**Compressed Natural Gas Direct Injection: Comparison Between Homogeneous and Stratified Combustion**

Shahrir Abdullah, Wan Mohd Faizal Wan Mahmood, Saad Aljamali and Azhari Shamsudeen

Additional information is available at the end of the chapter

http://dx.doi.org/10.5772/67336

#### **Abstract**

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[71] Wang D, Lunsford JH, Rosynek MP. Characterization of a Mo/ZSM-5 catalyst for the conversion of methane to benzene. J Catal [Internet]. 1997;169(1):347-58. Available from:

[72] Cook B, Mousko D, Hoelderich W, Zennaro R. Conversion of methane to aromatics over Mo2C/ZSM-5 catalyst in different reactor types. Appl Catal A Gen. 2009;365(1):34-41. [73] Gao J, Zheng Y, Fitzgerald GB, de Joannis J, Tang Y, Wachs IE, et al. Structure of Mo 2 C x and Mo 4 C x molybdenum carbide nanoparticles and their anchoring sites on ZSM-5 zeolites. J Phys Chem C [Internet]. 2014;118(9):4670-9. Available from: http://pubs.acs.

[74] Baba T, Sawada H. Conversion of methane into higher hydrocarbons in the presence of ethylene over H-ZSM-5 loaded with silver cations. Phys Chem Chem Phys.

[75] Rane N, Kersbulck M, van Santen RA, Hensen EJM. Cracking of n-heptane over Brønsted acid sites and Lewis acid Ga sites in ZSM-5 zeolite. Microporous Mesoporous Mater.

[76] Miao S, Wang Y, Ma D, Zhu Q, Zhou S, Su L, et al. Effect of Ag+ cations on nonoxidative activation of methane to C2-hydrocarbons. J Phys Chem B. 2004;108(46):17866-71. [77] Pidko EA, Hensen EJM, Van Santen RA. Dehydrogenation of light alkanes over isolated

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[79] Li L, Li GD, Yan C, Mu XY, Pan XL, Zou XX, et al. Efficient sunlight-driven dehydrogenative coupling of methane to ethane over a Zn+-modified zeolite. Angew Chem Int Ed.

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Elsevier B.V.; 2011;171(1):52-9. doi:10.1016/j.cattod.2011.04.001

http://www.sciencedirect.com/science/article/pii/S0021951797917127

401-10. doi:10.1016/j.fuel.2014.08.064

articlehtml/2008/ee/b810981h

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org/doi/abs/10.1021/jp4106053

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2011;50(36):8299-303.

Due to abundance of natural gas, the use of natural gas for automotive use, particularly for internal combustion engine (ICE), is more practical and cheaper than their future successors. Even though natural gas is a cleaner fuel than other fossil fuels and has a higher octane number and can lead to higher thermal efficiency, its low carbon number makes it less attractive as compared to gasoline and diesel. Based on its potential, an engine referred to as compressed natural gas direct injection engine (CNGDI) was designed, developed and tested to operate on compressed natural gas (CNG) as monofuel directly and centrally injected into the engine. Computational and experimental works have been performed to investigate the viability of the design. Computational fluid dynamics (CFD) simulations and experimental works with homogenous combustion showed that the results were in good agreement. From experimental works, it is found that combustion characteristics could be improved by using a stratified charge piston configuration with some drawback on performance. In terms of exhaust emissions, stratified configuration causes slight increase in the emission of CO, CO2 and NO*<sup>x</sup>* , which highlight a need for further study on this issue.

**Keywords:** CNGDI, internal combustion, performance, emissions, homogenous mixture, stratified mixture

### **1. Introduction**

In development of any engine, it is desirable to optimise the engine parameter and configuration in order to maximise its performance while keeping the emission within stipulated limits.

© 2017 The Author(s). Licensee InTech. This chapter is distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/3.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Due to abundance of natural gas, the use of natural gas for internal combustion engine (ICE) is more practical and cheaper than their future successors, such as electric and fuel cell cars. Several advantages related to natural gas utilisation in ICEs are its higher thermal efficiency and relatively lower exhaust emissions due to the higher octane level and lower ratio of carbon and hydrogen ratio, respectively [1].

