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Abstract

Experiments and simulations were conducted to study effects of charge density, temperature, and oxygen concentration on the mixing-controlled engine combustion pathway in heavy-duty diesel engines. Due to the inherent heterogeneity of diesel combustion in high-load operations, the rich and lean mixtures are simultaneous present. The mass and accompanying heat transfers were found to be decisive in determining the combustion path. The chemical transformation from a richer mixture to a leaner mixture is primarily driven by charge density, which activates the combustion process, and reduction in oxygen concentration, which stagnates the mass and heat transfer and chemical transformation, reduces the reactivity of the mixtures. The difference in mass and heat transfer processes causes differences in the mass fractions of mixtures with different equivalence ratio intervals. The different mixtures produce different mass fractions of intermediate combustion products (carbon dioxide, CO), different heat releases, and different mass temperature distributions. It is found that the accumulated CO correlates well with the gross indicated thermal efficiency and soot emission; the mass averaged temperature and the high temperature abidance scale (HTAS) correlate well with NO_x emissions. A significant optimization of the overall engine performance could be achieved by simultaneously minimizing the HTAS and accumulated CO.

Keywords

Heavy-duty diesel engine Miller Cycle mixing-controlled combustion emissions efficiency mass-averaged temperature CO accumulation

Introduction

The application of low-temperature combustion (LTC) is a suitable solution for the simultaneous reduction of nitrogen oxides (NO_x) and particulate matter (PM) emissions.^1–4 The LTC regime requires a very high exhaust gas recirculation (EGR) rate (>60%) to aggressively prolong the ignition delay. Barriers to LTC in high-load operations are associated with the supercharger system, heat loss at high EGR, and other engineering complications.^5,6

A compound combustion system without EGR was developed, which consists of premixed charge compression ignition (PCCI) combustion at low loads through early and modulated multi-pulse injections.⁷ The PCCI combustion was further combined with lean diffusion combustion methodology, using a high-mixing-rate combustion chamber and multi-pulse fuel injection technique.^8,9 Subsequently, a hybrid combustion control strategy consisting of mixing enhancements and inhibition of chemical reactions by using a high EGR rate was proposed for engines operating at low and medium loads.¹⁰ A high-density low-temperature diesel combustion (HD-LTDC) engine system was developed,¹¹ achieving high efficiency and low emissions under high and full load operations. It relied on a high charge density by increasing the boost pressure (P_b) up to 0.45 MPa, moderately low oxygen concentrations (φ_O2) using lower rate of EGR, and lowering the charge temperature at TDC (T_tdc) through the development of a variable Miller Cycle mechanism retarding the intake valve closing timing (IVCT). The combustion control strategy resulted in very low engine emissions and improved efficiency. However, the combustion mechanism of the HD-LTDC has not been thoroughly investigated.

Genzale et al.¹² studied the significance of enhancing the mixing rate via computational investigation on the effects of spray targeting, bowl geometry, and swirl ratio for low-temperature combustion in a heavy-duty diesel engine. Wakisaka et al.¹³ studied the effects of increasing boost pressure, high EGR rate, and high injection pressure on exhaust emissions from a high-speed direct-injection diesel engine. The mechanisms were then investigated under a high-load condition, and we concluded that increasing the charging efficiency, combined with a high injection pressure and high EGR rate, was effective for reducing NO_x and soot simultaneously. Variable valve timing (VVT) is an effective strategy to adjust the effective compression ratio, which is beneficial for controlling the combustion process of advanced combustion modes. Recently, Xu et al.¹⁴ optimized the PCCI combustion coupled with the VVT strategy at a wide load range, and it was found that the performance of fuel consumption, NO_x and soot emissions can be improved simultaneously at different loads with the employment of the late IVCT strategy. Xu et al.¹⁵ also evaluated the VVT strategy in a heavy-duty diesel engine with reactivity controlled compression ignition (RCCI) combustion under a wide load range.

