3.1. Thermal Decomposition of Different Origin Microwave Pre-Treated Biomass Blends
At the given configuration of the experimental device, the thermochemical conversion of biomass blends is governed by thermal decomposition/gasification of the biomass (1) promoting the yield of both condensable and non-condensable fractions of pellets. The main steps of thermal decomposition include biomass drying, the yield of volatiles, partial oxidation of combustible volatiles (2,3), char oxidation (4,5), and endothermic Boudouard, water vapor reactions (6,7):
In kinetic study of biomass blend thermal decomposition it is important to assess the contribution of each component in the process due to the different composition of blends. If the overall process is developing uniformly throughout the pellets, the weight loss of blend during the thermal decomposition can be approximately described using first-order reaction model [
31]:
where
is the mass conversion,
is the reaction rate constant,
is the original mass of the test sample,
is the mass of the test sample at time
,
is the final mass at the end of thermal decomposition,
is the activation energy,
is the temperature,
is the pre-exponential factor, and
is the universal gas constant.
A more detailed approach is to use models with distributed activation energy [
33,
34], where the thermal decomposition process can be described as many independent, parallel rate processes assuming them as irreversible first-order reactions. Considering the mass balance of species
i, reactions for volatile production read:
where
is the final quantity of volatile matter for the generic species,
, and
ki is the rate constant of the reaction expressed according to the Arrhenius law.
To successfully use this model, kinetic parameters of reactions (1–7) are necessary. Estimation of kinetic parameters from experimental data of biomass thermochemical conversion practically is not possible and data from the literature are necessary.
In a recent study, the weight loss rate and the yield of volatiles were studied and compared using the most widely available bioenergy resources in Latvia (wood, agriculture residues, and peat) and producing the selectively activated blends of commercially available pellets (straw* + straw, straw* + wood, straw* + peat, wood* + straw, wood* + peat) (
Figure 3a–e).
Results of kinetic studies of the weight loss of blends during their thermal decomposition/gasification have shown that for all blends MW pre-treatment of pellets has a significant role on the kinetics of the weight loss rate. In
Figure 3 it has been shown that even a relatively small mass fraction of pre-treated pellets in the blend (30%) can vary the weight loss rate.
Comparing average values of the weight loss rate of biomass blends of different MW pre-treatment temperatures and different mass fraction of pellets (
Figure 4), it can be concluded that MW pre-treatment of pellets promotes a higher weight loss rate and devolatilization of the blend than predicted using a simple additivity approach (13) [
25]. Such deviation from purely linear behavior suggests synergy mechanism between pre-treated and raw biomass pellets in the blends.
where:
, g/s—weight loss rate of the blend,
, g/s—weight loss rate of MW pre-treated wheat straw or wood pellets,
, g/s—weight loss rate of raw peat pellets,
—mass fraction of pre-treated pellets, and
—mass fraction of raw pellets in the blend.
The results in
Figure 4 allow to conclude that for the most of selectively activated blends a positive synergistic effect on the weight loss rates is achieved. However, a slightly negative synergistic effect is observed for the blend of raw wood with pre-treated wheat straw pellets.
Comparing the effect of changes in MW pre-treatment temperature of pellets on the kinetics of the weight loss rate of blends it can be concluded that they are significantly different (
Figure 3a–e) and can be related to both-diversity of the main characteristics of the blend components (
Table 1,
Figure 1) and MW-induced structural changes. It leads to variations of combustible volatile yield and a balance between the rates of reactions (1–7), which is confirmed by measurements of combustible volatiles yields at the outlet of the gasification reactor (
Figure 5a–f) and supported with measured yields of CO
2 and CO for the different MW pre-treatment temperatures in studied biomass blends (
Figure 6a–e).
Providing analysis of the main processes, which promote changes in the weight loss rates of the blends and the yield of volatiles during thermal decomposition/gasification of selectively MW pre-treated blends, it should be noticed that MW-induced structural changes with increased reactivity of pellets and changes in elemental composition with carbonization [
23,
24] of pellets enhance the development of gasification reaction (4), increasing the weight loss rate of blends, the yield of CO and the temperature in gasification zone. Increasing the temperature in the gasification zone enhances endothermic drying in raw biomass, thus promoting the yield of H
2O and additional weight loss in the blend defined by the moisture content and mass fraction of raw pellets in the blend.