It is understood that configuring conventional ICEs to improve efficiency while reducing exhaust emissions is difficult where strategies to improve engine efficiency will eventually increase harmful emissions, such as carbon monoxide (CO) and nitrogen oxides (NO*<sup>x</sup>* ) [2]. The significant advantage that compressed natural gas (CNG) has in antiknock quality is related to the higher auto-ignition temperature and higher octane number compared to that of gasoline. As the air-fuel ratio for natural gas is 17.23, which requires less fuel required that is less compared to other fuels such as gasoline and diesel, it is possible to obtain the maximum cylinder pressure and rate of heat release at the shorter combustion duration through a right combination of fuel injection, valve and ignition timings while keeping a low level of HC and CO emissions [3].

The use of alternative fuels, including CNG, has attracted popularity along with the importance of emergent alternative fuel technology because the progressively strict regulatory limits on emission levels [4]. Direct injection (DI) in the spark ignition engine considerably raises the engine volumetric efficiency and declines the requirement to use the throttle valve for regulatory purposes [5].

Hence, this chapter presents aspects of the design and development of a compressed natural gas direct injection engine (CNGDI), which can be optimised to yield maximum performance while keeping the emission low. In order to accomplish this study, two types of mixture will be analysed, namely, homogenous and stratified mixtures.

### **2. Development of the CNGDI engine**

In this work, a monofuel CNGDI engine was designed and developed based on a gasoline port injection (PI) engine as shown in **Figure 1**. This new engine design was designed with a specific purpose to enhance the natural gas engine performance as well as to minimise the exhaust emissions. It was also designed using two types of piston crown designs, which are a homogenous piston crown for optimum performance, and stratified piston crown for reduction of exhaust emission.

In general, the design and development process of the main components in an automotive engine are not straightforward. One of the main engine components is its cylinder head, where careful design is required for optimum performance and emission of a vehicle.

The cylinder head is also the platform that is heavily loaded with mechanisms for internal combustion process such as valve train and fuel rail [6]. Hence, the cylinder head of a direct injection engine is highly influenced by the geometry of the injector location at the combustion chamber and has to withstand a very high combustion pressure and temperature. In fact, Compressed Natural Gas Direct Injection: Comparison Between Homogeneous and Stratified Combustion http://dx.doi.org/10.5772/67336 155

**Figure 1.** CNGDI engine head showing the location of spark plug and fuel injector: (a) cylinder head for referral gasoline engine and (b) cylinder head for CNGDI engine.

small changes in the cylinder head geometry can lead to considerable changes in the air-fuel mixture distribution and performance of the engine [7].

The cylinder head could also fail during operation due to thermal fatigue cracking especially in the water jacket cooling area because of narrow path between the valves and the exhaust valve seat [8], as shown in **Figure 2**. For its structural strength, the finite element analysis can be used to obtain the stress and strain profiles of the cylinder structure, which could be analysed further to ensure that the maximum stress does not exceed the allowable yield strength limit [9]. Furthermore, the stress-strain and displacement distributions at various loads and pressure can be simulated. Besides, other researchers also had conducted similar analyses under combustion loading and critical assembly parts in the cylinder head [10]. In this work, the effect of gas pressure during combustion process was examined through the stress and displacement distributions, as shown in **Figure 3**.

Designs of the cylinder head intake and exhaust were guided by a computational fluid dynamics (CFD) simulation in order to ensure the smooth flows of air-fuel mixture and combustion products into and away from the combustion chamber, respectively. With optimal

**Figure 2.** Water jacket design in CNGDI cylinder head.

Due to abundance of natural gas, the use of natural gas for internal combustion engine (ICE) is more practical and cheaper than their future successors, such as electric and fuel cell cars. Several advantages related to natural gas utilisation in ICEs are its higher thermal efficiency and relatively lower exhaust emissions due to the higher octane level and lower ratio of car-