The hybrid combustion control principle for low and medium engine loads¹⁰ has been well understood using a combination of mixing rate and reaction rate. A high gross indicated thermal efficiency (ITE_g) of 53% and near-zero emissions over a wide range of diesel engine operations, up to a gross indicated mean effective pressure (IMEP) of 1.1 MPa, are realized. However, the primary challenge is to achieve high efficiency and low emissions in high and full load operations of a heavy-duty diesel engine. This study explores factors that affect the combustion when brake mean effective pressure (BMEP) exceeds 2 MPa. Accordingly, the effects of the combustion boundaries on overall engine performance have been investigated experimentally and numerically.¹⁶ However, the influencing mechanism of the boundaries on the combustion path has not been clearly explored. Therefore, a detailed correlation study of the boundaries, including charge density at TDC (ρ_tdc), T_tdc, and φ_O2, with combustion parameters was conducted. The correlations of the significant combustion boundaries in both burned and unburned mixtures, charge mass-averaged temperatures, and mass of the intermediate combustion product CO have been studied revealing a deeper understanding of the combustion process at very high engine loads.

Experimental set-up and CFD model

Experimental set-up

The experimental set-up was presented in Figure 1. The test engine was a single-cylinder engine modified from a six-cylinder heavy-duty diesel engine. The sixth cylinder of the diesel engine was used as the test cylinder, while the other five cylinders only dragged the sixth one. Since the combustion process of the other five cylinders was not controlled, they were equipped with common exhaust systems, turbocharged intercooled intake systems and mechanical fuel supply systems. The test system was composed of the electrically controlled high pressure common-rail fuel supply system, simulated pressurized intake system, VVT system, EGR system, multi-function combustion parameter acquisition and analysis system and exhaust gas emission test system.

Figure 1.

Schematic diagram of the experimental equipment.

The second-generation electrically controlled high-pressure common-rail fuel supply system Bosch was used to supply the sixth cylinder in the test. The EGR rate could be met by cooperatively adjusting the intake regulating valve, the exhaust back pressure regulating valve and the EGR valve.

A single-cylinder VVT system was a kind of variable valve system which could be continuously and flexibly adjusted to realize the Miller Cycle. By retarding IVCT, the effective compression ratio was reduced, the compression pressure and temperature at TDC were both decreased, and the exceeding limit of in-cylinder pressure caused by high pressure could be effectively avoided. And the expansion ratio remained unchanged to realize the Miller Cycle, which ensured the high thermal efficiency. The IVCT actuation system combined with the high pressurization and EGR systems could realize reasonable control of the state in the cylinder and was one of the indispensable means to realize the high density-low temperature combustion process. The adjustment range of variable valve system was determined by the engine piston, the original valve motion law and the valve motion law attached to the variable valve system. The real-time position of the engine piston and valve must be analyzed to know whether there was interference between piston motion and valve motion. Considering a certain safety factor, it was absolutely possible to avoid the collision between the piston and the valve by limiting the additional valve action range of 50°CA between the inlet cam vertex and the TDC. Besides, the later the IVCT was closed, the lower the effective compression ratio was, and the lower the temperature in the compression stage was. Under overall consideration, the IVCT was fixed at −60° CA ATDC for cases 2–8 in Table 2 to fully utilize the Miller Cycle.

A multi-function combustion parameter acquisition and analysis software based on single-cylinder pressure acquisition was developed in LabView language and it had a real-time man-machine interface at each working point of a single cylinder. The purpose of this interface was to monitor and collect the power diagram, the mean indicated pressure, the peak in-cylinder pressure, the maximum pressure rise rate, the start point of combustion, the instantaneous heat release rate in real time, and the key parameters of the combustion process after adopting the VVT system.

The engine emissions, including NO_x, CO₂, CO, UHC, and O₂, were measured with a Horiba 7100 gas analyzer. An AVL 415S smoke meter was used to measure soot emissions, whose presentation of measurement results was filter smoke number (FSN), resolution ratio was 0.001 FSN, lower limit of detection was 0.002 FSN, measuring range was 0–10.

Table 1 provides the specifications and operating parameters of the engine. Table 2 presents the engine experimental conditions and overall performances for various cases, in which the ρ_tdc and T_tdc are calculated by the ideal gas equation of state and adiabatic equation. According to experimental result, the in-cylinder temperature at IVCT with retarded IVCT is already much higher than the intake temperature, which can also be estimated by GT-POWER.

