Environmentally, the results highlight a distinct trade-off between carbon reduction and NOx formation. CO2 emissions decrease nearly linearly with increasing hydrogen content, achieving a reduction of approximately 20% at 20% hydrogen blending, which directly reflects the lower carbon intensity of the fuel mixture. At the same time, NOx emissions increase from 40 mg/kWh to 52 mg/kWh, indicating intensified thermal NOx formation driven by higher flame temperatures and increased radical concentrations. In contrast, CO emissions remain low and stable, while particulate matter remains negligible across all conditions, confirming that combustion completeness is maintained despite changes in fuel composition.
3.1. The Operational Test Results
The introduction of hydrogen led to a measurable increase in combustion reactivity, thereby improving ignition stability, particularly at lower load conditions. This effect is quantified in
Figure 3, which shows a systematic reduction in ignition delay with increasing hydrogen volumetric fraction, indicating enhanced fuel reactivity and improved ignition performance.
Figure 3 shows that the ignition delay decreases markedly with increasing hydrogen fraction, confirming the enhanced reactivity of the fuel mixture. The ignition delay is reduced from 120 ms at 0% H
2 to 105 ms at 10% H
2 and further to 95 ms at 20% H
2, corresponding to an overall reduction of about 10–11% across the investigated range. This reduction reflects the lower ignition energy and higher diffusivity of hydrogen, which facilitate faster initiation of combustion reactions. The observed trend indicates that hydrogen addition accelerates the pre-flame chemical processes, particularly through increased availability of reactive radicals such as H, O, and OH, which promote chain-branching reactions and shorten ignition times [
62]. As a result, the combustion process becomes more stable, especially under conditions where ignition would otherwise be delayed, such as at reduced loads or during transient operation.
From an operational viewpoint, the decrease in ignition delay contributes to improved flame anchoring and reduced risk of flame instability or blow-off. The relatively linear reduction observed in
Figure 3 also suggests a predictable and controllable relationship between hydrogen fraction and ignition behavior, which is advantageous for combustion system optimization.
The data presented in
Table 7 indicate that combustion stability is largely maintained across the investigated hydrogen blending range, with stable operation observed up to at least 20% hydrogen by volume.
Key stability indicators show only minor deviations, with fluctuations in flame behavior remaining within a narrow margin (typically below 3–5% variation compared to the baseline case of 100% methane). No instances of flame instability or blow-off were recorded, suggesting that the boiler system accommodated moderate hydrogen admixtures without compromising operational safety. Under the investigated operating conditions, no measurable decrease in boiler efficiency was observed with increasing hydrogen fraction.
Additionally, combustion characteristics such as flame speed and heat release rate exhibit measurable changes, with hydrogen-enriched mixtures showing faster combustion kinetics. This can enhance mixing and combustion completeness but may also require minor adjustments in burner control settings to maintain optimal air–fuel ratios. Despite these changes, the overall thermal output of the system remains relatively stable, with deviations generally within ±2% across the tested scenarios.
Also, thermal output and boiler efficiency remain constant across all tested fuel compositions, indicating that hydrogen substitution does not introduce efficiency penalties under short-term nominal operating conditions. A systematic reduction in ignition delay is observed with increasing hydrogen content, reflecting enhanced fuel reactivity and improved ignition characteristics.
As shown in
Figure 4, hydrogen enrichment leads to a systematic modification of key combustion characteristics. The adiabatic flame temperature increases from 1950 °C at 0% H
2 to 2020 °C at 10% H
2 and 2100 °C at 20% H
2, corresponding to an overall increase of approximately 5.1%.
This trend is accompanied by a rise in laminar flame speed from 0.38 m/s to 0.45 m/s and 0.52 m/s, representing an increase of nearly 37%, which reflects the enhanced reactivity and faster combustion kinetics associated with hydrogen addition.
Because only three hydrogen blending ratios (0%, 10%, and 20%) were experimentally investigated, the curve shown in
Figure 4 is intended only to facilitate visualization of the observed trend and should not be interpreted as a fitted mathematical relationship.
In terms of emissions, when expressed per unit of useful thermal energy delivered by the boiler, CO2 intensity decreased from 202 kg/MWh for pure methane operation to 181 kg/MWh at 10 vol.% H2 and to 161 kg/MWh at 20 vol.% H2. The observed reduction reflects the lower carbon intensity of the blended fuel under constant-load operation and should not be interpreted as implying a universally proportional relationship between volumetric hydrogen substitution and energy-normalized CO2 emissions. Conversely, NOx emissions increase from 40 mg/kWh at 0% H2 to 45 mg/kWh at 10% H2 and 52 mg/kWh at 20% H2, corresponding to a relative increase of approximately 30%, primarily due to elevated flame temperatures and intensified thermal NOx formation pathways.