It is understood that configuring conventional ICEs to improve efficiency while reducing exhaust emissions is difficult where strategies to improve engine efficiency will eventually increase harmful emissions, such as carbon monoxide (CO) and nitrogen oxides (NO*<sup>x</sup>*

The significant advantage that compressed natural gas (CNG) has in antiknock quality is related to the higher auto-ignition temperature and higher octane number compared to that of gasoline. As the air-fuel ratio for natural gas is 17.23, which requires less fuel required that is less compared to other fuels such as gasoline and diesel, it is possible to obtain the maximum cylinder pressure and rate of heat release at the shorter combustion duration through a right combination of fuel injection, valve and ignition timings while keeping a low level of

The use of alternative fuels, including CNG, has attracted popularity along with the importance of emergent alternative fuel technology because the progressively strict regulatory limits on emission levels [4]. Direct injection (DI) in the spark ignition engine considerably raises the engine volumetric efficiency and declines the requirement to use the throttle valve for

Hence, this chapter presents aspects of the design and development of a compressed natural gas direct injection engine (CNGDI), which can be optimised to yield maximum performance while keeping the emission low. In order to accomplish this study, two types of mixture will

In this work, a monofuel CNGDI engine was designed and developed based on a gasoline port injection (PI) engine as shown in **Figure 1**. This new engine design was designed with a specific purpose to enhance the natural gas engine performance as well as to minimise the exhaust emissions. It was also designed using two types of piston crown designs, which are a homogenous piston crown for optimum performance, and stratified piston crown for reduc-

In general, the design and development process of the main components in an automotive engine are not straightforward. One of the main engine components is its cylinder head,

The cylinder head is also the platform that is heavily loaded with mechanisms for internal combustion process such as valve train and fuel rail [6]. Hence, the cylinder head of a direct injection engine is highly influenced by the geometry of the injector location at the combustion chamber and has to withstand a very high combustion pressure and temperature. In fact,

where careful design is required for optimum performance and emission of a vehicle.

be analysed, namely, homogenous and stratified mixtures.

**2. Development of the CNGDI engine**

) [2].

bon and hydrogen ratio, respectively [1].

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HC and CO emissions [3].

regulatory purposes [5].

tion of exhaust emission.

**Figure 3.** Finite element analysis of the cylinder head: (a) stress and (b) displacement.

shape design, the inflow and outflow can increase the efficiency of combustion engines and influence the engine performance and exhaust emissions.

During the design of the cylinder head, the intake and exhaust valves were orientated a few degrees from the central axis of the cylinder bore in order to accommodate the spark plug and the fuel injector vertically close to the central axis. The combined valve train and cam system was analysed for kinematic and dynamic responses in order to optimise the angle of valve orientation and some other characteristic parameter for the cam system. By combining the finite element analysis on the stress-strain profile of the cylinder head, the CFD analysis of the cooling system and the dynamic response analysis of the valve train and cam system, the improved design for cylinder head can be produced. Then, prototypes of the CNGDI singlecylinder engine and the CNGDI multi-cylinder head were fabricated by casting as shown in **Figure 4**. These prototypes were installed and single- and multi-cylinder engine test beds for further internal combustion experiments.

**Figure 4.** Cylinder head prototypes: (a) single-cylinder engine and (b) multi-cylinder head.

### **3. Methodology**

shape design, the inflow and outflow can increase the efficiency of combustion engines and

During the design of the cylinder head, the intake and exhaust valves were orientated a few degrees from the central axis of the cylinder bore in order to accommodate the spark plug and the fuel injector vertically close to the central axis. The combined valve train and cam system was analysed for kinematic and dynamic responses in order to optimise the angle of valve orientation and some other characteristic parameter for the cam system. By combining the finite element analysis on the stress-strain profile of the cylinder head, the CFD analysis of the cooling system and the dynamic response analysis of the valve train and cam system, the improved design for cylinder head can be produced. Then, prototypes of the CNGDI singlecylinder engine and the CNGDI multi-cylinder head were fabricated by casting as shown in **Figure 4**. These prototypes were installed and single- and multi-cylinder engine test beds for

influence the engine performance and exhaust emissions.