Table 1.

Engine specifications and operating parameters.

Bore × stroke (mm)	126 × 155
Swirl ratio	1.2
Maximum cylinderpressure (MPa)	16.5
Engine speed (rpm)	1600
Injection system	Common rail
Injection timing (°CA ATDC)	3.5
Injection pressure (MPa)	160
Nozzle	8 holes
	Included spray angle: 143°
	Hole diameter: 0.217 mm
Combustion chamber	BUMP combustion bowl¹⁷
Valve events	With intake valve closingtiming control
Intake temperature (°C)	46~51

Table 2.

Experimental control parameters and resulting performance.

Case	IVCT/°CAATDC	ε	P_b/MPa	φ_O2/%	EGR/%	Φ_m	ρ_tdc/kg/m³	T_tdc/K	m_f/mg	NO_x/g/KWh	Soot/g/kWh	CO/g/kWh	UHC/g/kWh	IMEP/MPa	Δη_t/%
1	−146	16.1	0.30	21	0	0.43	46.9	981	192	10.7	0.013	0.38	0.03	1.85	0
2	−60	5.96	0.265	21	0	0.59	31.4	903	192	8.47	0.019	0.56	0.03	1.79	−3
3	−60	5.96	0.41	21	0	0.44	48.0	899	192	7.72	0.006	0.62	0.22	1.95	+6
4	−60	5.96	0.46	21	0	0.38	60.3	906	192	8.11	0.003	0.69	0.29	2.03	+10
5	−60	5.96	0.265	19.0	12.6	0.65	32.5	891	192	3.81	0.038	0.98	0.04	1.75	−5
6	−60	5.96	0.41	18.6	19.6	0.51	48.0	892	192	1.21	0.011	1.55	0.32	1.90	+3
7	−60	5.96	0.46	18.4	23.0	0.46	60.4	892	192	1.19	0.013	1.48	0.39	1.89	+2
8	−60	5.96	0.41	17.2	26.6	0.57	51.0	888	214	0.75	0.092	4.58	0.24	2.09	+1

Numerical simulation models

The extended coherent flame combustion model in three zones (ECFM3Z)¹⁸ developed by the Groupement Scientifique Moteur (GSM) consortium was employed. The model was featured an additional level of refinement by simulation of the subgrid turbulent mixing between air, EGR gas, and fuel. Two states of mixture zones, namely, the unburned mixture zones and the burned mixture zones, were considered during combustion. The ERC soot model,¹⁹ kinetic oxidation of CO, and extended Zeldovich mechanism of NO_x²⁰ were introduced. Simulations were performed with STAR-CD, developed by the CD-Adapco Group.²¹ In the above mentioned computer program, the Reitz–Diwakar model was used to simulate high-pressure diesel spray atomization and secondary breakup,²² whereas the Bai model, developed by Bai and Gosman,²³ was used to simulate droplet-wall interactions. The RNG κ–ε turbulence model, developed by Han and Reitz,²⁴ was used to model turbulent mixing, and the double-delay auto-ignition model, developed by Colin et al.,²⁵ was used to model diesel auto-ignition. The double-delay auto-ignition model uses pre-computed values representing the results of complex calculations for the auto-ignition of n-heptane and provides values for both delays as a function of pressure, temperature, equivalence ratio, and EGR. As shown in Figure 2, the calculated values of in-cylinder pressure (P_cyl), rate of heat release (ROHR), the NO_x, soot, and CO emissions are in reasonable agreement with the measured values.

Figure 2.

Comparison of experimental and calculated results for various cases in Table 2: (a) P_cyl and ROHR and (b) NO_x, soot and CO emissions.

