Using Statistical Methods to Identify the Impact of Solid Fuel Boilers on Seasonal Changes in Air Pollution
Abstract
1. Introduction
2. Materials and Method
2.1. Air Pollution Measurement Methodology
- Humidity measurement: Measurement accuracy ±3% (in the absolute humidity range from 20% to 80%).
- Pressure measurement: Measurement accuracy ±0.12% (in the barometric pressure range from 700 kPa to 900 kPa).
- Temperature measurement accuracy:
- ○
- ±0.5% (in the temperature range from 0 to 65 °C);
- ○
- ±1.25% (in the temperature range from −20 to 0 °C);
- ○
- ±1.5% (in the temperature range from −40 to −20 °C).
2.2. Characteristics of Low-Power Boilers with Manual Fuel Loading
- Periodic increases in thermal energy demand resulting from seasonal changes and seasonal drops in outdoor temperatures observed between October and April. This is a natural phenomenon occurring in the analyzed climate zone, requiring residents to utilize heating devices to ensure comfortable living conditions. During these periods, we recorded local increases in air pollution resulting from the operation of the heating devices presented.
- Daily changes in air pollution indicators resulting from the operating characteristics of boilers with manual fuel loading. Technical data regarding the operation of these devices indicate that the boilers have a burn time of up to 24 h; unfortunately, in real conditions, the burn time is limited to a range of 6 to 12 h, depending on the outside temperature and the amount of fuel loaded [43,44].
- Fuel loading. Due to the residents’ lifestyles, this phase typically begins in the afternoon after returning from work. It can be assumed that most residents work a single shift and return home between 3 and 5 PM. During this period, both the boiler and the heating system are completely cooled (the water temperature in the boiler is approximately 20 °C). The boiler should be cleaned of ash and any remaining burnt fuel. A new batch of fuel, ranging from a few to a dozen kilograms, is then loaded. In addition to the fuel, a “kindling” in the form of pieces of wood or other materials is also placed in the boiler to ensure a quick flame with a combustion temperature sufficient to ignite the primary fuel (coal, fine coal, wood).
- Ignition phase. This is the combustion phase that produces the highest levels of pollutants. This phase lasts from one to several hours. During this phase, flammable materials ignite, with combustion temperatures sufficient to ignite the main fuel bed. The combustion process involves both the combustion of solid carbon and the combustion of volatile combustible components released from the fuel as a result of degassing, which is one of the combustion phases. During this phase, the combustion chamber is at a low temperature, preventing rapid degassing of combustible components. This combustion phase produces high emissions of carbon monoxide and soot, which are not combusted due to the low temperature of this process.
- The boiler operating parameters stabilization phase. After the ignition period, the combustion process gradually stabilizes. This phase lasts approximately 1 h. During this time, the water in the boiler and heating system reaches a temperature of 50 to 70 °C, which guarantees an increase in the temperature in the combustion chamber. In this phase of the combustion process, pollutant emissions gradually decrease, but the observed level of emitted pollutants still exceeds the emission standards for class 3 and 4 boilers according to PN-EN 303-5:2012.
- The stable combustion phase. This is the longest phase of the combustion process, lasting from 6 to 7 hours. During this period, the boiler operates stably. The building’s energy performance, in the form of poor thermal insulation, guarantees stable heat collection, enabling a uniform combustion process. Pollutant emissions are reduced.
- The bed burnout phase. This is the final phase of the combustion process. The fuel is completely burned, and the boiler water temperature gradually drops. During this phase, we observe low pollutant emissions and high oxygen concentration in the exhaust gases resulting from the absence of combustible substances. This phase lasts approximately one hour.
3. Results
- Standard combustion process (SCP)—Weekdays, when most residents return home in the afternoon.
- Weekend (WEEKEND)—Days off from work, characterized by a different lifestyle of the residents.
- Constant heat reception (CHR)—Days with forced, continuous boiler operation cycle with manual fuel loading. The heating system does not cool down because the low outside temperature remains at a similar level throughout the day.
- Int0: Hours in the interval between [3.00 PM and 9.00 PM);
- Int1: Hours in the interval between [9.00 PM and 9.00 AM);
- Int2: Hours in the interval between [9.00 AM and 3.00 PM).
