3.2. Biomass Liquefaction
The main reason for this study was to evaluate and perform the modelling of burnt pine heartwood specifically sourced from maritime pine wood after a forest fire in Leiria National Forest in 2017.
The liquefaction process was performed on burnt pine heartwood samples under different conditions to evaluate the influence of the wildfires on the yield of the process and modelling the liquefaction of burnt pine heartwood. The reaction lasted 30 to 180 min, under 120, 140, and 160 °C. The results are summarised in
Table 3, and the best conversion liquefaction achieved was 86.03% when the reaction occurred at 160 °C with a reaction time of 180 min, and the worst liquefaction yield value was 44.14% at 140 °C, 30 min of reaction time. In light of this information, burnt pine heartwood gave a good liquefaction yield under specific conditions.
The results show that the conversion is similar to the previous studies, in which pTSA was used as an acid catalyst [
5,
12,
13,
14,
18,
38]. On the other hand, pTSA has a lower crystallinity than commercially used mineral acids. The low percentage of crystallinity of residues when pTSA is used may result in better liquefaction of organic sulfonic acid pTSA than sulphuric and hydrochloric acid, for instance [
39]. Regarding the degradation reaction that occurs, it is known that cellulose degradation starts with glycosidic oxygen protonation, followed by carbonium ion formation and cleavage of the glycosidic bond. After the glycosidic bond is broken, cellulose depolymerisation can occur at both the reducing and non-reducing chain ends [
40].
It is possible to assume that higher temperatures gave a better conversion yield than in other trials. Experiments with a reaction temperature above 160 °C generally showed a conversion efficiency of over 80%, regardless of the reaction time. After the maximum conversion is achieved, a solid residue formation occurs, leading to an increase in the insoluble solid fraction. These solids are generally ascribed to the tar type and humin content and are associated with the recondensation reactions of degradation products, leading to a reduction in liquid fraction yields. However, the remaining biomass continues to liquefy for more extended reactions, increasing the yield [
29].
Low biomass conversions were observed at lower temperatures, such as 120 °C and 140 °C. The decomposition activation energy of the components, hemicellulose, cellulose, and lignin, of the feedstock is different, which is better understood when it is considered that lignin has the highest value, followed by cellulose and hemicellulose. It is necessary to consider the presence of crystalline cellulose, which can affect the process. The decomposition activation energy is higher for crystalline cellulose than its amorphous counterpart. At low temperatures, the energy of the reaction is insufficient to break down the crystalline structure of cellulose and the glycosidic bonds. Thus, this may remark that hemicellulose and amorphous cellulose are the only species that hydrolyse at low temperatures [
13].
In this study, the response surface method was applied to perform the optimisation. It is also a good way to show the relationship between different experimental variables and responses graphically. Using this procedure, it is possible to derive polynomial equations that show the effect of variables on the system’s response, which, in this case, is the liquefaction yield. MODDE 12.1 Pro® software was used to create an experimental matrix, and the Box–Behnken design was chosen.
First, the effects of three variables (T, cat, time), the second-order effects, the interactions between the two variables (T*cat), temperature and catalyst concentration were evaluated.
Figure 4 shows the coefficient plot of the model, as well as the correlation coefficient. The influence of each variable is a measure of the effect of its variation on the response. It can also be observed that the factor with the most significant influence on the conversion is temperature, while the catalyst concentration has a lower influence on the yield.
The obtained model offers a good correlation with the experimental data as R
2 = 0.988. This R
2 value indicates that 98.8% of the observations can be explained by the independent variables in the factor range, while the other 1.2% cannot be explained. The model shows a remarkable ability to predict new correct responses with a probability of 98.8%. The Q
2 value of 0.765, ideally >0.5, showed a high predictive power, allowing a confident estimation of the effect of changing process parameters and process optimisation. The model also showed a strong validity score, far exceeding the required value of 0.25. Similarly, the obtained value of 0.988 for reproducibility, which significantly exceeded the required value of 0.5, indicating good experimental control and low pure error [
41].
For further model validation, a mismatch plot and ANOVA were used to compare model error and pure error. The software claimed that no pure error is available for this obtained model.
The regression model equation was based on correlation coefficients and their effect on yield, as shown in
Table 4. Values were determined from the effect plot (
Figure 4). The positive or negative effect on the yield is considered significant if the confidence interval exceeds the origin, excluding insignificant effects from the model, giving the regression model equation:
where
Y1 corresponds to yield,
X1 to the catalyst concentration,
X2 to the reaction time, and
X3 to the temperature.