Results and discussion

Experimental results and discussion

As shown in Table 2, case 1, the baseline case for comparison of thermal efficiency and emissions, is with P_b of 0.3 MPa, EGR of zero, and IVCT of −146° crank angle (CA) after top dead center (ATDC) with corresponding effective compression ratio (ε) of 16.1. For cases 2–8, the IVCTs are all retarded to −60° CA ATDC by Miller Cycle mechanism with corresponding ε of 5.96. For cases 3 and 4, P_b is increased from 0.265 MPa (the value obtained in case 2) to 0.41 MPa and 0.46 MPa, respectively. Therefore, the ρ_tdc increases from 31.4 kg/m³ (the value obtained in case 2) to 48 kg/m³ and 60.3 kg/m³ for cases 3 and 4, respectively. The in-cylinder peak combustion pressures are consistently below 16.5 MPa because of the retarded IVCT. Accordingly, the in-cylinder overall equivalence ratio (Φ_m) decreases from 0.59 to 0.44 and 0.38 with a constant φ_O2 of 21%. For cases 5, 6, and 7, the P_b, ρ_tdc, and IVCT are set almost identical to those in cases 2, 3, and 4, respectively; however, the φ_O2 decreases from 21% to 19%, 18.6%, and 18.4%, respectively, using EGR. Case 8, with an EGR of 26.6% and φ_O2 of 17.2%, represents an over-high EGR scenario.

Comparing case 3 with the original case 1, the T_tdc is reduced by up to 82 K due to the retardation of IVCT from −146° to −60° CA ATDC. A reduction in NO_x and soot emissions of 28% and 54%, respectively, and a 6% increase in ITE_g are shown in Table 2. The significant effect of ρ_tdc is observed by comparing cases 2, 3, and 4. Soot reduction by a factor of 2–5 and a slight NO_x reduction are obtained as ρ_tdc increases from 31.4 to 60.3 kg/m³. For cases 5, 6, 7, and 8, the combined effects of ρ_tdc and φ_O2 demonstrate that the NO_x emissions are significantly reduced while the exhaust emissions maintain acceptable levels until φ_O2 decreases to 18.4%.

Simulation results and discussion

Combustion path model

Simulations demonstrate that the combustion field is heterogeneous in equivalence ratio and temperature, including ignition and non-ignition charge zones, which are denoted as the burned zone mass (M^b) and unburned zone mass (M^u), respectively. The combustion path is depicted by the overall behavior of mixing and chemical reactions of the charge zones in the combustion processes. The M^b and M^u charge zones are further categorized into three subzones according to the local fuel/oxygen equivalence ratio Φ: the lean zone 0 < Φ ≤ 1, rich zone 1 < Φ < 2, and over-rich zone Φ ≥ 2. Driven by the energy of the gas entrainment motion, the fuel mass in a richer zone is transferred to a leaner zone in both burned and unburned. The occurrence of ignition in a local unburned zone indicates immediate transfer from M^u to M^b. However, the combustion path is determined by the Φ as indicated in Figure 3. Only the fuel mass in the lean zone can be completely oxidized and form CO₂ and H₂O, releasing chemical heat, when the zone temperature is higher than 1400 K. This is shown on a Φ–T map of CO distribution created by Huang and Su.²⁶ The study proved that the formation of CO and other intermediate combustion products is caused by the existence of rich and over-rich mixtures in M^b. The Φ–T map of CO showed the distribution of CO as a function of the Φ and combustion temperature. For rich zones, even at very high temperatures of combustion, CO and other intermediate combustion products are produced first and eventually transformed into the complete combustion products of CO₂ and H₂O when they react with oxidizers (O, O₂, and OH). The rate of production is controlled by the mixing rate of intermediate products with oxidizers as well as the mixing temperature, which promotes NO formation if the mixing rate is high. The over-rich zone is richer than the equivalence ratio threshold of soot formation (e.g. Φ ≥ 2). The soot particles are also an intermediate product. The final soot emission is determined by the net difference of the formation process and oxidation process.¹⁹

Figure 3.

Schematic depiction of combustion paths.

