The Application of Vibroacoustic Mean and Peak-to-Peak Estimates to Assess the Rapidly Changing Thermodynamic Process of Converting Energy Obtained from Various Fuel Compositions Using a CI Engine
Abstract
:1. Introduction
- (a)
- The effectiveness of mapping the course of creation and kinetic combustion of alternative fuel (diesel fuel + DME) in characteristics and vibration parameters (impulsive and energetic) for compression ignition (CI) engines. This study contributes to the development of the knowledge necessary for the application of continuous monitoring and diagnosis of the combustion process (the entire period of operation and taking into account tribological changes in the system), assessment of the correlation between the type of fuel composition and its conversion efficiency, and identification of sources of irregularities (this work will provide graphics and reference parameters for a given fuel, changes between them, and deviations from their values);
- (b)
- Assessment of the quality of the fuel composition determined in relation to emission parameters (CO, HC, NOx, and PM), engine performance indicators, and measures of the vibration process (graphic and parametric representations of this variability). This research complements knowledge in the field of real correlation between the emissions of new fuel and variables affecting them, along with an empirical correlation of emissions with operational and vibration indicators;
- (c)
- Mathematical equations describing the above relationships (emission, vibrations, and indication) in relation to combustion (diesel fuel+DME). This study creates new value in the scope of the mathematical modeling of combustion of new fuels (and hybrid methods), the creation of a database (classical and AI models), and STD (together with the assessment of the uniformity of cyclical combustion kinetics).
2. Analysis of the Knowledge State in Research Topics
- Composition and combustion of DME [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]:
- (a)
- (b)
- (c)
- (d)
- (e)
- (f)
- (g)
- (h)
- (i)
- (j)
- (k)
- (l)
- (m)
- (n)
- The dimethyl ether combustion performance and low NOx emissions of a compression ignition engine at a high injection pressure and a high EGR rate [32] and DME with diesel fuel mixture preliminary injection characterization of the injection rate and the quantity [33], as well as the effects of high EGR rates on DME fuel combustion performance, exhaust emissions, and particle emission characteristics in a small direct injection diesel engine under various injection timings [34].
- Conclusion:
- There is currently widespread interest in science and engineering in various application areas in the use of DME as a natural fuel within its composition with other alternative fuels. The aim of this research is to search for effective fuel that allows for obtaining the highest possible performance indicators of a mechanical object in stationary and non-stationary conditions of its operation, as well as its reliability and the lowest possible emission of harmful exhaust components (meeting future emission regulation requirements). The assessment of knowledge in this area reveals a lack of detailed empirical studies on the quantitative assessment of the combustion kinetics of a specific DME composition with diesel fuel together with its hybrid quantification, taking into account the indicated parameters and exhaust emissions, as well as their connection with vibration processes and their impulse and energy characteristics.
- Vibration diagnostics of the combustion process in the context of DME applications [35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51]:
- (a)
- The diagnostics of methanol active thermal atmosphere combustion in a compression ignition engine using an optical method [35] and the study of internal and external EGR combined with oxygenated n-butanol, polyoxymethylene dimethyl ethers, and dimethyl carbonate fuels to optimize the combustion process of Fischer–Tropsch synthetic diesel [36];
- (b)
- (c)
- (d)
- (e)
- (f)
- (g)
- (h)
- (i)
- An analytical approach to convert a vibration signal to combustion characteristics in diesel engines [51].
- Conclusion:
- The analysis of the set of scientific achievements in the field of diagnosing compression ignition engines clearly indicates the significance of the scientific issues discussed. There are various approaches to this type of problem. They are both in the context of theoretical, empirical, and model approaches, which make it possible to assess the operation of such objects, taking into account the area of their design and operation in specific conditions and for specific fuel. However, these achievements do not include the following aspects:
- (a)
- The empirical and mathematical assessment of the correctness of DME combustion with diesel fuel, taking into account estimates and characteristics of vibration processes;
- (b)
- Linking vibration characteristics with the assessment of emission parameters;
- (c)
- The assessment of the reliability of the impulsive and energy vibration parameters in terms of their vibration equivalents;
- (d)
- The assessment of the sensitivity and statistical reliability of each engine work cycle in relation to its reference representation for the particular fuel composition;
- (e)
- Mapping the kinetic representation of the combustion process in a mathematical model, taking into account engine work variables, fuel properties, and statistical significance of the data set (which is useful for modeling and testing with artificial intelligence methods—mapping continuous monitoring and process and design diagnostics in variable conditions, taking into account learning models for the early identification of irregularities).
