the comparison
of CO2, H2O, OH and H2O2 at two different operating conditions (conditions 2 and 3). It can be 17
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observed that CO2 and H2O species mole fractions obtained by new mechanism are almost same
with that of others mechanisms at two different conditions (Fig.9 (a) and (c)). The maximum error
is that the crank angle of species increase delay 4 °CA compared with that of detailed mechanism
at the condition 1. The maximum H2O2 mole friction is smaller than that of published mechanism
by Chang et al., but it is higher than that of detailed mechanism, which can be obvious seen in Fig.9
(b) at two conditions. The crank angle of species increase also delay by compared with trend of
detailed mechanism at the condition 2. The OH mole fraction is slightly smaller than that of others
mechanism for Condition 2 (Fig .9(d)). The different value decrease gradually, the mole fraction of
detailed mechanism is 0.0026, and the value of new mechanism is 0.0022. The mole fraction almost
same for three mechanisms at condition 3. Every species has a lot of generation and consumption
paths. The paths and rates of oxidation reactions for n-tetradecane reaction lead to the different of
mechanisms. The new mechanism can well predict the trends of main species mole fractions.
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Page 19 of 30
0.012
H2O Mole Fraction
0.12
Chang et al Detailed mod 74-species
0.010
H2O2 Mole Fraction
0.14
0.10 0.08 0.06 0.04
0.008
0.006
0.004
0.000
0.00 -40
Chang et al Detailed mod 74-species
0.002
0.02
-30
-20
-10
0
10
20
30
40
-40
-30
-20
-10
Crank angle/℃ A
0
10
20
30
40
20
30
40
Crank angle/℃ A (b) H2O2
(a) H2O 0.014 0.12
Chang et al Detailed mod 74-species
0.012
Chang et al Detailed mod 74-species
0.10
OH Mole Fraction
0.010
CO2 Mole Fraction
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0.08 0.06 0.04 0.02
0.006 0.004 0.002
0.00 -40
0.008
0.000 -30
-20
-10
0
10
20
30
40
-40
-30
-20
-10
0
Crank angle/℃ A
Crank angle/℃ A
(c) CO2
(d) OH
Condition 2 : Φ= 1 T= 350 K P= 1 atm
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0.016
0.16 Chang et al Detailed mod 74-species
0.014
0.12
0.012
0.10
0.010
H2O2 Mole Fraction
H2O Mole Fraction
0.14
0.08 0.06 0.04
Chang et al Detailed mod 74-species
0.008 0.006 0.004 0.002
0.02
0.000
0.00 -0.02 -40
-30
-20
-10
0
10
20
30
-0.002 -40
40
-30
-20
Crank angle/℃ A
-10
0
10
20
30
40
20
30
40
Crank angle/℃ A (b) H2O2
(a) H2O 0.10
0.08
Chang et al Detailed mod 74-species
0.010
Chang et al Detailed mod 74-species
OH Mole Fraction
0.008
CO2 Mole Fraction
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
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0.06
0.04
0.02
0.004
0.002
0.00 -40
0.006
0.000 -30
-20
-10
0
10
20
30
40
Crank angle/℃ A
-40
-30
-20
-10
0
10
Crank angle/℃ A
(c) CO2
(d) OH
Condition 3 : Φ= 1.2 T= 325 K P= 1 atm
Fig.9 Comparison of main species mole fractions at different conditions
CO is not only the important intermediate species for the CO2 produce process, but also the
emission pollutant for the internal combustion engine. So, it is necessary to compare CO mole
fraction. Fig. 10 shows the CO mole fractions at conditions 2 and 3. It can be observed that the
trends of CO mole fraction are in agreement with that of others mechanism. The values are also
same when the crank angle is 40 °CA at conditions 2 and 3. The maximum error is that the crank
angle delay 4 °CA by compared with that of detailed mechanism at condition 2. The similarly
conclusion can be got from the Fig.9 at condition 2. The new mechanism can predict the main 20
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species mole fractions for internal combustion engine.
