4.1. Characteristic temperature analysis
Each coal sample's weight loss reflects the difficulty that it was to burn, and the coal sample's weight loss is directly proportional to the coal's complete combustion. The larger the weight loss, the easier it is for the coal sample to burn completely. Similarly, it can be seen that the weight gain related to oxygen uptake is also proportional to the adsorption capacity of coal samples.
Figure 2 and
Figure 3 displayed the TG and DTG curves from the experiment.
Figure 2 and
Figure 3 showed the curve variations of the various experimental coal samples throughout oxidation heating process. The range of temperatures that corresponds to each of its four oxidation process: The weight loss stage is T
1–T
2. The weight gain stage is T
2–T
3. The pyrolysis stage is T
3–T
4. The combustion stage is T
4-T
6.0
Low-temperature oxidation of the coal sample took place under the thermogravimetric analyzer's temperature program. While the coal sample's water gradually evaporated, it adsorbed O2 and released CO, CO2 and other gases. At the beginning, the coal sample's evaporation rate of water was far greater than the rate of O2 adsorption. So, The rate of weight loss in the coal sample kept increasing. When the critical temperature T1 was reached, the rate of weight loss in the coal sample was peaked. The T1 corresponded to the DTG curve's initial peak position, which was also the first temperature point at the velocity of the coal oxygen composite reaction increased. The rate that coal sample's oxygen adsorptive capacity increases with temperature, the thermal weight loss rate of coal sample slowly decreased. When the water evaporation rate of coal sample itself and the oxygen adsorption rate of coal sample reached dynamic equilibrium, the coal sample's rate of thermal weight loss was 0. At this time, the coal sample's water essentially evaporated as the dry cracking temperature T2 was reached. When the dry cracking temperature T2 was reached, some active groups started to react with O2 to generate oxygen containing intermediates which were stored in the coal sample, and he quality started to increase. When the temperature reached the thermal decomposition temperature T3, the coal's weight gain rate due to oxygen absorption and its own reaction consumption rate reached dynamic equilibrium. The coal sample's thermal weight loss rate again became 0, and its mass growth rate maximized, indicating the end of weight gain stage. After reaching the pyrolysis temperature T3, the coal sample was oxidized and decomposed, resulting in a significant reduction in quality. The internal energy of coal molecules increased as the temperature kept rising, leading to the thermal decomposition of the circular structure inside the coal molecules. The coal sample's quality continued to decrease, and after reaching ignition temperature T4, the coal sample started to burn. After exceeding T4, the coal sample had a violent oxidation reaction, resulting in a significant quantity of gas being released and the primary coal molecules' backbone structure being disrupted, which quickly reduced the coal sample's quality. After reaching the temperature T5, the coal sample's thermal weight loss rate reached its maximum value. The maximum pyrolysis rate temperature T5 on the DTG curve corresponded to lowest point. Now, the heated oxidation chemical decomposition reaction was the most intense, generating CO, CO2, H2O and other trace gases. The active ingredient in the coal was basically consumed, and the coal combustion rate gradually decreased after this point. Until reaching the burnout temperature T6, The coal sample's quality tended to stabilize and no longer changes. The TG-DTG curve inclined to a stable value at the T6, indicating that coal's oxidation and decomposition process had basically over.