Effects of ρ_tdc and φ_O2 on the combustion paths

Figure 4 shows the change in the mass fractions of equivalence ratio zones in M^u and M^b for cases 2, 3, and 4. The cases have an equal φ_O2 of 21% and a near-equal T_tdc of 903 K, 899 K, and 906 K, respectively, whereas, they have varying ρ_tdc of 31.4 kg/m³, 48 kg/m³, and 60.3 kg/m³, respectively. The mass fractions of various equivalence ratio zones in M^u for the three cases are quantitatively quite similar at the beginning of fuel injection. More precisely, for case 2 (ρ_tdc = 31.4 kg/m³), the three mass fractions of the lean zone, rich zone, and over-rich zone are approximately 25%, 35%, and 40%, respectively. In contrast, for case 4 (ρ_tdc = 60.3 kg/m³) the fractions are more evenly distributed as 30% (lean zone), 35% (rich zone), and 35% (over-rich zone). The start of combustion, recognized by the appearance of the fuel mass in M^b, is retarded from 7° to 9° and to 12° CA ATDC as ρ_tdc decreases from 60.3 kg/m³ to 48 kg/m³ and to 31.4 kg/m³. Case 4 with the highest ρ_tdc of 60.3 kg/m³ has the earliest ignition, fastest mass consumption in the equivalence ratio zone of M^u, and the fastest rate of increase in M^b. At approximately 15° CA ATDC, the total M^b can be as high as 95% of the total evaporated fuel, which is distributed as approximately 50% in the lean zone, 25% in the rich zone, and 20% in the over-rich zone. In comparison, case 2 has the lowest ρ_tdc of 31.4 kg/m³, its M^b is nearly zero, and the ignition is barely possible at 15° CA ATDC.

Figure 4.

Effect of ρ_tdc on mass fractions of different equivalence ratio intervals in M^u and M^b with no EGR.

The findings confirm that increasing ρ_tdc does not obviously change the distribution of M^u fractions at the beginning of fuel injection, but significantly enhances the mass transfer rate from M^u to M^b. Enhancing the environment charge of the spray by increasing ρ_tdc would enhance the entrained gas motion, oxygen entrainment, and heat into the spray, resulting in an increased mixing rate of fuel with oxygen and elevated mixture temperature. The local equivalence ratios in M^u are determined by balancing the fuel evaporation rate and mixing rate of evaporated fuel with entrained air. As ρ_tdc increases, the fuel evaporation rate and mixing rate of evaporated fuel are promoted because heat transfer is enhanced by air entrainment. Therefore, the mass fractions of all equivalence ratio zones in M^u do not clearly change in the early stage of combustion. Subsequently, the mass fractions in M^u decrease rapidly as more and more mixtures in M^u zones are transferred to M^b because of an increase in temperature caused by combustion. It can be concluded that transfer rates both from richer zones to leaner zones and from M^u to M^b are strongly dependent on ρ_tdc.

For cases 5, 6, and 7, the combustion control parameters P_b, ρ_tdc, and IVCT are the same as those of cases 2, 3, and 4, respectively, with the exception of the φ_O2 which is 19% (case 5), 18.6% (case 6), and 18.4% (case 7) instead of 21% (case 2–4). Figure 5 shows the change in the mass fractions of various equivalence ratio zones of M^u and M^b. In comparison to Figure 4, it is illustrated that the ignition occurrences for cases 5, 6, and 7 are almost identical to cases 2, 3, and 4, indicating that the ignition occurrence is dominated by ρ_tdc and T_tdc rather than φ_O2 in high-load operations. This is predicted by the ignition delay model.²⁵ However, the mass fractions of rich and over-rich zones in M^u increase by approximately 5% at the beginning of fuel injection due to the low φ_O2; this increase is not significant. However, comparing cases 3 and 6 with the same high ρ_tdc (48 kg/m³) but with different φ_O2 of 21% and 18.6%, respectively, the total mass fractions of M^b in case 3 increase more rapidly than those in case 6 due to the higher φ_O2. This results in considerably faster, early heat release. In contrast, case 6, with a lower φ_O2 of 18.6%, yields a slower, delayed heat release, as illustrated in Figure 6. For the in-cylinder temperatures at injection timing of case 3, 6, and 8 are all above the ignition temperature of the fuel, as a result, the ignition times differ little, however, the lower φ_O2 slows down the combustion rate, thus, the ROHR is slowed down with decreasing φ_O2. Therefore, it can be concluded that lowering the φ_O2 reduces the ROHR and heat release phase.

Figure 5.

Effect of ρ_tdc on the mass fractions of different equivalence ratio intervals in M^u and M^b with basically fixed φ_O2.