**Figure 3.** Finite element analysis of the cylinder head: (a) stress and (b) displacement.

**Figure 4.** Cylinder head prototypes: (a) single-cylinder engine and (b) multi-cylinder head.

further internal combustion experiments.

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For the internal combustion study, the analysis started with a CFD simulation of combustion process, which was used to derive the optimum shape of critical engine components that form the combustion chamber as well as the characteristic parameters such as injection and ignition timings. Based on the optimal CFD results, the experiment was performed to further explore the performance and emissions of the newly designed engine.

#### **3.1. Engine specifications and fuel properties**

A four-cylinder spark ignition engine direct injection connected to CNG tanks as the source of fuel was used in this work. The engine specifications are given in **Table 1**.

In addition, **Table 2** lists key properties of CNG for internal combustion as compared to gasoline. Based on the table, it can be deduced that there are several properties in which CNG has advantages, such as a better antiknock quality, that is related to higher auto-ignition temperature and higher octane number, as well as higher air-fuel ratio and heating value. In Malaysia, the typical composition of commercially available CNG is 94.42% methane, 2.29% ethane, 0.03% propane, 0.25% butane, 0.57% carbon dioxide, 0.44% nitrogen and 2% other compounds.


**Table 1.** Engine specifications.


**Table 2.** Combustion-related properties of gasoline and CNG.

#### **3.2. Model for CFD simulation**

In internal combustion engine spark ignition, a complete combustion can produce better engine performance by controlling of engine combustion parameters. Therefore, a numerical study and optimisation of combustion parameters in a CNGDI engine were performed using a computational fluid dynamics (CFD) simulation with single cylinder moving mesh modelling with a source code developed and incorporated as user subroutine to the base CFD code. In developing the moving mesh and boundary algorithms, every event is made as a function of crank angle and represents different configurations of mesh and boundary geometries for an engine cycle [11], as shown in **Figure 5**.

**Figure 5.** Mesh formation using CFD software: (a) surface mesh and (b) volume mesh.

The combustion process was simulated using the Eddy break-up model with the three global reaction schemes. The injection and ignition events were implemented to the engine computational mesh to control the combustion parameters. The CFD analysis used moving mesh simulation, which has been programmed to follow the motion of the intake valves, the exhaust valves and the piston. As the piston moves from bottom dead centre (BDC) to top dead centre (TDC), the height of the cylinder and valve position varies depending on the specific time step used and certain designated events.

During CFD simulation, several engine speeds were simulated in order to investigate the effect of the three engine parameters, namely, timings for the start of injection (SOI), the end of injection (EOI) and the spark ignition (SI), which will affect the engine performance and emission levels of CO, HC and NO. With a correct combined set of timings of SOI, EOI and SI, the indicated power can be optimised while maintaining a sound CO and NO levels. Then, the optimisation work was done by the combined CFD, the Gaussian process and genetic algorithm (GA) methods at every engine speed. The development of single-cylinder model was developed based on the following five stages:


### **3.3. Experimental configuration**

**3.2. Model for CFD simulation**

**Table 2.** Combustion-related properties of gasoline and CNG.

Stoichiometric mixture density

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Heating value of stoichiometric

Spontaneous ignition temperature

(kg/m<sup>3</sup> )

(°C)

mixture (MJ/kg)

an engine cycle [11], as shown in **Figure 5**.

In internal combustion engine spark ignition, a complete combustion can produce better engine performance by controlling of engine combustion parameters. Therefore, a numerical study and optimisation of combustion parameters in a CNGDI engine were performed using a computational fluid dynamics (CFD) simulation with single cylinder moving mesh modelling with a source code developed and incorporated as user subroutine to the base CFD code. In developing the moving mesh and boundary algorithms, every event is made as a function of crank angle and represents different configurations of mesh and boundary geometries for

1.38 1.24

2.83 2.72

480–550 645

**Properties Gasoline CNG** Motor octane number 80–90 120 Molar mass (g/mol) 110 16.04 Carbon weight fraction (mass %) 87 75 Air-fuel ratio 14.7 17.23

Heating value (MJ/kg) 43.6 47.4

Flammability limits (vol. % in air) 1.3–7.1 5–15

**Figure 5.** Mesh formation using CFD software: (a) surface mesh and (b) volume mesh.

Using the CNGDI engine installed on a test bed, experimental investigations can be performed in order to study the performance and exhaust emissions of homogenous mixture and stratified mixture [12].