3. Experimental Set-Up
- −
- The multichannel high-speed signal acquisition system: B&K Pulse type 3560C.
- −
- The advanced B&K Pulse software platform (version no. 17) for signal data acquisition and analysis (calibration was carried out before each test programmatically).
- −
- The three-axis vibration acceleration transducer: B&K type 4504A.
- −
- The laser encoder: B&K type MM0360 (synchronization of measurement signals with the specific position of an engine crankshaft).
- −
- Number of parallel input/output channels: 5/1.
- −
- Number of auxiliary channels: 16.
- −
- Type of input channels: Direct, CCLD.
- −
- Frequency range [Hz]: 0–25,600.
- −
- Absolute amplitude precision (1 kHz, 1 V input): ±0.05 dB, typical ±0.01 dB.
- −
- Absolute maximum input [Vpeak]: ±35.
- −
- A/D conversion: 2 × 24 bits.
- −
- Voltage [V (DC)]: 10−32.
- −
- Nominal/max power consumption [W]: 30/42.
- −
- Dimensions: height/width/depth [m]: 0.105/0.376/0.300.
- −
- Speed range [rpm]: 0–300,000.
- −
- Operating range: 1.5 (0.6) to > 70 cm (27″) and > 30° from the center line.
- −
- Laser spot: <Ø5 mm at a 70 cm distance.
- −
- Maximum continuous input voltage [V]: −5 to +30.
- −
- Laser class 3R. Visible 660–690 nm, CW, P [optical] < 2mW. Complies with EN/IEC 60825–1: 2007.
- −
- Operating temperature range [°C]: −10 to +50.
- −
- Input type CCLD (DeltaTron or ICP® inputs from 3 to 20 mA), U ≥ 20V.
4. Materials and Methods
4.1. Alternative Fuel Specifications and Their Attainment
- −
- It cannot be used on its own as a fuel for spark-ignition engines (due to its low self-ignition temperature, which increases the risk of knocking combustion);
- −
- Lower viscosity and lubricity than diesel fuel (possible mixture leaks, as well as faster fuel pump wear);
- −
- Chemical stability during storage, diffusion coefficient, and the risk of tank explosion during heating of DME pose a threat (hence the need to store it in liquid form, under moderate pressure, above 0.6 MPa);
- −
- Application requires modification of vehicle power supply systems and creation of a distribution system;
- −
- The calorific value of DME is lower than the calorific value of diesel fuel (larger tanks for DME).
4.2. Methods and Conditions of Empirical Studies
5. Results and Discussion
5.1. Assessment of Fuel Type Impact on Exhaust Compound Concentrations
- −
- It drastically reduced the HC concentration in exhaust gases, with a positive effect on the quality of the combustion and the efficiency of the entire fuel dose utilization in individual engine operation cycles (Table 6). This is related to the DME properties: a favorable O2/C/H2 in %mass (DME = 34.8/52.2/13; diesel = 0/86/14); a lower Molar mass/liquid density in [g/mol]/[kg/m3] (DME = 46.07/667; diesel = 170/831), a better C/H ratio (DME/diesel = 0.337/0.516). The HC concentration was only 1.7–4.1% of the value obtained for diesel fuel in relation to the pressure of 0.2 MPa and 1.0–3.9% of the concentration for the pressure of 0.4 MPa. The increase in load had a clear effect on the HC concentration reduction (regardless of the supply pressure value). A slight HC concentration reduction in the range of 0.2–0.9% (depending on the operating point) was observed when the pressure increased twice. However, this benefit may also constitute an added value to the total emission in the case of taking into account the entire set of vehicles in a given area and their traffic intensity (global effects expected currently and in the future from power sources, taking into account the criteria of maximizing the overall efficiency and minimizing environmental impact).