Drying is followed by the enhanced thermal decomposition of blend components by increasing of the yields of volatiles (CO
2, CO, and H
2) and the weight loss. In accordance with data [
35], polymer-like hemicelluloses decompose, increasing the temperature to 540–560 K and promoting the enhanced yield of CO
2, cellulose decomposes at temperatures above 580–600 K with the enhanced yield of CO, while lignin decomposes at temperatures between 430–1100 K with the enhanced yield of H
2. The enhanced yields of H
2O and CO
2 during drying and thermal decomposition of hemicelluloses are the main factors, which promote an endothermic carbon and water steam reaction (7) increasing yields of CO and H
2 as well as the Boudouard reaction (6), which has high importance in the process of biomass gasification [
19]. These reactions are responsible for the additional yield of CO and the weight loss of the blends.
This is confirmed by analyzing results of the FTIR measurements (
Figure 7), where the yields of CO
2 and CO at different stages of thermal decomposition selectively pre-treated blends are shown. Two major stages can be distinguished. In the primary stage (e.g.,
Figure 7a, t < 1200 s and
Figure 7b, t < 2000) enhanced gasification promotes correlating increase in yields of CO and CO
2. In the second or end stage (e.g.,
Figure 7a, t > 1200 s and
Figure 7b, t > 2000) the char conversion occurs and development of the Boudouard reaction promotes an increase in the CO yield with correlating decrease in the CO
2 yield.
The balance between the exothermic gasification of biomass blend (4) and endothermic processes (6, 7) changes the weight loss rates of the blends (
Figure 3a–e) and the average values of the yields of volatiles (
Figure 5 and
Figure 6a–e) depending on pre-treatment conditions and composition of blends, thus varying the thermal and chemical interaction between the components and synergistic effects of interactions (
Figure 4).
In cases of a positive synergetic effect, e.g., when pre-treated wheat straw pellets are co-fired with raw straw, wood, or peat pellets, the exothermal gasification of pre-treated pellets acts as a heat source, enhancing drying and thermal decomposition of raw pellets. It leads to a faster weight loss of the blend (
Figure 3a) and the yield CO
2 and by varying relation between the yields of CO
2 and CO. In case of low pre-treatment temperature of wheat straw pellets (T = 473 K) the balance between exothermic and endothermic reactions (1, 4, 6, 7) is achieved, when the mass fraction of pre-treated straw pellets in the blend reaches 30% which leads to increase in CO
2 yield to the maximum value and limits the yield of CO. As follows from
Figure 5a and
Figure 6a, the yield of CO
2 tends to decrease with the pre-treated wheat straw pellets increase in the blend above 30–45%. It is caused by the heat release during exothermal gasification of the pellets (4) exceeding the amount of heat required to induce endothermic reactions (6, 7). As a result, the rate of reactions (6, 7) tends to increase, increasing the yields of combustible volatiles (CO, H
2) while decreasing the relation between the yields of CO
2 and CO.
The more effective increase in the yield of combustible volatiles (CO, H
2) up to the maximum value with correlating decrease to minimum value the yield of CO
2 is observed by increasing the pre-treatment temperature to T = 548 K (
Figure 5a and
Figure 6a). It leads to an increase in the reactivity of pre-treated pellets and heat release during gasification of pre-treated pellets (4), thus enhancing the development of reactions (6, 7), responsible for the enhanced yield of combustible volatiles (CO, H
2).