CO emissions remain low and stable, decreasing slightly from 7 mg/kWh to 6 mg/kWh at higher hydrogen fractions, indicating consistently complete combustion. Particulate matter emissions remain below the detection limit (<1 mg/m3) across all conditions, confirming the absence of solid-phase formation mechanisms in the gaseous fuel system.
From a GHG emissions perspective again, and as shown in
Table 8, CO
2 emissions decreased linearly with increasing hydrogen fraction, while CO emissions remained low and stable across all test conditions, with measured values of 7 mg/kWh at 0% H
2 and 6 mg/kWh at both 10% and 20% H
2, indicating complete combustion with no measurable formation of incomplete oxidation products. Particulate matter (PM) emissions were below the detection limit of the measurement system (<1 mg/m
3) throughout all operational tests, which is consistent with the absence of solid-phase precursors in the gaseous fuel mixture.
In contrast, NOx emissions increased from 40 mg/kWh at 0% H2 to 45 mg/kWh at 10% H2 and 52 mg/kWh at 20% H2, corresponding to an overall increase of approximately 30% across the investigated hydrogen blending range. This increase is attributed to elevated flame temperatures and enhanced thermal NOx formation mechanisms associated with hydrogen-enriched combustion.
CO2 emissions decreased systematically with increasing hydrogen substitution, from 202 kg/MWh at 0% H2 to 181 kg/MWh at 10% H2 and 161 kg/MWh at 20% H2, corresponding to an overall reduction of approximately 20% across the investigated hydrogen blending range. Although the decrease in CO2 emissions closely followed the increase in hydrogen fraction under the investigated operating conditions, this relationship should not be interpreted as universally linear because it is influenced by the lower volumetric energy density of hydrogen and by the normalization of emissions to delivered thermal energy.
This trend closely follows theoretical expectations based on the reduced carbon content of the fuel mixture, confirming that the observed emission reductions are primarily governed by fuel composition rather than operational variability. The nearly linear decrease in CO2 emissions indicates stable combustion conditions and consistent fuel–air mixing across all test cases, with no evidence of incomplete combustion or efficiency losses. These results demonstrate that hydrogen blending provides a direct and effective pathway for reducing carbon intensity in thermal energy production without adversely affecting combustion performance.
These results demonstrate that the environmental benefits of hydrogen blending can be achieved without compromising emission compliance when appropriate combustion control strategies are applied.
In terms of emissions, the combined effect of increased excess air and implicit air staging plays a key role in controlling NOx formation. While hydrogen addition promotes NOx formation through higher flame temperatures and radical concentrations, the applied control strategy effectively limits peak temperatures and stabilizes combustion. Consequently, NOx emissions remained within applicable regulatory limits across all tested conditions.
The combined emission trends for CO
2 and NO
x as a function of hydrogen blending ratio are shown in
Figure 5, highlighting the trade-off between GHG emission reduction and NO
x formation.
The observed trade-off between reduced CO
2 emissions and increased NO
x formation represents a key challenge in the implementation of hydrogen-enriched combustion systems. While the reduction in CO
2 emissions is directly linked to the lower carbon content of the fuel mixture, the increase in NO
x emissions can be attributed primarily to elevated flame temperatures and enhanced reaction kinetics associated with hydrogen addition. The higher adiabatic flame temperature promotes thermal NO
x formation via the Zeldovich mechanism [
63], leading to the increasing trend observed in
Figure 5.
This trade-off has important implications for the operation and retrofitting of existing DH boilers. Although hydrogen blending contributes to decarbonization goals, the corresponding rise in NOx emissions may necessitate the implementation of additional emission control strategies to ensure compliance with environmental regulations. These may include optimization of excess air ratios, staged combustion techniques, flue gas recirculation, or the integration of post-combustion treatment systems such as selective non-catalytic reduction or selective catalytic reduction. Furthermore, the balance between CO2 reduction and NOx increase must be evaluated in the context of system-level optimization, where operational parameters are adjusted to minimize total environmental impact rather than a single emission component. This highlights the importance of integrated approaches combining fuel composition control, combustion tuning, and emission mitigation technologies.