The engine test bed used in this experiment is depicted in **Figure 6**. Furthermore, investigation of optimum injection timings and the in-cylinder combustion pressure measurement of both homogeneous and stratified combustions were carried out, analysed and compared. The test was performed at engine speeds of 1500–4000 rpm. Some of the results were compared with the CFD analysis mentioned earlier. An engine control system and portable exhaust gas analyser were used for controlling engine operations and recording engine performance and emission data. The software used for the test bench shown above is Kronos 4. Fuel system had the pressure regulator to keep fuel pressure around 20 bar, which was maintained at the fuel entry into the combustion chamber. An air mass flow sensor was installed before the throttle

**Figure 6.** Experimental setup.

valve to record air mass flow, a dynamometer typed FR250 with maximum load of 800 Nm was connected and the torque measured was calibrated using the control levers and weights.

The results were recorded in a steady-state condition and at ambient pressure, temperature and humidity. All readings were recorded in order to estimate the optimal air inlet density. The portable Kane-May exhaust gas analyser was used and calibrated for each test to ensure correct results. The pressure was measured by a pressure sensor of type 6125B-Kistler in the first cylinder to record in-cylinder pressure with specified accuracy. The setting of the electronic control unit (ECU) is modified using the MoTeC software.

The engine was run under the full load wide-open throttle conditions, and the experiments were run using two types of piston configuration, as follows:


**Figure 7.** Homogenous piston configuration.

Compressed Natural Gas Direct Injection: Comparison Between Homogeneous and Stratified Combustion http://dx.doi.org/10.5772/67336 161

**Figure 8.** Stratified piston configuration.

valve to record air mass flow, a dynamometer typed FR250 with maximum load of 800 Nm was connected and the torque measured was calibrated using the control levers and weights. The results were recorded in a steady-state condition and at ambient pressure, temperature and humidity. All readings were recorded in order to estimate the optimal air inlet density. The portable Kane-May exhaust gas analyser was used and calibrated for each test to ensure correct results. The pressure was measured by a pressure sensor of type 6125B-Kistler in the first cylinder to record in-cylinder pressure with specified accuracy. The setting of the elec-

The engine was run under the full load wide-open throttle conditions, and the experiments

1. The homogenous piston configuration is used as shown in **Figure 7** in the first test.

2. The stratified piston configuration is used as shown in **Figure 8** in the second test.

tronic control unit (ECU) is modified using the MoTeC software.

were run using two types of piston configuration, as follows:

**Figure 7.** Homogenous piston configuration.

**Figure 6.** Experimental setup.

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### **4. Results and discussion**

This section displays some results from the CFD simulation, which has been used as the basis for design optimisation of the cylinder head before it was fabricated. Then, the cylinder head together with the valve train, the cam system and the fuel rail was installed on the current based engine on the test bed before it was tested for various engine speeds.

#### **4.1. CFD simulation of combustion process**

The CFD simulation results of the same work have been presented and discussed in Refs. [1, 2, 11]. The simulation was performed on a combustion chamber of the engine cylinder specified in **Table 1** for a stoichiometric air-fuel mixture. The simulation results for 3000 rpm were given in **Figure 9** for different crank angles, where the fuel is considered as 100% methane [13].

The simulation depicts the progression of air-methane profile in a shrinking cavity of combustion chamber at pre-ignition stage during the compression stroke. The post-ignition stage

**Figure 9.** Simulated air-fuel mixture contour during compression stroke.

resulted in rapid increase of in-cylinder pressure, which produced torque and power output as depicted in **Figure 10** in the graph of pressure with the engine displacement. The CFD results were compared with the experimental results as explained in the next section.