Figure 6.

Effect of φ_O2 on ROHR at constant ρ_tdc and IVCT.

Effects of ρ_tdc and φ_O2 on the NO_x, CO, and soot emissions

To analyze the combined effects of ρ_tdc and φ_O2 on NO formation, a combustion process parameter termed as the charge mass averaged temperature is defined as follows:

\bar{T} (ca) = \frac{\sum_{T > 2000 K} m_{i} T_{i}}{\sum_{T > 2000 K} m_{i}}

(1)

where m_i and T_i are the mixture mass and temperature of a calculation cell, respectively. The collected temperature is deliberately set above 2000 K, which is assumed to be the threshold temperature for rapid NO formation. Therefore, the charge mass averaged temperature is a comprehensive measurement of the historical high temperature and high-temperature mass scale. Higher m_i and T_i values result in a higher formation rate of NO. Figure 7 shows the calculated charge mass averaged temperature versus crank angle for all experimental cases in Table 2. In case 2, with a low ρ_tdc of 31.4 kg/m³, a lower mass averaged temperature is obtained in comparison with that of the higher ρ_tdc cases in the early period. However, soon after the start of combustion, it exceeds the higher ρ_tdc cases and lasts for a considerably longer time, resulting in higher NO emissions. In contrast, cases 3 and 4, with higher ρ_tdc, result in slightly lower and shorter mass averaged temperature curves. The effects of ρ_tdc on the charge mass averaged temperature are manifold. On one hand, an increase in ρ_tdc promotes the mixing process and increases NO formation, and on the other hand, an increase in ρ_tdc also increases the heat capacity of the charge. Therefore, the final charge mass averaged temperature is actually a combined result of the two opposing effects of ρ_tdc: the enhancement of the mixing rate and the inhibition of the elevated charge temperature due to heat capacity. The effect of T_tdc on the charge mass averaged temperature can also be observed in Figure 7 by comparing case 1 and case 3. Case 3, with a retarded IVCT and an 82 K lower T_tdc, results in a lower mass averaged temperature curve.

Figure 7.

The deduced mass-averaged temperature for all cases in Table 2.

For cases 5, 6, and 7, all operation control parameters, including P_b, ρ_tdc, and IVCT, are consistent with those of cases 2, 3, and 4, respectively, with the exception of the φ_O2 of 19% (case 5), 18.6% (case 6), and 18.4% (case 7) versus 21% (cases 2–4). This causes the peak of the mass averaged temperature to decrease from approximately 2350 K to approximately 2250 K, and the high temperature duration of the mass averaged temperature curve becomes 10° CA shorter. For case 8, the over-high EGR case with a ρ_tdc of 51 kg/m³ and φ_O2 of 17.2%, the mass averaged temperature is significantly reduced to 2150 K in peak and an additional 15° CA shorter in duration. Therefore, it can be concluded that reducing the in-cylinder φ_O2 can substantially reduce the mass averaged temperature due to the effect of inhibited heat release. Relative to this effect, increasing the ρ_tdc is secondary for decreasing the mass averaged temperature through an increase in charge heat capacity. Moreover, a further increase of ρ_tdc from 48 kg/m³ to 60.3 kg/m³ does not effectively reduce the mass averaged temperature due to the counter action of enhanced mixing and increased heat capacity. Figure 8 shows the calculated NO formation processes for all test cases in which the formation rate, phase, and accumulated quantity are very well correlated to the mass averaged temperature.

Figure 8.

Effect of ρ_tdc, φ_O2, and IVCT on calculated NO formation.

High temperature, high oxygen concentration and high temperature duration time were three key factors to form thermal NO. To further understand this phenomenon, the high temperature abidance scale (HTAS) is defined to analyze NO_x formation and is as follows:

HTAS = \sum_{Δ t} \sum_{T > NFBT} m_{O_{2}} T

(2)

where T is the cell temperature which is higher than the NO_x formation boundary temperature (NFBT), m_O2 is the mass of oxygen in the cell and Δt is the duration of combustion. HTAS is an indication of the duration and scale of the high temperature zone. Figure 9 displays the correlation of HTAS with NO_x emissions in each test case. The number in the frames in the figure denotes the test case number. The results indicate that the NO_x emissions correlate well with the HTAS, higher HTAS leads to higher NO_x emissions.