3.1. Air Pollution Recording Results for the Pleszew Administrative Area (Poland) over the Years 2022–2024
- Average annual limit: 15 µg/m3 (previously 20 µg/m3);
- Daily limit: 45 µg/m3 (previously 50 µg/m3).
- Annual limit: 40 µg/m3;
- Daily limit: 50 µg/m3.
- The impact of air temperature outside heated buildings (relative to boiler use intensity) on PM10 levels. We answer the question of how PM10 values change depending on the temperature. Based on the years 2022–2024, we created a prediction model for each month that allowed us to predict the level of PM10 pollution in the future depending on the temperature.
- For randomly selected days, we analyzed how PM10 concentrations changed over the course of a single 24 h period depending on the time of day. This is, of course, closely related to the stages of the combustion process, i.e., the operation of hand-fired grate boilers. This confirmed the thesis that hand-fired grate boilers are the main cause of increased air pollution on a daily and hourly basis.
3.2. Daily Distribution of Air Pollution for the Administrative Area of Pleszew (Poland) over the Years 2022–2024
3.3. Linear Regression Model
- sxy is the sample covariance: ;
- is the sample standard deviation for the variable X, ;
- is the sample standard deviation for the variable Y, .
- 0—No linear relationship;
- 0–0.2—Very weak linear relationship;
- 0.2–0.4—Weak linear relationship;
- 0.4–0.6—Moderate linear relationship;
- 0.6–0.8—Strong linear relationship;
- 0.8–1—Very strong linear relationship.
- Jan—Data from January 2022, January 2023, and January 2024 taken together;
- Feb—Data from February 2022, February 2023, and February 2024 taken together;
- …
- Dec—Data from December 2022, December 2023, and December 2024 taken together.
- is the observed individual i-th value in the j-th year (random variable, dependent);
- is the intercept of the linear regression (fixed parameter);
- is the linear regression coefficient (fixed parameter);
- is the i-th value of the independent variable (covariate) in the j-th year;
- is the random effect of the j-th year;
- is the random error of the i-th observation in the j-th year.
- , ;
- , ;
- , .
3.4. Regression Analysis of PM10 Concentration on Temperature
- is the observed individual i-th value (random, dependent variable);
- is the intercept of linear regression (fixed parameter);
- is the linear regression coefficient (fixed parameter);
- is the i-th value of the independent variable (covariate);
- is the random error of the i-th observation.
- , ;
- , .
3.5. Daily and Hourly Air Pollution Analysis
- (1)
- on 15 November 2022 and two days preceding and two days following (five consecutive days randomly selected from the 2022 heating period);
- (2)
- on three randomly selected days from the 2023 heating period (a spring day, an autumn day, and a winter day);
- (3)
- on randomly selected days (from three years), taking into account the combustion process and heat reception.
- means the average concentration of PM10 during the time interval Int0, i.e., in the hourly interval from [3:00 PM to 9:00 PM);
- means the average concentration of PM10 during the time interval Int1, i.e., in the hourly interval from [9:00 PM to 9:00 AM);
- means the average concentration of PM10 during the time interval Int2, i.e., in the hourly interval from [9:00 AM to 3:00 PM).
- 15 November 2022—Tuesday;
- 15 March 2023—Wednesday;
- 23 October 2023—Monday;
- 14 April 2024—Monday.
- 19 November 2022—Saturday;
- 10 February 2024—Saturday.
- 12 November 2024—Tuesday—Temperature around 0 °C all day.
4. Discussion and Conclusions
- The statistical analysis carried out in this study showed a significant relationship between the temperature drop and the increase in the concentration of suspended PM10 particulate matter in the heating season, which confirms the hypothesis about the dominant influence of atmospheric conditions (especially low temperature) on pollutant emissions.
- The key role of manually hand-fired boilers in shaping the level of particulate matter emissions was pointed out, which suggests the need for further regulation and modernization of this type of combustion source.
- The daily PM10 standard, i.e., 50 µg/m3 (according to EU regulations), was exceeded on days when constant heat removal occurred due to low outside temperatures.
- Division of the day into three time intervals (Int0, Int1, Int2) proved to be an effective analytical tool enabling the identification of periods with the highest risk of high PM10 concentrations.