Figure 4 showed the characteristic temperature changes of various coal samples before and after inhibition during the thermogravimetric experiment. After the coal samples were treated with hydrated phase change materials, their critical temperatures (T
1) increased. Lower coal spontaneous combustion grade and lower coal body spontaneous combustion capacity were associated with higher critical temperatures. At low temperatures, hydrated phase change materials exhibited the most effective inhibitory effect on coal spontaneous combustion at temperatures ranging from 60℃ to 90℃. This was because at temperatures ranging from 60℃ to 90℃, hydrated phase change materials underwent phase change when heated to the critical temperature point of phase change, which maximized heat absorption and reduced the rate at which coal's temperature increased, while also isolating oxygen from the coal, resulting in the prevention of coal spontaneous combustion. The inhibited lean coal sample and coal inhibited meager sample had higher thermal decomposition temperatures T
3 and dry cracking temperatures T
2 than the raw coal. The inhibited gas coal sample's the temperature of maximum thermal weight loss rate T
5,the burnout temperature T
6, and T
2 were all higher than the raw coal. The T
2, ignition temperature T
4 and T
5 of the inhibited long flame coal sample were higher than that of the raw coal, indicating that the hydrated phase change material mainly acted on the stages of water loss, weight loss, oxygen absorption and weight gain of the meagre coal and lean coal. It also acted on the stages of water loss, weight loss and combustion stage of gas coal and the stage of water loss, weight loss and pyrolysis of long flame coal.
The characteristic temperature points after inhibition were relatively lagging when coal samples before and after inhibition were examined. Among them, the deviation of critical temperature and ignition point temperature was the largest, indicating that hydrated phase change materials had the optimal result during the low-temperature phase of the self-heating oxidation process. The inhibited coal sample's mass loss was 1.6%–9.3% less than that of raw coal, and the rate of oxidation was slowed down.
Figure 5 showed the weight loss rate and its reduction ratio in the thermogravimetric experiment before and after inhibition of various coal samples. The calculation formula of weight loss rate decrease ratio is shown in Eq.(1):
Where, is the weight loss reduction ratio,%. is the weight loss rate before inhibition,%. is the weight loss rate after inhibition, %.
According to the characteristic temperature and weight loss rate before and after coal sample inhibition, the hydrated phase change materials can considerably reduce the weight loss rate of gas coal and long flame coal, making them more appropriate for these types of coal.
4.2. Combustion characteristic parameter analysis
The parameters that describe the properties of coal combustion during combustion are called combustion characteristic parameters, such as combustion intensity, combustion difficulty, combustion rate, ignition performance, and burnout performance. Typically, they are used to reflect the coal's combustion state. The combustion characteristic parameters mainly include the flammability index and the comprehensive combustion characteristic index. Currently, they are also used for studying on the mixed substances, flame-retardant materials and non-coal materials during combustion.
The combustion intensity and difficulty of flammable materials are frequently assessed using the flammability index.reflecting their combustion rate, combustion performance, etc. The flammability index is a key indicator that determines the combustible material performance in terms of ignition and combustion. Better ignition stability and combustion performance of flammable materials are indicated by higher flammability index values. The flammability index of the performance testing experiment in this article can be calculated from the maximum combustion rate and ignition temperature. As shown in Eq.(2), the flammability index is directly inversely proportional to the square of the sample ignition point temperature and proportional to the sample's maximum combustion rate.
Where,
C is the flammability index,%•min
-1•K
-2.
is the maximum mass loss rate, %/min.
is the ignition temperature, K.
When assessing the combustible materials' ability to ignite, the comprehensive combustion characteristic index is frequently employed, reflecting the quality of their combustion performance [
29]. According to Eq.(3), the sample's comprehensive combustion performance improves with a bigger the comprehensive combustion characteristic index value.
Where,
S is the comprehensive combustion characteristic index,%•min
-1•K
-3.
is the average combustion rate,%/min.
is the burnout temperature, K.
The combustion characteristic parameters obtained through calculation were shown in
Table 2.The flammability index of meagre coal sample and lean coal sample added with hydrated phase change materials significantly decreased compared to the raw coal sample, but the comprehensive combustion characteristic index increased when compared to the raw coal sample. In comparison to the raw coal sample, both the average combustion rate and the maximum mass loss rate increased. When compared to the raw coal sample, the inhibitory gas coal sample and the inhibitory long flame coal sample displayed lower comprehensive combustion characteristic index, lower maximum mass loss rate, higher average combustion rate, and higher flammability index. The comprehensive combustion characteristic index of gas coal and long flame coal, as well as the flammability index of meagre coal and lean coal, can all be lowered by adding hydrated phase change materials. Meanwhile, the maximum mass loss rate of long flame coal and gas coal can be decreased by adding hydrated phase change materials.