The measured NO
x emissions remained within applicable regulatory limits throughout all experimental conditions. In the context of the study, these limits are defined by the EU Industrial Emissions Directive [
64] and corresponding national Latvian regulations for medium-scale combustion plants, which typically specify NO
x emission thresholds in the range of 100–200 mg/Nm
3, depending on plant classification and operating regime.
At the highest investigated hydrogen blending ratio (20% H2), NOx emissions approached the upper range of baseline values but remained safely below the applicable emission limits, indicating that hydrogen enrichment at this level does not compromise regulatory compliance under the tested conditions. Nevertheless, the observed increasing trend highlights the importance of active combustion control to prevent exceedance at higher hydrogen fractions or under transient operation. To maintain compliance, the boiler control system continuously adjusted key operational parameters, particularly the air-to-fuel ratio and excess air coefficient, based on real-time feedback from oxygen sensors and flue gas measurements. This dynamic control strategy enabled stabilization of combustion temperature and oxygen availability, thereby limiting thermal NOx formation. In addition, implicit air staging effects, resulting from burner design and flow distribution, contributed to moderating peak flame temperatures. The combination of these control mechanisms ensured that NOx emissions remained within regulatory thresholds while preserving stable and efficient boiler operation.
Slight, non-critical variations in the Wobbe index associated with hydrogen addition, shown in
Table 9, were also observed.
This trend indicates the significantly lower volumetric energy density of hydrogen compared to methane, despite hydrogen’s high gravimetric energy content. As the hydrogen fraction rises from 0% to 20%, the reduction in Wobbe Index suggests that, under constant pressure conditions, a larger volumetric flow rate of fuel would be required to deliver the same thermal input. This has direct implications for the compatibility of existing gas infrastructure and end-use appliances, particularly those calibrated for a narrow Wobbe Index range. Although the observed decrease remains within tolerable limits for many conventional gas systems, indicating that moderate hydrogen blending can be accommodated without substantial hardware modifications. However, the gradual shift in gas quality parameters may influence burner performance, air–fuel mixing behavior, and combustion efficiency. Therefore, while the results support the technical feasibility of methane-based gas and hydrogen blending from a calorific standpoint, they also highlight the importance of regulatory standards and adaptive control strategies to ensure safe and efficient operation across varying blend compositions.
During the operational tests, hydrogen-sensitive monitoring systems detected no leakage, and ventilation systems-maintained hydrogen concentrations well below safety thresholds. Emergency shutdown systems responded correctly during simulated fault conditions, and control system alarms functioned as designed. Operator workload did not increase during blended-fuel operation, and routine maintenance requirements remained unchanged compared with baseline methane-based gas operation.
Post-test material inspections revealed no visible degradation of pipelines, valves, seals, or heat exchanger components. No evidence of hydrogen-induced embrittlement or abnormal corrosion was observed after the gas mixture exposure period. However, it should be noted that the tests were conducted over relatively short-term operating intervals, which are not sufficient to capture long-term material degradation mechanisms. Phenomena such as hydrogen embrittlement, microstructural changes, and cumulative corrosion effects typically develop over extended exposure durations and under cyclic loading conditions. While the results indicate that no immediate or short-term material compatibility issues arise under the tested hydrogen blending conditions, these findings cannot be directly extrapolated to long-term operation.
Instrumentation performance was uninterrupted despite increased moisture content in the flue gas, and data-acquisition systems provided high-resolution diagnostics of combustion behaviour and emissions. Repeatability tests conducted under identical operating conditions confirmed the consistency and robustness of the experimental results, with system availability maintained at 100% throughout the operational tests.
The results generally confirmed that hydrogen co-combustion up to a 20% volumetric share is technically feasible, operationally stable, and environmentally effective for medium-scale DH applications. The system demonstrated sufficient adaptability to accommodate changes in fuel composition without compromising safety, performance, or regulatory compliance. The experimental outcomes align closely with findings reported in comparable pilot projects and provide strong evidence supporting hydrogen blending as a near-term decarbonization pathway. Boiler house A case study, therefore, serves as a highly replicable reference for similar DH installations across the EU and provides a solid empirical basis for future scale-up, long-term operation, and policy-supported deployment.
Boiler thermal efficiency remained statistically unchanged across all investigated hydrogen blending ratios (0%, 10%, and 20% H2), with observed variations remaining within the bounds of measurement uncertainty (±0.5%). Statistical analysis confirmed that the differences between the mean efficiency values at different hydrogen fractions were not statistically significant (p > 0.05), indicating that hydrogen addition had no measurable effect on the overall energy conversion efficiency under steady-state operating conditions.