- The highest concentrations were recorded in the autumn–winter season during the afternoon and evening hours (Int0) on weekdays, which is associated with the intensification of solid fuel combustion in households.
- The results confirm that pollutant emissions are not solely a function of technical factors but are also significantly related to residents’ lifestyles, highlighting the importance of social aspects in air quality research.
- The developed linear regression model enables effective forecasting of local PM10 concentrations depending on temperature, which is a useful tool in planning environmental policy and preventive measures.
- The conducted analysis of variance (ANOVA) and Tukey’s post hoc tests revealed significant differences among the average particulate matter concentrations during the three daily intervals, indicating the complex nature of emission dynamics and the need to account for temporal variability in research and modeling.
Author Contributions
Funding
Data Availability Statement
Conflicts of Interest
Abbreviations
ANOVA | Analysis of Variance |
CHR | Constant Heat Reception |
EU | European Union |
PM | Particulate Matter |
SCP | Standard Combustion Process |
WHO | World Health Organization |
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Month | 2022 | 2023 | 2024 |
---|---|---|---|
January | 40.24 | 34.84 | 39.81 |
February | 23.34 | 41.48 | 29.46 |
March | 54.30 | 34.44 | 38.02 |
April | 25.64 | 29.58 | 17.23 |
May | 12.98 | 16.12 | 13.62 |
June | 12.51 | 14.65 | 13.05 |
July | 7.97 | 8.44 | 9.80 |
August | 11.59 | 10.61 | 13.21 |
September | 15.01 | 17.31 | 19.88 |
October | 27.31 | 22.39 | 29.61 |
November | 44.29 | 32.26 | 36.16 |
December | 43.47 | 42.02 | 29.41 |
Annual average: | 26.61 | 25.23 | 24.09 |
Month: | Jan | Feb | Mar | Apr | May | Jun | Jul | Aug | Sep | Oct | Nov | Dec |
---|---|---|---|---|---|---|---|---|---|---|---|---|
r | −0.54 | −0.34 | −0.21 | 0.01 | 0.07 | 0.37 | 0.58 | 0.72 | 0.17 | −0.05 | −0.45 | −0.62 |
December | |
---|---|
Temperature [°C] | PM10 [µg/m3] |
−10 | 96.9123 |
−5 | 74.7538 |
0 | 52.5953 |
5 | 30.4368 |
10 | 8.2783 |
Day | p Value of ANOVA |
---|---|
13 November 2022 | <0.001 *** |
14 November 2022 | <0.001 *** |
15 November 2022 | <0.001 *** |
16 November 2022 | <0.001 *** |
17 November 2022 | <0.001 *** |
Day | Hour | Interval | Mean Value of PM10 | Tukey Group |
---|---|---|---|---|
13 November 2022 | [3:00 PM–9:00 PM) | Int0 | 56.55556 | a |
[9:00 AM–3:00 PM) | Int2 | 47.12500 | b | |
[9:00 PM–9:00 AM) | Int1 | 44.15278 | b | |
14 November 2022 | [3:00 PM–9:00 PM) | Int0 | 49.08333 | a |
[9:00 PM–9:00 AM) | Int1 | 48.75694 | a | |
[9:00 AM–3:00 PM) | Int2 | 38.09722 | b | |
15 November 2022 | [3:00 PM–9:00 PM) | Int0 | 70.59722 | a |
[9:00 AM–3:00 PM) | Int2 | 58.29167 | b | |
[9:00 PM–9:00 AM) | Int1 | 49.59722 | c | |
16 November 2022 | [9:00 PM–9:00 AM) | Int1 | 26.77083 | a |
[9:00 AM–3:00 PM) | Int2 | 17.63889 | b | |
[3:00 PM–9:00 PM) | Int0 | 10.79167 | c | |