- −
- It significantly reduced the PM concentration (Table 7), which is more effective the higher the torque and supply pressure are. The amount of PM is 40.5–63.5% of the value obtained for diesel fuel (for a pressure of 0.2 MPa) and 33.8–78.4% of the reference value (for a pressure of 0.4 MPa). The above benefit results from the improvement in combustion conditions and reduction in the average droplet diameter during the work cycle, which affects their better evaporation and increases the share of fuel burned completely (fulfillment of the international postulate in PM emission reduction). The favorable chemical structure of DME, related to the oxygen share (34.8 %mass), lower carbon share by 17.2%, and improvement in the C/H ratio by 34.6%, results in a lower share of both the insoluble fraction (derived from C) and the soluble PM fraction (from the liquid form of HC). A twofold increase in the supply pressure reduces concentrations in the range of 2.6–52.6%. There was no beneficial effect only for the torque of 0 N∙m for the pressure of 0.2 MPa (too low of a supply pressure; lower efficiency of the diesel fuel oxidation process), which was not confirmed in the remaining operating conditions.
- −
- It reduced the CO concentration (Table 8), and the increase in torque resulted in a globally mild CO reduction for both supply pressures (an improvement in combustion stoichiometry conditions and efficiency of fuel conversion into mechanical work). A doubling of the supply pressure had a clear effect on reducing this concentration for higher torques (from 40 N∙m), and for lower values, it was ambiguous or small (0.7% for 0 N∙m).
- −
- It increased the NOx concentration (Table 9), and the more intense it was, the higher the torque value (which is consistent with the combustion theory). The improvement in combustion efficiency is accompanied by an unfavorable emission effect, which intensifies with the supply pressure increase (0.9–7.9%). It can be limited by appropriate corrections in the scope of fuel injection and its combustion, as well as by using DeNOx exhaust gas cleaning systems. The source of higher NOx emission during DME combustion is the higher O2 content, which improves the formation of a homogeneous mixture structure and faster fuel evaporation. This results in improved combustion conditions, visible in the form of higher pressure and temperature in the combustion chamber. The low autoignition temperature and better evaporation of DME favor this phenomenon. A higher cetane number is an additional measure in this area.
- −
- Precise mathematical equations were developed for individual HC, PM, CO, and NOx concentrations in relation to the engine torque, fuel type, and various supply pressures described in more detail in [64], for which the R2 indices were in the range of 0.88–0.96 (for HC), 0.80–0.98 (for PM), 0.95–0.99 (for CO) and 0.97–0.99 (for NOx).
5.2. Evaluation of Fuel Type Impact on Vibration Acceleration Characteristics
5.3. Assessment of Fuel Type Impact on Vibration Diagnostic Parameters
5.4. Estimation of Vibration Diagnostic Parameter Reliability
- −
- Faster fuel evaporation from the cylinders, as well as a shorter combustion time of the DME mixture with air.
- −
- High oxygen content in the molecule, which affects the lowering of the self-ignition temperature of the compound (faster combustion of the DME mixture with air).
- −
- A low boiling point supports faster mixing of air with fuel, which causes a significant acceleration of ignition (due to the lack of direct carbon bonds).
- −
- Even the course of combustion development, resulting from a slower increase in dp/dt in the kinetic phase of the process, is indirectly related to the high cetane number.
- −
- More intensive oxidation is related to the reduction in combustion enthalpy to a level lower than in the case of diesel fuel.
- −
- Bonds in DME disintegrate much faster, which results in a shorter ignition delay.
5.5. Vibration Diagnostic Parameters in Mathematical Relations
- (a)
- For the mean value of the vibration acceleration and diesel fuel:
- (b)
- For the mean value of the vibration acceleration and diesel fuel+DME:
- (c)
- For the peak-to-peak value of the vibration acceleration and diesel fuel:
- (d)
- The peak-to-peak value of the vibration acceleration and diesel fuel+DME:
6. Conclusions
- (a)
- For HC: 1.7–4.1% (pinj = 0.2 MPa) and 1.0–3.9% (for pinj = 0.4 MPa)—Table 6.
- (b)
- For PM: 40.5–63.5% (pinj = 0.2 MPa) and 33.8–78.4% (for pinj = 0.4 MPa)—Table 7.
- (c)
- For CO: 80.5–97.5% (pinj = 0.2 MPa) and 82.8–98.4% (pinj = 0.4 MPa)—Table 8.
- (d)
- For NOx: 101.2–108.1% (pinj = 0.2 MPa) and 103.9–110.6% (pinj = 0.4 MPa)—Table 9.