Thermodynamically, the stability of thermal efficiency can be explained by the balance between two opposing effects. On the one hand, hydrogen has a lower volumetric calorific value compared to methane, which could potentially reduce the energy density of the fuel mixture. On the other hand, hydrogen exhibits higher reactivity and flame speed, promoting more complete combustion and efficient heat release. The experimental results indicate that these effects compensate each other, resulting in no measurable efficiency penalty.
The results also demonstrate that condensing heat recovery performance was not negatively affected by increased water vapor content. On the contrary, the elevated water vapor fraction may enhance the potential for latent heat recovery, if flue gas temperatures remain below the dew point. Although the increased water vapor content may influence condensation behavior and latent heat recovery, the present experimental results showed no measurable change in overall boiler efficiency under the investigated operating conditions. Relationship between hydrogen fraction and boiler performance parameters is visualized in
Figure 6.
The figure presents the variation of boiler thermal efficiency and flue gas water vapor content as a function of hydrogen volumetric fraction in the fuel mixture (0–20%). The results demonstrate that thermal efficiency remains effectively constant across the investigated range, with only minor fluctuations that fall within the measurement uncertainty (±0.5%). This indicates that the substitution of methane with hydrogen does not lead to any measurable deterioration in the overall energy conversion efficiency of the boiler under steady-state operating conditions.
In contrast, the water vapor content in the flue gas exhibits a clear increasing trend with rising hydrogen fraction, reflecting the higher hydrogen-to-carbon ratio of the fuel mixture and the corresponding increase in water formation during combustion. This behavior is consistent with stoichiometric combustion principles, whereby hydrogen oxidation produces a greater proportion of water vapor compared to methane-based fuels.
3.2. Statistical Evaluation of Experimental Results
The statistical analysis was performed using the mean values obtained from independent experimental runs. For each hydrogen blending level (0%, 10%, and 20% H2), three independent experiments were conducted (n = 3), yielding a total sample size of nine observations for ANOVA. High-frequency measurements collected at 1 s intervals during each 30 min steady-state period were used solely to calculate representative run averages and associated variability and were not considered independent observations in the ANOVA procedure.
Prior to ANOVA application, the underlying assumptions were evaluated. The normality of residuals was assessed using the Shapiro–Wilk test, while homogeneity of variances was verified using Levene’s test. In all cases, no statistically significant violations were detected (
p > 0.05), confirming the suitability of parametric statistical analysis. The results of the ANOVA are summarized in
Table 10.
The analysis indicates that hydrogen blending has no statistically significant effect on thermal efficiency (F = 0.84, p = 0.46), which is consistent with the experimentally observed variation of less than ±0.2 percentage points across all test conditions. The corresponding effect size (η2 = 0.07) is small, further confirming that hydrogen addition does not meaningfully influence energy conversion efficiency under steady-state operation.
In contrast, a highly significant effect of hydrogen fraction on CO2 emissions was identified (F = 152.3, p < 0.001), with a very large effect size (η2 = 0.94). This result reflects the direct dependence of CO2 formation on the carbon content of the fuel and confirms that the observed emission reductions (202 to 161 kg/MWh) are primarily driven by fuel substitution rather than experimental variability. Post hoc comparisons using Tukey’s HSD test indicate that differences between all hydrogen blending levels are statistically significant.
Similarly, NOx emissions were found to be significantly affected by hydrogen blending (F = 48.7, p < 0.001), with a large effect size (η2 = 0.86). The increase from 40 to 52 mg/kWh is therefore statistically robust and can be attributed to elevated flame temperatures and enhanced thermal NOx formation mechanisms. Post hoc analysis confirms that the increase is statistically significant, particularly between 0% and 20% H2 conditions.
For CO emissions, no statistically significant effect was observed (F = 1.92, p = 0.21), and the associated effect size (η2 = 0.14) indicates only a minor influence of hydrogen blending. This is consistent with the stable and low measured values (6–7 mg/kWh), confirming complete combustion across all operating conditions.
Particulate matter emissions were below the detection limit of the measurement system in all experiments and were therefore not subjected to statistical analysis. This result further supports the conclusion that hydrogen– methane-based gas combustion does not promote particulate formation under the investigated conditions.
The performed statistical analysis confirmed that the observed trends in CO2 and NOx emissions are both statistically significant and practically meaningful, while variations in thermal efficiency and CO emissions remain statistically insignificant and within measurement uncertainty.