0.10
0.12 Chang et al Detailed mod 74-species
0.10
CO Mole Fraction
0.08
CO Mole Fraction
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0.06
0.04
Chang et al Detailed mod 74-species
0.08
0.06
0.04
0.02
0.02 0.00 -40
0.00 -30
-20
-10
0
10
20
30
40
-40
-30
Crank angle/℃ A
-20
-10
0
10
20
30
Crank angle/℃ A
(a) Φ= 1 T= 350 K P= 1 atm
(b) Φ= 1.2 T= 325 K P= 1 atm
Fig.10 Comparison of CO species mole fraction at different conditions
3.3 Comparison to Results of PAHs in JSR/PFR
The (jet stirred reactor) JSR/PFR (plug flow reactor) model was used to validate the accuracy
of new mechanism for PAHs mole fractions. The temperature was set at 1630 K, and the equivalence
ratio was 2.2. The 74-species mechanism can be validated with the experimental data and the
published mechanism data, which can be got from the tutorials of chemical 33.
Fig .11 shows the comparison of main species mole fractions, H2, C2H2, A1, A2 and A4. It can
be observed that the trends and the quantity of C2H2, H2 and A1 species are almost same for three
different mechanisms. The large errors can be found in comparisons of A2 and A4. However, the
trends of species A2 and A4 are almost same with that of experiment. The mole fractions of new
mechanism main species are close to the experimental data than that of published mechanism for
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A2 and A4. C2H2 and A4 often used as nucleation species in the soot model. The new mechanism
can be used in predicted soot mass. H2
0.1
C2H2
0.01
Mole Fraction
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 22 of 30
1E-3
A1 1E-4
A2 1E-5
1E-6
A4
1E-7 0
4
8
12
16
20
Residence Time /ms
Fig.11 Comparison of PAHs species mole fractions (the solid symbols represent the experiment, the open symbols represent the new mechanism, the lines represent the published mechanism 33)
4. The Reduced Chemical Mechanism Validation
Due to the large structure of marine diesel engine, the new mechanism needs to be reduced.
The calculated time can be saved for using reaction mechanism to deal with combustion. The
reduced mechanism consists of 279 reactions and 62 species. The reduced mechanism will be
validated with the experimental data in 3-D marine diesel engine model.
Fig.12 shows the comparisons of ignition delay times for new and reduced mechanisms at
different pressure and equivalence ratios. It can be observed that the ignition delay times almost
have no difference with the data of new mechanism. Because the absolute tolerance and relative
tolerance of the ignition delay time can be control as 1e-06 and 10 %, respectively.
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10000
1000
Ignition delay time/us
P=13 atm 74-species 62-species P=40 atm 74-species 62-species
10000
Ignition delay time/us
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100
P=13 atm 74-species 62-species P=40 atm 74-species 62-species 1000
100 10 0.75
0.80
0.85
0.90
0.95
1.00
1.05
1.10
1.15
0.80
0.85
0.90
1000/T (1/K)
0.95
1.00
1.05
1.10
1.15
1000/T (1/K) (b) Φ= 1
(a) Φ= 0.5
Fig.12 Comparison ignition delay times of new and reduced mechanisms at different pressure and equivalence ratios
The mechanism is established to simulate the combustion of marine diesel engine fuel. Fig. 13
shows the comparison of in-cylinder pressure of marine diesel engine. The in-cylinder pressure of
reduced mechanism can be compared with the experimental data, result of published mechanism by
Chang et al. and the semi-detailed reaction mechanism. It can be shown that the in-cylinder pressure
of the reduced mechanism is in good agreement with experimental data. The comparisons of key
parameters are shown in Table.3, including the maximum compress pressure and combustion
pressure, the time of break pressure, power and break specific fuel consumption (BSFC). From the
perspective of pressure, the maximum compress pressure and combustion pressure, the time of break
pressure of new and reduced mechanism CFD models are close to the experimental data, which can
also be sown in Fig.13. The errors of new mechanism and reduced mechanism CFD models power
are 0.2 % and 2.4 %, which are acceptable.