- (a)
- For the mean value: 0.99 (diesel fuel) and 0.722 (diesel+DME).
- (b)
- For the peak-to-peak value: 0.899 (diesel fuel) and 0.728 (diesel+DME).
- (c)
- For the RMS: 0.925 (diesel fuel) and 0.753 (diesel+DME).
- (d)
- For the peak value: 0.908 (diesel fuel) and 0.709 (diesel+DME).
Author Contributions
Funding
Data Availability Statement
Conflicts of Interest
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Parameter | Unit | Value |
---|---|---|
Engine displacement | cm3 | 1845 |
Width × Length × Height: | cm | 95 × 116 × 116 |
Compression ratio | – | 15.8 |
Engine mass | kg | 650 |
Specific fuel consumption | g/kWh | 245 |
Maximum engine speed | rpm | 2500 |
Maximum torque | N∙m | 140 |
Pressure in the lubrication system | MPa | 0.41 |
Angle of the beginning of fuel delivering to a cylinder (for a previous non-modified fuel injection system) | o | 26 |
Parameter | Unit | Value |
---|---|---|
Frequency | Hz | 1–10,000 |
Sensitivity | mV/g | 10 |
Temperature range | °C | −50–125 |
Residual noise level in spec. freq. range (RMS) | mg | ±0.4 |
Maximum operational/shock level (peak) | g | ±750/±3000 |
Resonance frequency | kHz | 50 |
Triaxial/TEDS/Connector | – | Yes/No/10–32 UNF |
Parameter | Unit | DME | Diesel Fuel | δ = |DME/Diesel| [%] |
---|---|---|---|---|
Molar mass | [g/mol] | 46.07 | 170 | 73 |
Surface tension | [N/m] | 0.012 | 0.027 | 55 |
Liquid density | [kg/m3] | 667 | 831 | 20 |
Kinematic viscosity of liquid | [cSt] | <0.1 | 3 | >97 |
Vapor pressure | [kPa] | 530 | <<10 | >>5200 |
Critical pressure | [MPa] | 5.37 | 3.00 | 79 |
Lower calorific value | [MJ/kg] | 27.6 | 42.5 | 35 |
Lower/Upper explosion limit | [% vol.] | 3.2/18 | 0.6/7 | 433/157 |
Cetane index | 57 | 40–50 | 14–42 | |
Stoichiometric ratio of air and fuel | 9 | 14.6 | 38 | |
C/H ratio | 0.337 | 0.516 | 34 | |
Chemical structure | CH3–O–CH3 | – | – | |
Boiling point at 1atm | °C | −25 | 176–370 | 106–114 |
Critical/Self-ignition temperature | °C | 126/234 | 434/249 | 71/6 |
O2/C/H2 content | [% mass] | 34.8/52.2/13 | 0/86/14 | –/39/7 |
Engine Speed n [rpm] | Engine Torque Mo [N∙m] | Injection Pressure [MPa] | Number of Measurement Series | Emission Compound | ||||
---|---|---|---|---|---|---|---|---|
CO [%] | HC [ppm] | NO [ppm] | CO2 [%] | O2 [%] | ||||
900 | 0 | 40 | 3 | 0–10 | 0–4000 | 0–4000 | 0–16 | 0–25 |
10 | 40 | 3 | ||||||
20 | 40 | 3 | ||||||
30 | 40 | 3 | ||||||
40 | 40 | 3 | ||||||
50 | 40 | 3 |
Fuel Type | Time of Injection tinj [ms] | |||||
---|---|---|---|---|---|---|
0 N∙m | 10 N∙m | 20 N∙m | 30 N∙m | 40 N∙m | 50 N∙m | |
Diesel | 0.89 | 1.04 | 1.19 | 1.4 | 1.75 | 1.97 |
DME (0.2 MPa) | 0.85 | 0.92 | 0.98 | 1.12 | 1.32 | 1.67 |
DME (0.4 MPa) | 0.78 | 0.92 | 0.99 | 1.18 | 1.34 | 1.67 |
δ = (|x1 − x2|/x1) ∗ 100 [%] | 4.5–12.0 | 11.5 | 16.8–17.6 | 15.7–20.0 | 23.4–24.5 | 15.2 |