#### **4.2. Comparison between homogenous and stratified combustions**

The next subsections show the results obtained from experiment using both types of piston configuration, where the results are plotted in the same graphs. The results for power and torque were also compared with the CFD results for homogenous piston configuration. Together with the CFD simulation, the experiment was limited to a speed of 4000 rpm.

#### *4.2.1. Power and torque*

**Figure 11** shows the brake power and brake torque with the engine speed. The results were recorded from 1500 to 4000 rpm for both homogenous and stratified combustions. From the results, higher power and torque were obtained in stratified combustion with improvement observed at low speeds between 1500 and 2500 rpm. The maximum power recorded with stratified combustion was 54.75 kW at 4000 rpm, which is 3% higher than that of homogenous combustion. This finding is consistent with the study carried out by Sendyka and Cygnar [14] on gasoline direct injection engine.

In both combustion modes, the torque curves exhibit dual-peak profile, which is the typical characteristic of a double overhead cam (DOHC) engine with unmodified cam profile as used in the present investigation. Higher power obtained is the results of higher pressure and higher heat release rate. In addition, a late injection timing with high pressure and suitable combustion duration increases the engine performance, and good propagation flame is obtained [15]. Furthermore, high heat released with the lean mixture produced high indicated power.

**Figure 10.** Simulated pressure and engine displacement in a *p*-*v* diagram.

Compressed Natural Gas Direct Injection: Comparison Between Homogeneous and Stratified Combustion http://dx.doi.org/10.5772/67336 163

**Figure 11.** Power and torque of homogeneous and stratified combustions at different engine speeds.

As comparison, in another study by Kalam and Masjuki [16], the average brake power over the test cycle obtained was 47.39, 36.90 and 45.37 kW the gasoline port injection, CNG bi-fuel and CNG direct injection engines, respectively, using homogenous piston. The main factor affecting the brake torque is the lack of chemical energy conversion to mechanical energy, which is strongly related to volumetric efficiency, fuel mixing, net heat release rate and cylinder pressure [12].

#### *4.2.2. Brake mean effective pressure*

resulted in rapid increase of in-cylinder pressure, which produced torque and power output as depicted in **Figure 10** in the graph of pressure with the engine displacement. The CFD

The next subsections show the results obtained from experiment using both types of piston configuration, where the results are plotted in the same graphs. The results for power and torque were also compared with the CFD results for homogenous piston configuration. Together with the CFD simulation, the experiment was limited to a speed of 4000 rpm.

**Figure 11** shows the brake power and brake torque with the engine speed. The results were recorded from 1500 to 4000 rpm for both homogenous and stratified combustions. From the results, higher power and torque were obtained in stratified combustion with improvement observed at low speeds between 1500 and 2500 rpm. The maximum power recorded with stratified combustion was 54.75 kW at 4000 rpm, which is 3% higher than that of homogenous combustion. This finding is consistent with the study carried out by Sendyka and Cygnar [14]

In both combustion modes, the torque curves exhibit dual-peak profile, which is the typical characteristic of a double overhead cam (DOHC) engine with unmodified cam profile as used in the present investigation. Higher power obtained is the results of higher pressure and higher heat release rate. In addition, a late injection timing with high pressure and suitable combustion duration increases the engine performance, and good propagation flame is obtained [15]. Furthermore, high heat released with the lean mixture produced high indicated

results were compared with the experimental results as explained in the next section.

**4.2. Comparison between homogenous and stratified combustions**

*4.2.1. Power and torque*

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power.

on gasoline direct injection engine.

**Figure 10.** Simulated pressure and engine displacement in a *p*-*v* diagram.

Generally, the brake mean effective pressure (BMEP) is affected by heat release rate, good mixture and sufficient combustion time. **Figure 12** depicts the BMEP with the engine speeds. The results show that BMEP increases with the engine speed and higher BMEP was obtained with the stratified combustion, especially at several low speeds as shown. The maximum value recorded for the stratified combustion is 10.3 bar at 4000 rpm.