4.3. Reaction activation energy analysis
In atmospheric environment, coal will undergo oxidation and spontaneous combustion reaction with air, which is usually called gas-solid reaction. There are various phases to the coal spontaneous combustion, and many small elements are involved in the reaction at each level. During the reaction process, a certain activation energy is required to overcome the corresponding energy barriers and transform into activated molecules. According to calculation and analysis, the activation energy and the spontaneous combustion tendency of coal are related under certain conditions, and there is an inverse ratio between the two.
Based on the above research on Thermogravimetric analysis method, we can study and analyze the coal body's chemical process under conditions of temperature change or isothermal oxidation kinetics of solid materials. To resolve the reaction's activation energy, this experiment uses Coats Redfern integration method to process the thermogravimetric curve [
30], and its oxidation reaction kinetics equation is expressed as:
Where,
is the heating rate.
T is the thermodynamic temperature, K.
is the mechanism function describing the spontaneous combustion reaction of coal.
is the reaction rate constant.
is the conversion rate of coal at time t, as shown in Eq.(5):
Where,
is the coal's initial weight ,mg.
is the weight at time t, mg.
is the final weight , mg.
Arrhenius proposed that the rate constant and temperature have the following relationship:
Where,
E is the activation energy, kJmol
-1.
A is the pre-exponential factor.
R is the gas molar constant, 8.314J/(mol·K).
Eq.(7) is obtained by combining Eq.(4) and Eq.(6).
Due to the low temperature at the beginning of the reaction, the reaction rate can be ignored. By integrating Eq.( 7), Eq.(8)can be obtained:
Eq.(9) can be obtained by combining the Eq.(8) and the Coats-Redfern equation:
Where,
is the integral function of the reaction mechanism of coal oxidation process, that is, the original function of
.
For the majority of E and the general response temperature range of coal samples,
is much smaller than 1,
.Therefore, Eq.(9) can be changed to Eq.(10):
The general coal oxidation reaction is generally a first order reaction, and the integral function of the reaction mechanism is usually
.Therefore, the coal oxidation reaction function obtained in this experiment is shown in Eq.(11):
Set
and
are plotted as a function graph, and the slope on the graph is
. The activating energy can be obtained by calculation. The intercept on the graph is
, which can be calculated to the pre-exponential factor.
Figure 6 and
Figure 7 showed the correlation analysis of oxidation reactions before and after inhibition in coal samples with four varying intensities of metamorphism.
There was a good association between the oxidation reactions of the four coal samples prior to and following inhibition, with correlation coefficients greater than 0.9, indicating that the coal oxidation reaction was well-fitted by this function. As shown in
Table 3, pre-exponential factor and activating energy can be obtained by fitting equations.
Table 3 showed the inhibitory coal samples of meagre coal, lean coal, gas coal, and long flame coal had higher activating energy than their raw coal samples, with increases of 1.138 KJmol
-1, 23.048 KJmol
-1, 5.23 KJmol
-1, and 5.673 KJmol
-1, respectively. The activating energy of coal sample is a parameter that measures the spontaneous combustion characteristics, which has an inverse relationship with the tendency of coal to spontaneous combustion. Therefore, hydrated phase change materials can reduce the possibility of coal spontaneous combustion. The pre-exponential factor reflects the possibility of collision between activated groups in coal oxidation processes. The bigger the value of pre-exponential factor, the bigger the possibility of collision between activated groups. The pre exponential factors after inhibition were greater than those before inhibition, as shown in
Table 3. However, based on the changes in each coal sample's activating energy before and after inhibition, it can be inferred that the increase in pre exponential factor had less impact on coal oxidation reaction than the increase in activating energy.
In summary, hydrated phase change materials had an inhibitory effect on the coal spontaneous combustion effect, which can increase the activating energy of coal and cause the oxidation and combustion process of coal to move backwards.