17 November 2022 | [3:00 PM–9:00 PM) | Int0 | 32.05556 | a |
[9:00 PM–9:00 AM) | Int1 | 23.50694 | b | |
[9:00 AM–3:00 PM) | Int2 | 22.16667 | b |
Day | Hour | Interval | Mean Value of PM10 | Tukey Group |
---|---|---|---|---|
15 March 2023 | [3:00 PM–9:00 PM) | Int0 | 57.38889 | a |
[9:00 PM–9:00 AM) | Int1 | 32.04167 | b | |
[9:00 AM–3:00 PM) | Int2 | 10.61111 | c | |
23 October 2023 | [3:00 PM–9:00 PM) | Int0 | 40.86111 | a |
[9:00 PM–9:00 AM) | Int1 | 27.13889 | b | |
[9:00 AM–3:00 PM) | Int2 | 17.5000 | c | |
1 December 2023 | [3:00 PM–9:00 PM) | Int0 | 240.7222 | a |
[9:00 PM–9:00 AM) | Int2 | 186.3611 | b | |
[9:00 AM–3:00 PM) | Int1 | 153.9028 | c |
Day | Hour | Interval | Mean Value of PM10 | Tukey Group | |
---|---|---|---|---|---|
SCP (Tuesday) | 15 November 2022 | [3:00 PM–9:00 PM) | Int0 | 70.59722 | a |
[9:00 AM–3:00 PM) | Int2 | 58.29167 | b | ||
[9:00 PM–9:00 AM) | Int1 | 49.59722 | c | ||
SCP (Wednesday) | 15 March 2023 | [3:00 PM–9:00 PM) | Int0 | 57.38889 | a |
[9:00 PM–9:00 AM) | Int1 | 32.04167 | b | ||
[9:00 AM–3:00 PM) | Int2 | 10.61111 | c | ||
SCP (Monday) | 23 October 2023 | [3:00 PM–9:00 PM) | Int0 | 40.86111 | a |
[9:00 PM–9:00 AM) | Int1 | 27.13889 | b | ||
[9:00 AM–3:00 PM) | Int2 | 17.5000 | c | ||
SCP (Monday) | 14 April 2024 | [3:00 PM–9:00 PM) | Int0 | 21.861111 | a |
[9:00 PM–9:00 AM) | Int1 | 10.722222 | b | ||
[9:00 AM–3:00 PM) | Int2 | 5.111111 | b | ||
WEEKEND (Saturday) | 19 November 2022 | [9:00 PM–9:00 AM) | Int1 | 39.22222 | a |
[3:00 PM–9:00 PM) | Int0 | 30.31944 | b | ||
[9:00 AM–3:00 PM) | Int2 | 28.500 | b | ||
WEEKEND (Saturday) | 10 February 2024 | [9:00 PM–9:00 AM) | Int1 | 58.47222 | a |
[3:00 PM–9:00 PM) | Int0 | 53.58333 | b | ||
[9:00 AM–3:00 PM) | Int2 | 46.33333 | c | ||
CHR (Tuesday) | 12 November 2024 | [9:00 AM–3:00 PM) | Int2 | 55.36111 | a |
[9:00 PM–9:00 AM) | Int1 | 52.90278 | ab | ||
[3:00 PM–9:00 PM) | Int0 | 51.63889 | b |
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Share and Cite
Bakinowska, E.; Dota, A.; Urbaniak, R.; Ciupek, B.; Żurawski, M.; Dębczyński, M. Using Statistical Methods to Identify the Impact of Solid Fuel Boilers on Seasonal Changes in Air Pollution. Energies 2025, 18, 5428. https://doi.org/10.3390/en18205428
Bakinowska E, Dota A, Urbaniak R, Ciupek B, Żurawski M, Dębczyński M. Using Statistical Methods to Identify the Impact of Solid Fuel Boilers on Seasonal Changes in Air Pollution. Energies. 2025; 18(20):5428. https://doi.org/10.3390/en18205428
Chicago/Turabian StyleBakinowska, Ewa, Alicja Dota, Rafał Urbaniak, Bartosz Ciupek, Marcin Żurawski, and Marek Dębczyński. 2025. "Using Statistical Methods to Identify the Impact of Solid Fuel Boilers on Seasonal Changes in Air Pollution" Energies 18, no. 20: 5428. https://doi.org/10.3390/en18205428
APA StyleBakinowska, E., Dota, A., Urbaniak, R., Ciupek, B., Żurawski, M., & Dębczyński, M. (2025). Using Statistical Methods to Identify the Impact of Solid Fuel Boilers on Seasonal Changes in Air Pollution. Energies, 18(20), 5428. https://doi.org/10.3390/en18205428