For the blend of raw wood pellets with pre-treated wheat straw pellets replacing a part of raw wood with pre-treated additives of wheat straw pellets results in changes in the heating value of the blend and contents of hemicelluloses, cellulose, and lignin in the blend, increasing content of hemicellulose, responsible for the higher yield of CO
2, while decreasing contents of cellulose and lignin in the blend, responsible for the yields of CO and H
2. Like changes in the yield of CO
2 for the blends of pre-treated wheat straw with raw wheat straw pellets, at low temperature pre-treatment of wheat straw pellets (T = 473 K) the balance between endothermic and exothermic reactions is achieved when the mass fraction of pre-treated straw pellets in the blend with raw wood pellets increases and reaches 30–45%, increasing up to the maximum value the yield of CO
2, while limiting the yields of CO and H
2. The more effective the increase in the yields of combustible volatiles (CO, H
2) up to the maximum value with a correlating decrease to the minimum value of the yield of CO
2 can be achieved by increasing the pre-treatment temperature to T = 548 K (
Figure 5 and
Figure 6), when increasing reactivity of pre-treated pellets, which enhances gasification of the blend (4) and correlates with enhanced development of endothermic reactions (6, 7). During the thermal decomposition of pre-treated wheat straw blend with raw wood pellets a difference in chemical composition of lignocellulosic wood and wheat straw pellets influences the synergetic effect of interaction on the weight loss and the yields of combustible volatiles. According to [
22], the thermo-chemical conversion of biomass decomposition of cellulose leads to a positive synergetic effect, whereas decomposition of hemicellulose and lignin can result in both positive and negative synergistic effects depending on the blend composition and temperature. A similar trend is observed when only partially (15%) adding pre-treated wheat straw to raw wood pellets (
Figure 4).
A faster thermal decomposition of the blends (
Figure 3c) with a positive synergetic effect (
Figure 4) is also observed when mixing pre-treated wheat straw with raw peat pellets. Pre-treated pellets promote the evident changes in chemical composition of the blend, increasing contents of hemicellulose, cellulose, and lignin in the blend compared to raw peat pellets. A low pre-treatment (T = 473 K) temperature of wheat straw enhanced the reactivity of the pellets, promoting faster thermal decomposition of the blend and increasing the heat release during the blend gasification. In addition, increasing the content of hemicelluloses in the blend enhances the yield of CO
2, increasing to a maximum value the ratio of CO
2/CO. Thus, the balance between the reactions (1, 4, 6, 7) at low mass fraction of pre-treated wheat straw (15%) is achieved. Increasing the pre-treatment temperature to 548 K of wheat straw pellets enhanced carbonization and HHV leads to an enhanced gasification of the blend with correlating decrease in the relation CO
2/CO, which suggests the development of endothermic reactions (6, 7).
Faster decomposition of the blends (
Figure 4d,e) with a positive synergetic effect is observed also during the thermal decomposition of pre-treated wood with raw wheat straw and peat pellets (
Figure 3). Replacing raw straw or peat with pre-treated wood pellets promotes changes in chemical composition of blends and HHV of the blends. Analogous to pre-treated wheat straw blends, the most pronounced increase in the positive synergetic effect is observed for the blend of pre-treated wood pellets with peat. In this case, additives of pre-treated wood pellets promote an increase in hemicelluloses in the blend, thus enhancing volatilization of the blend and development of endothermic processes (6, 7) responsible for the enhanced yields of CO and H
2, and decreasing the relation between the yields of CO
2 and CO (
Figure 5d,e and
Figure 6d,e).
3.2. Thermochemical Conversion of Microwave Pre-Treated Biomass Blends of Different Origin
MW-induced changes in thermal decomposition/gasification of pre-treated pellets are responsible for thermochemical conversion of fuel blends, including processes of flaming combustion of volatiles, char conversion, and heat energy production (2–5). At the given pilot device configuration (
Figure 2) the development of combustion dynamics at biomass thermochemical conversion is influenced by mixing of the axial flow of volatiles with secondary air swirl determining the formation of typical flame temperature and flow velocity profiles close to the inlet of the combustor [
36]. Experimental temperature and velocity profiles of raw straw combustion at height L/D = 1.5 are compared with numerically calculated results using 2D axisymmetric model [
37] and presented in
Figure 8.