**Figure 12.** BMEP of homogeneous and stratified combustions at different engine speeds.

#### *4.2.3. Brake-specific fuel consumption*

**Figure 13** shows brake-specific fuel consumption (BSFC) versus engine speed. The results show a lower BSFC obtained with stratified combustion in comparison with homogenous combustion for all engine speeds.

The main reason is that stratified combustion has lower fuel consumption where the fuel surrounding the spark plug is richer. This leads to ignition and initiation of combustion at this area that produces sufficient energy to propagate the flame and sustain the combustion smoothly through the leaner layers of air-fuel mixture, resulting in a more efficient combustion. This is consistent with the experiment by Baeta et al. on their torch ignition engine [17].

### *4.2.4. Lambda and volumetric efficiency*

**Figure 14** depicts the lambda and volumetric efficiency versus engine speed. The recorded lambda was more than one (λ ≥ 1) accounting for a lean combustion which in turn decreases the fuel consumption. The lambda is more at the stratified combustion than the homogenous combustion. Consequently, for the stratified combustion, the volumetric efficiency is higher. From these results, there were two critical points at engine speeds, i.e. at 2000 and 3000 rpm as shown by the volumetric efficiency values in the graph.

#### *4.2.5. Combustion pressure*

Based on the same experimental data, the in-cylinder pressure generated from the combustion process is plotted against engine displacement or piston swept volume. **Figure 15** shows the cylinder pressure of the homogenous combustion versus cylinder volume and crank angle. The maximum recorded pressure was 186 bar at 4000 rpm just after the top dead centre.

From the *p*-*v* diagram, the indicated work and heat release can be calculated. Other factors affecting the *p*-*v* cycles include the air-fuel ratio and ignition timing. At 2500 rpm, the BMEP

**Figure 13.** BSFC of homogeneous and stratified combustions at different engine speeds.

Compressed Natural Gas Direct Injection: Comparison Between Homogeneous and Stratified Combustion http://dx.doi.org/10.5772/67336 165

**Figure 14.** Lambda and volumetric efficiency of homogeneous and stratified combustions at different engine speeds.

and torque produced higher than that of 3000 rpm, which explains the double-peak phenomenon for the DOHC engine with fixed cam profiles. The work then increased at 3500 rpm and eventually at 4000 rpm. The combustion pressure influences the brake mean effective pressure as shown, which in turn affects the power and torque produced in **Figure 11**. All the peak pressure occurred just after TDC.

As comparison, **Figure 16** shows the cylinder pressure of a stratified combustion versus engine displacement and crank angle. A high combustion pressure of 145 bar was observed at 4000 rpm at 7° after TDC. However, all the peak values of pressure are about 20% lower than the ones produced by the homogenous combustion.

Similarly, the indicated work at 3000 rpm is lower than at 2500 rpm and subsequently at 3500 and 4000 rpm. Consequently, the BMEP is more at 2500 rpm than at 3000 rpm with values of 9.69 and 9.08 bar, respectively, as shown in the figure. The most likely reasons that lead to this kind of pressure degree variation are the same with that for the homogenous combustion.

**Figure 15.** Cylinder pressure in homogenous combustion.

*4.2.3. Brake-specific fuel consumption*

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combustion for all engine speeds.

*4.2.4. Lambda and volumetric efficiency*

*4.2.5. Combustion pressure*

as shown by the volumetric efficiency values in the graph.

**Figure 13.** BSFC of homogeneous and stratified combustions at different engine speeds.

**Figure 13** shows brake-specific fuel consumption (BSFC) versus engine speed. The results show a lower BSFC obtained with stratified combustion in comparison with homogenous

The main reason is that stratified combustion has lower fuel consumption where the fuel surrounding the spark plug is richer. This leads to ignition and initiation of combustion at this area that produces sufficient energy to propagate the flame and sustain the combustion smoothly through the leaner layers of air-fuel mixture, resulting in a more efficient combustion. This is consistent with the experiment by Baeta et al. on their torch ignition engine [17].