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180 150
Pressure/ bar
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EXP Chang et al 74-species 62-species
120 90 60 30 0 200
150
350
300
250
400
450
o
Crank angle/ CA
Fig. 13 Comparison of in-cylinder pressure for marine diesel engine
Table .3 The comparison of important parameters
Exp17
Chang et al.25
74-species
62-species
Maximum Compress pressure (bar)
162.47
163.96
163.93
163.90
Maximum Combustion pressure (bar)
174.83
173.92
172.79
172.05
The time of break pressure (°CA)
365.35
364.4
364.4
364.5
Power output (kW)
3575
3646.02
3583.75
3662.08
Break specific fuel consumption (g/kWh)
180
176.54
179.61
175.793
The emission pollutants have also been compared with experimental data, including NOx and
CO2, which can be observed in the Fig. 14. The quantities of CO2 using mechanism combustion
models are lower than experimental data, since the difference can be existed in simulated and
actually condition. However, the error is 1.5 %, which can be gotten by comparing the reduced
mechanism and the published mechanism by Chang et al CFD models. From the NOx aspect, we
can observe that the error of 62-species mechanism CFD model is 2.2 %, which is closer to the 24
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experimental data. The result of 74-pecies mechanism CFD model is higher than reduced
mechanism CFD model value, the reason is that the differences of temperature and oxygen
concentration distribution.
CO2 / g/kWh
570 555 540 525 510 495 480 EXP
Chang et al
74-species
62-species
EXP
Chang et al
74-species
62-species
14.4
NOx / g/kWh
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14.0 13.6 13.2 12.8 12.4
Fig. 14 Comparison of emission pollutants in marine diesel engine
Due to the limited experiment condition, the soot cannot be validated with the marine diesel
engine. However, the PAH as the precursor of soot, which has directly relationship with the soot.
Fig. 15 displays the comparison of main species mole fraction. It can be observed that the results of
62-species mechanism model are in good agreement with that of the 74-species mechanism model.
In conclusion, the n-tetradecane can be used as alternative fuel of the marine diesel engine. It can
greatly predict the emission pollutants, especially for NOx.
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H2
0.1
C2H2
0.01 1E-3
Mole Fraction
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Page 26 of 30
A1 1E-4 1E-5
A2
1E-6
A4
1E-7 1E-8 0
4
8
12
16
20
Residence Time /ms
Fig.15 Comparison of PAHs species mole fractions for the 74-species and 62-species mechanisms
5. Conclusions
A semi-reduced kinetic model can be constructed to investigate the performance of marine
diesel engine, which comprised 341 elementary reactions and 74 species. Then, the Directed
Relation Graph with Error Propagation (DRGEP) and the sensitivity analysis were used to reduce
semi-reduced kinetic mechanism. The reduced mechanism consists of 279 reactions and 62 species.
The semi-detailed and the reduced mechanisms were validated with experimental data. The results
are listed as following:
1. In shock tube conditions, the ignition delay times with the new and reduced mechanisms
were validated with the experimental data. Good agreements of ignition delay times were
obtained.
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2. The semi-detailed mechanism was tested under internal combustion engine conditions,
which compared with the detailed and published mechanisms. It was found that the trends
of temperature, pressure and main species mole fractions were in good agreement with the
detailed and published mechanisms.
3. The semi-detailed and reduced mechanisms were validated with the experimental data in
marine diesel engine CFD model. It can be seen that the pressure was in good agreement
with the experimental data. The NOx of reduced mechanism CFD model has a 2.2 % error
with experimental data, which is the minimum error compared with that of published
mechanism CFD model.
4. The PAHs were also validated with experimental data for the semi-detailed and reduced
mechanisms. The results of reduced mechanism were closer to the experimental data,
especially for A4.
Acknowledgements
This work was supported by National Natural Science Foundation of China (No. 51376136),
National Sci-Tech Support of China (2015BAG16B01) and Natural Science Foundation of Tianjin
(No. 14JCYBJC21300).
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