where x1—value for diesel fuel (reference fuel); x2—value for DME at i-th pressure value (0.2 MPa, 0.4 MPa). |
Fuel Type | HC [%] (Diesel Fuel = 100%) | |||||
---|---|---|---|---|---|---|
0 N∙m | 10 N∙m | 20 N∙m | 30 N∙m | 40 N∙m | 50 N∙m | |
DME (0.2 MPa) | 4.1 | 34.9 | 3.7 | 3.1 | 2.0 | 1.7 |
DME (0.4 MPa) | 3.9 | 3.3 | 2.9 | 2.2 | 1.1 | 1.0 |
∆ = (x1 − x2) [%] | 0.2 | 31.6 | 0.8 | 0.9 | 0.9 | 0.7 |
where x1—value for DME (0.2 MPa); x2—value for DME (0.4 MPa) |
Fuel Type | PM [%] (Diesel Fuel = 100%) | |||||
---|---|---|---|---|---|---|
0 N∙m | 10 N∙m | 20 N∙m | 30 N∙m | 40 N∙m | 50 N∙m | |
DME (0.2 MPa) | 100 | 63.5 | 49.3 | 99.0 | 40.5 | 52.7 |
DME (0.4 MPa) | 78.4 | 60.3 | 46.7 | 46.4 | 33.8 | 45.1 |
∆ = (x1 − x2) [%] | 21.6 | 3.2 | 2.6 | 52.6 | 6.7 | 7.6 |
Fuel Type | CO [%] (Diesel Fuel = 100%) | |||||
---|---|---|---|---|---|---|
0 N∙m | 10 N∙m | 20 N∙m | 30 N∙m | 40 N∙m | 50 N∙m | |
DME (0.2 MPa) | 96.7 | 97.5 | 82.5 | 80.5 | 95.1 | 94.6 |
DME (0.4 MPa) | 96.0 | 98.4 | 111.3 | 82.8 | 91.4 | 87.8 |
∆ = (x1 − x2) [%] | 0.7 | −0.9 | −28.8 | −2.3 | 3.7 | 6.8 |
Fuel Type | NOx [%] (Diesel Fuel = 100%) | |||||
---|---|---|---|---|---|---|
0 N∙m | 10 N∙m | 20 N∙m | 30 N∙m | 40 N∙m | 50 N∙m | |
DME (0.2 MPa) | 101.2 | 102.7 | 105.2 | 108.1 | 105.2 | 101.9 |
DME (0.4 MPa) | 108.3 | 110.6 | 106.1 | 103.9 | 109.5 | 108.9 |
∆ = (x1 − x2) [%] | −7.1 | −7.9 | −0.9 | 4.2 | −4.3 | −7.0 |
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Waligórski, M.; Bajerlein, M.; Karpiuk, W.; Smolec, R.; Pełczyński, J. The Application of Vibroacoustic Mean and Peak-to-Peak Estimates to Assess the Rapidly Changing Thermodynamic Process of Converting Energy Obtained from Various Fuel Compositions Using a CI Engine. Energies 2025, 18, 1091. https://doi.org/10.3390/en18051091
Waligórski M, Bajerlein M, Karpiuk W, Smolec R, Pełczyński J. The Application of Vibroacoustic Mean and Peak-to-Peak Estimates to Assess the Rapidly Changing Thermodynamic Process of Converting Energy Obtained from Various Fuel Compositions Using a CI Engine. Energies. 2025; 18(5):1091. https://doi.org/10.3390/en18051091
Chicago/Turabian StyleWaligórski, Marek, Maciej Bajerlein, Wojciech Karpiuk, Rafał Smolec, and Jakub Pełczyński. 2025. "The Application of Vibroacoustic Mean and Peak-to-Peak Estimates to Assess the Rapidly Changing Thermodynamic Process of Converting Energy Obtained from Various Fuel Compositions Using a CI Engine" Energies 18, no. 5: 1091. https://doi.org/10.3390/en18051091
APA StyleWaligórski, M., Bajerlein, M., Karpiuk, W., Smolec, R., & Pełczyński, J. (2025). The Application of Vibroacoustic Mean and Peak-to-Peak Estimates to Assess the Rapidly Changing Thermodynamic Process of Converting Energy Obtained from Various Fuel Compositions Using a CI Engine. Energies, 18(5), 1091. https://doi.org/10.3390/en18051091