In
Figure 8a temperature profiles indicate higher flame temperature in the central part of the cylindrical reactor, then decreasing closer to the outer wall. While profiles qualitatively agree, the estimated temperature by numerical model is higher in the central part, but lower in the near-wall region, while the average temperature is similar in both cases. In
Figure 8b, tangential velocity profiles are compared. Moreover, in this case qualitative agreement is obtained. Order of magnitude of tangential velocity is c.a. 1 m/s closer to the wall. The biggest differences of experimental and numerical results are found in the central part, where the numerical model predicts the gradual decay of tangential velocity towards the symmetry axis.
In
Figure 8c, the largest differences from the numerical to experimental results are observed. It should be noted that in zone r/R = 0.6…0.8 it was not possible to measure negative axial velocities that are caused by recirculation of flow. First, numerical results predict negative axial flow near the wall, but in the experiment a strong positive flow is observed. In both cases, positive velocity is observed in the central part of reactor; however, the numerical model significantly overestimates it. It should be noted that the numerically obtained axial velocity profile corelates with the temperature profile. It suggests that the experimentally observed positive axial velocity in the near wall could contribute to the smaller temperature gradient from the center to near wall region.
The differences of the current numerical model compared to the experimental data in
Figure 8 suggests that a higher order reaction model could be necessary to model the process more precisely. Moreover, the influence of the 2D axi-symmetric geometry could contribute to differences of velocity distribution. Due to the transient nature of the process, a time-dependent study should be also considered. Further development of the numerical model is ongoing to obtain better agreement between experimental and numerical results.
The kinetics of the flame temperature as well the total amount of produced heat power (
Figure 9a–e) correlate with kinetics of the weight loss rate of blends shown in (
Figure 3a–e). The analysis of such a correlation suggests that MW pre-treated additives enhance the axial flow of combustible volatiles, thus promoting faster ignition and transition to self-sustaining combustion conditions. In addition, the radiative heat transfer from the reaction zone, which supports the thermal decomposition of blends, is responsible for the formation of the interrelated processes of thermal decomposition and thermochemical conversion of the blends.
As follows from
Figure 9a–e, the kinetics of the heat production is importantly dependent on the chemical and elemental composition of the blend components, the changes in which depend on the MW pre-treatment temperature and mass fraction of pre-treated pellets in the blends. It leads to variation in the rate of the main reactions (1–7) developing during the thermochemical conversion of the blends. Comparing kinetic profiles of the thermal decomposition and heat power during thermochemical conversion of the selectively MW pre-treated blends, one can see that the more pronounced changes in produced heat power with faster and higher heat production can be obtained, when the MW pre-treated wheat straw or wood pellets are blended with raw peat (
Figure 9c,e), since additives of pre-treated wheat straw enhance devolatilization of raw peat pellets.
As follows from
Figure 5a,b, the average yield of the combustible volatiles importantly depend on blend components, thus producing different flux of combustible volatiles in the inlet of the reactor. At constant primary and secondary air supply rates in the device the changes in the axial flow of combustible volatiles correlate with changes in the air to fuel supply by varying the average value of the air excess ratio at the inlet of the combustor, combustion conditions in the reaction zone, and burnout of volatiles. As follows from
Figure 10a–c, the air excess ratio at the inlet of the combustor tends to decrease with the increase in the fraction of pre-treated pellets leading to nearly stoichiometric combustion conditions. As a result, the average values of the flame temperature increase up to the maximum value and tend to decrease with the increase in the mass fraction of pre-treated pellets in the blend and the heat output from the device. In addition, the dependence of the flame temperature and produced heat on the mass fraction of pre-treated pellets confirm the presence of synergistic effects of interaction between the components.
It should be noted that at the fixed distance from the inlet of the reactor (L/D = 3) a higher average value of the flame temperature with a lower amount of produced heat is observed pre-treated wheat straw with raw wheat straw pellets blends (
Figure 10b,c), when flaming combustion of volatiles produced during thermal decomposition of hemicelluloses dominates. The average flame temperature tends to decrease with the increase in the average value of produced heat and heat loss from the flame reaction zone.