**Figure 14** depicts the lambda and volumetric efficiency versus engine speed. The recorded lambda was more than one (λ ≥ 1) accounting for a lean combustion which in turn decreases the fuel consumption. The lambda is more at the stratified combustion than the homogenous combustion. Consequently, for the stratified combustion, the volumetric efficiency is higher. From these results, there were two critical points at engine speeds, i.e. at 2000 and 3000 rpm

Based on the same experimental data, the in-cylinder pressure generated from the combustion process is plotted against engine displacement or piston swept volume. **Figure 15** shows the cylinder pressure of the homogenous combustion versus cylinder volume and crank angle. The maximum recorded pressure was 186 bar at 4000 rpm just after the top dead centre. From the *p*-*v* diagram, the indicated work and heat release can be calculated. Other factors affecting the *p*-*v* cycles include the air-fuel ratio and ignition timing. At 2500 rpm, the BMEP

**Figure 16.** Cylinder pressure in stratified combustion.

#### *4.2.6. Emissions*

For the final sets of result, various emissions are plotted versus the engine speeds as shown in **Figure 17**. The results demonstrate a high CO at stratified combustion at a low engine speed, but CO decreases at high speed compared to homogenous combustion. Meanwhile, CO<sup>2</sup> is also lower for stratified combustion in high speed, whereas the value of CO<sup>2</sup> increases with the engine speed increase for both combustion modes.

**Figure 17.** Emissions for homogeneous and stratified combustion at different engine speeds.

Moreover, NO is recorded lower with stratified combustion mode only at 2000 and 4000 rpm, while slightly higher than homogeneous combustion at other speeds. However, the study of Baeta et al. [17], which employed the side injection strategy as opposed to the central injection strategy used in this work, reported reductions of NO*<sup>x</sup>* , CO and CO2 with stratified combustion in gasoline engine. This highlights the need for further studies, which are underway to look into the emission issue for the central injection strategy, particularly on NO.

### **5. Conclusions**

A CNGDI engine that operates on monofuel, namely, natural gas, has been designed, developed and tested. Computational and experimental works have been performed to investigate the viability of the new design. Baseline computational and experimental works with homogenous combustion showed that the results were comparable. From computational work, detailed CNGDI homogeneous combustion characteristics were obtained via CFD simulation and studied. Combustion characteristics could be improved by using a stratified charge piston configuration. Experimental work on stratified piston configuration has shown that it improves the engine torque and power especially at low speeds as compared to the homogeneous piston. In terms of exhaust emissions, stratified CNGDI design causes slight increase in the emission of CO, CO2 and NO*<sup>x</sup>* . This highlights the need for further studies, which are underway to look into this emission issue.

### **Author details**

is

increases with

*4.2.6. Emissions*

For the final sets of result, various emissions are plotted versus the engine speeds as shown in **Figure 17**. The results demonstrate a high CO at stratified combustion at a low engine speed, but CO decreases at high speed compared to homogenous combustion. Meanwhile, CO<sup>2</sup>

also lower for stratified combustion in high speed, whereas the value of CO<sup>2</sup>

**Figure 17.** Emissions for homogeneous and stratified combustion at different engine speeds.

the engine speed increase for both combustion modes.

**Figure 16.** Cylinder pressure in stratified combustion.

166 Advances in Natural Gas Emerging Technologies

Shahrir Abdullah1,2\*, Wan Mohd Faizal Wan Mahmood1,2, Saad Aljamali1 and Azhari Shamsudeen2

\*Address all correspondence to: shahrir@ukm.edu.my

1 Department of Mechanical and Materials Engineering, Faculty of Engineering and Built Environment, Universiti Kebangsaan Malaysia, UKM Bangi, Selangor, Malaysia

2 Centre for Automotive Research, Faculty of Engineering and Built Environment, Universiti Kebangsaan Malaysia, UKM Bangi, Selangor, Malaysia

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**Advances in Natural Gas Alternative**