Figure 9.

Correlation between HTAS and NOx emissions.

To understand the mechanism of lowering φ_O2 by adding EGR to decrease the mass averaged temperature and NO formation, we look at the transfer rate from M^u to M^b. For case 4, with a ρ_tdc of 60.3 kg/m³ and φ_O2 of 21%, the sum of the mass fractions in M^b is approximately 98% at 20° CA ATDC which falls in the lean zone resulting in quick heat release. Compared with case 4, with the same ρ_tdc but a reduced φ_O2 of 18.4%, the sum of the mass fractions in M^b is only 90% for case 7. The sum of the mass fractions in M^b is even lower when the ρ_tdc and φ_O2 are lowered, especially when the mass fraction in the lean zone (0 < Φ ≤ 1) is lower. This allows much of the mixture to leave unburned zones or rich burned zones during the later stage of combustion (e.g. after 20° CA ATDC), causing the presence of a larger fuel fraction as unburned hydrocarbons (UHC) and other intermediate products, including CO. Consequently, the mass averaged temperature is lower, which in turn decreases the transfer rate from M^u to M^b. The presence of different mass fractions of UHCs and intermediate combustion products, resulting from different charge densities and oxygen concentrations, is an important characteristic of diesel combustion paths.

In this study, the intermediate combustion product CO is considered as an indicator of the combustion intermediate products, as shown in Figure 10. The formation of intermediate combustion products, including CO, releases a small quantity of heat according to chemical thermodynamics. Therefore, the mass fraction of CO and its maintenance in the combustion process would retard and slow down the heat release. It would benefit in reduction of NO_x but counter against the oxidation of soot particles and ITE_g. Because soot formed in the early combustion phase can only be oxidized upon contacting oxidizers. Thus, in the later phase of combustion, the mixing rate of soot with the oxidizers, which is effectively promoted by increasing the ρ_tdc, is a decisive factor for soot emission. In this study, the cases of high ρ_tdc combined with moderate φ_O2 (e.g. 18.4%–19%) yield very low NO_x emissions along with acceptable soot emissions. In the formation of CO during the early combustion phase, the fuel releases negligible heat but maintains a “cool atmosphere,” which is favorable for mixing time and avoids the formation of both NO and soot. The fuel refers to the fuel mass in “cold storage of CO”. Figure 6 shows that reducing φ_O2 slows the ROHR and prolongs the overall heat release duration; the increase of CO cold storage is illustrated in Figure 10. However, in the later phase of combustion, the presence of CO produces a lower mixing rate, lower heat release, and lower combustion temperature, which results in lower ITE_g and poor soot emission.

Figure 10.

Effect of ρ_tdc, φ_O2, and IVCT on CO formation.

The factors influencing the cold storage of CO are illustrated according to significance in Figure 10. The ρ_tdc is the most important factor influencing the change of CO. Case 5 shown in Figure 10, with a lower ρ_tdc of 32.5 kg/m³ and lower φ_O2 of 19% exhibits the highest peak of CO at approximately 30° CA ATDC and very slow CO consumption. The operation control parameters of case 2 are the same as those of case 5, with the exception that φ_O2 = 21%, which reduces the peak and final maintenance time of CO. Therefore, φ_O2 is another influencing factor of CO over time. Comparing case 1 with case 3, the T_tdc also affects the order of the CO curves. It is illustrated that the higher values of ρ_tdc result in a lower CO curve. For the cases with the same values of ρ_tdc, φ_O2 is the decisive factor. The higher values of φ_O2 result in a lower CO curve. The concept of accumulated cold storage of CO is introduced, which is the integration of CO mass throughout the combustion process. As shown in Figure 11, the accumulated cold storage of CO correlates well with the measured soot emission and ITE_g. The number in the frames in the figure denotes the test case number. The data with arrowheads denotes the gross indicated thermal efficiency increase, Δη_t, relative to the base case 1. The significance of the influencing factors on the accumulated cold storage of CO is (in ascending order) T_tdc, φ_O2, and ρ_tdc. A higher ρ_tdc, higher φ_O2, and lower T_tdc result in a lower accumulated cold storage of CO, lower soot emission, and higher Δη_t.