The lower the value of average temperature, the higher the value of the produced heat observed for blends of pre-treated wood with peat. This suggests that increasing the fraction and MW pre-treatment temperature of pre-treated wood pellets in the blend enhances transition from flaming combustion to char conversion, which can be related to the increase in the fixed carbon content and HHV (
Figure 1). As a result, the flame length and measured flame temperature decreases.
The MW-induced changes in the thermochemical conversion of blends influence the total amount of produced heat energy in the device (
Figure 11a–f), which is predominately determined by the MW-induced changes in the balance between the reactions (1–7) during thermal decomposition of the blends, changes in the yield of combustible volatiles pellets, and relation between the yields of CO
2 and CO (
Figure 5 and
Figure 6a–e). As follows from
Figure 11a–f, the total amount of produced heat energy predominately tends to increase with the pre-treatment temperature and the mass fraction of MW pre-treated additives in the blends up to 30–45%. This suggests of MW pre-treated additives can be used to complete thermochemical conversion of the blends. A slight decrease in produced heat is observed at low MW pre-treatment temperature (T = 473 K), when the relatively low HHV, reactivity of pre-treated pellets [
23], and intensive endothermic drying of raw pellets are limiting factors for the yield of combustible volatiles (
Figure 5a–f) and thermochemical conversion.
3.3. The Composition of Emissions of Blends with MW Pre-Treated Biomass Pellets
As discussed above, the yield of combustible volatiles and CO
2 depend on the diversity of carbon contents in pellets and MW-induced changes, varying structure of pellets and their reactivity rate of reactions (1–7). Additionally, the formation of carbon-neutral CO
2 emissions during thermochemical conversion of the blends depends on the inlet conditions of the reactor, the burnout of volatiles (2, 3), and the temperature of the reaction zone. As follows from
Figure 12, for all blends, increasing the mass fraction of pre-treated additives in the blend and pre-treatment temperature correlates with an increase in the volume fraction of CO
2 in the products, confirming that MW pre-treated additives enhance thermochemical conversion of the blends. By analogy with the MW-induced changes in the yield of combustible volatiles (
Figure 5 and
Figure 6), the most effective increase in the CO
2 volume fraction in the products can be obtained for the blend of pre-treated pellets with peat (
Figure 12). The less effective increase in CO
2 for the blend of pre-treated straw with wood, the thermochemical conversion of which enhances flaming combustion of volatiles, produced the higher average amount of heat downstream of the combustor (
Figure 11).
The diversity of elemental composition of pellets with difference of nitrogen contents in raw pellets (
Table 1) and their changes during MW pre-treatment (
Figure 1), as well as MW-induced changes in the inlet conditions and the flame temperature, also influence the formation of NO
x emissions, primarily in the form of NO. In the combustion of biomass blends there are two main mechanisms of NO formation—thermal NO and fuel NO. According to the Zeldovich mechanism [
38], intensive production of thermal NO
x occurs at temperatures above 1500 K and are more pronounced when the mixture is on the fuel-lean side. At temperatures below 1000 K, the formation of thermal NO is limited and can be neglected. Fuel NO
x results from oxidation of nitrogen contained in biomass [
39].
During the combustion of biomass blends, the oxidation of fuel-bound nitrogen is the dominant mechanism of forming NO
x and depends on the nitrogen and oxygen content in the blend components (
Figure 13). As follows from the
Figure 13a, the blending of pre-treated wheat straw with raw wheat straw or wood pellets promotes an increase in nitrogen content in blends, while blending pre-treated wheat straw with raw peat pellets leads to the nitrogen content decrease. A similar decrease in the nitrogen content in the blend is observed for the blends of pre-treated wood with raw wheat straw of peat pellets. Comparing changes in nitrogen contents in blends with changes in the yields of NO
x suggest (
Figure 13b) that the formation of NO
x emissions at the thermochemical conversion of the blends is slightly influenced by the synergistic effects on NO
x formation and the mass fraction of NO
x emissions in the products cannot be approximated with linear dependence on the mass fraction of pre-treated pellets in the blend, assuming the development of interactions, which can influence the NO
x formation and require additional research.