Figure 11.

Correlation of soot emission and ITE_g with the accumulated CO cold storage.

Cases 2 and 5, with the lowest ρ_tdc of the test cases, yield the highest accumulated cold storage of CO. For case 6 (ρ_tdc = 48 kg/m³ and φ_O2 = 18.6%) and case 7 (ρ_tdc = 60.4 kg/m³ and φ_O2 = 18.4%), the accumulated cold storage of CO is less in comparison with cases 2 and 5 due to the increased ρ_tdc. Finally, for cases 1, 3, and 4, the accumulated cold storage of CO is further reduced due to the increase in φ_O2 and decrease in T_tdc.

In case 3 (ρ_tdc = 48 kg/m³ and φ_O2 = 21% ) and case 7 (ρ_tdc = 60.4 kg/m³ and φ_O2 = 18.4%), the cold storage of CO plots almost coincide and yield a similar value of measured soot emission and difference of Δη_t at 4%, as shown in Figure 11. A high ρ_tdc can balance the inhibiting effect of low φ_O2 on combustion rate, benefiting NO reduction and increasing soot emission with a limited negative impact on ITE_g. Therefore, the technology of compromising a high ρ_tdc and moderate EGR is very important for diesel mixing-controlled combustion under high-load operations. From Figures 8 and 10, it is found that optimization of the overall engine performance is actually attributed to simultaneously minimizing the HTAS as well as the accumulated cold storage of CO.

Conclusion

The changes in mass fraction of combustion intermediate products, such as CO and UHC, are the significant indicators of combustion paths. This can be represented through the formation phase, quantity versus time, and maintenance duration of the intermediate products. Formation of intermediate products in the early phase of combustion can inhibit heat release, thereby inhibiting the rise of charge temperature, optimizing mixing time, and reducing NO formation. The maintenance of intermediate products in the later phase of combustion is a crucial factor for reducing charge activation, leading to poor thermal efficiency and soot emission.

The charge density and oxygen concentration are the decisive factors affecting formation and maintenance in time and accumulation of the intermediate products in diesel engine combustion at high-load operations. Increase in charge density can activate the combustion and enhance the transfer from intermediate combustion products to complete combustion products. In contrast, the oxygen concentration of the charge can reduce the reactivity of the charge resulting in the formation and maintenance of intermediate products. In comparison with oxygen concentration, charge density is a more significant parameter in the later phase of combustion, affecting the behavior of intermediate products.

The deduced mass averaged temperature and the HTAS correlates very well with the measured NO_x emissions, and the deduced accumulated CO correlates very well with the soot emissions and gross indicated thermal efficiency. Optimization of overall engine performance is attributed to determining a technique to simultaneously minimize the HTAS and the accumulated CO by utilizing proper charge density and EGR.

Footnotes

Appendix

Handling Editor: James Baldwin

Declaration of conflicting interests

The author(s) declared no potential conflicts of interest with respect to the research, authorship, and/or publication of this article.

Funding

The author(s) disclosed receipt of the following financial support for the research, authorship, and/or publication of this article: This research was supported by the Natural Science Foundation of China through its youth project funding (grant number 51806097) and the Open Subject of State Key Laboratory of Engines of Tianjin University (grant number K2018-08).

ORCID iD

Yingying Lu

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Influence of charge density and oxygen concentration on combustion paths,thermal efficiency and emissions in a heavy-duty diesel engine

Abstract

Keywords

Introduction

Experimental set-up and CFD model

Experimental set-up

Numerical simulation models

Results and discussion

Experimental results and discussion

Simulation results and discussion

Combustion path model

Effects of ρtdc and φO2 on the combustion paths

Effects of ρtdc and φO2 on the NOx, CO, and soot emissions

Conclusion

Footnotes

Appendix

Declaration of conflicting interests

Funding

ORCID iD

References

Effects of ρ_tdc and φ_O2 on the combustion paths

Effects of ρ_tdc and φ_O2 on the NO_x, CO, and soot emissions