The derived regression model equation describes a complex process with linear and/or quadratic relationships for all parameters with liquefaction yield. The most important factor that has a linear effect on yield is the temperature (X3), followed by the reaction time (X2). As the concentration increases, there is a positive effect on the yield; but an increase in catalyst concentration and the reaction time leads to a decrease in the yield value. All three factors had a significant relationship with the change in the liquefaction yield.
The performance of the model described by Equation (7) for both calibration and validation sets is shown in
Figure 5. This plot shows that the calibration model developed for predicting burnt pine heartwood liquefaction has a great predictive ability, even for experiments carried out at different temperatures and catalyst concentrations.
The contour plot of the model is presented in
Figure 6, showing that temperature is the most important factor. However, the reaction time also acts in parallel with the conversion. In fact, conversions above 80% can be achieved using a low catalyst concentration (1%) as long as the temperature is applied at the highest level (160 °C) and the longest reaction time (180 min). In addition, when using a reaction time of 180 min and temperatures below 160 °C, the liquefaction conversion is always less than 85%, even when using the highest amount of catalyst (10%).
These experiments also showed that pine heartwood affected by wildfires could produce bio-oil without any impact on conversion rates, as other biomass liquefaction trials yielded similar conversions [
7,
18,
29]. Therefore, liquefaction may be an opportunity to recover and reclaim part of the biomass value lost during wildfires.
3.4. Fourier Transformed Infrared (FTIR-ATR) Analysis of Biomass, Bio-Oil and Solid Residue Samples
The FTIR-ATR spectra obtained from fresh biomass, solid and liquid samples as solid residue, and bio-oil product are shown in
Figure 7 and
Figure 8.
The characteristic bands corresponding to the related peaks are shown in
Table 6. According to the FTIR results, the bands in the range between 3600 and 3200 cm
−1 are referred to as O-H stretching bonds that can result from the presence of water or hydroxyl groups. The range in the region between 3000 and 2800 cm
−1 corresponds to the C-H stretching and the presence of the solvent, 2-EHEX. The signal is located in the range of 1730–1700 cm
−1, corresponding to the C=O carbonyl groups, and significates unconjugated ketone, ester, or carboxylic groups on aliphatic chains in liquefied biomass, which is related to the conversion of hemicellulose. Moreover, the C-O-H single bond, which is in the area between 1440 and 1395 cm
−1, may show aromatic carbohydrate derivates. The information also confirms the presence of the hydroxyl group by the peaks that are observed for bio-oil samples, with wavenumbers of 1036–1035 cm
−1 and 1118–1117 cm
−1. Furthermore, the peaks due to the C-O stretching of cellulose, between 1200 and 1000 cm
−1, show that the hydroxyl groups are removed from the solid fraction and transferred into the liquefied biomass. The bands between 950 and 850 cm
−1, expressing the C-H stretch decrease in solid residues compared to fresh biomass. However, liquefied biomass shows these bands as being as intense as fresh biomass, indicating that these bonds are transferred to the liquid fraction.
3.6. Thermogravimetric Analysis (TGA) of Biomass, Bio-Oil, and Solid Residue Samples
TG curves are shown in
Figure 10 and
Figure 11 to display the weight loss of biomass, solid residue, and bio-oil samples from the reaction with the best liquefaction yield with the temperature rise, and the specific mass loss of the liquid and solid samples to the related TG temperature ranges are listed in
Table 7.
For the biomass and solid residue samples, the first phase starts at 30 °C and ends at 220 °C. The mass loss at this stage is due to the removal of moisture and very volatile components. The second stage starts at 220 °C and ends at 360 °C, with a 53% mass loss for the biomass. This stage mostly indicates active pyrolysis due to the degradation of hemicellulose and cellulose. The third stage starts at 360 °C and ends at 590 °C, with a 24% mass loss. This step significates the active pyrolysis step, which is due to the degradation of cellulose. The thermal degradation behaviours of hemicellulose, cellulose, and lignin have been stated that the decomposition temperature ranges are 210–325, 310–400 and 160–900 °C, respectively [
48]. Although the above steps of active pyrolysis are mainly seen as a degradation of both hemicelluloses and cellulose, lignin is also degraded in this temperature range. At temperatures of 590 °C and above, the mass loss is very low due to slow degradation to produce charcoal as a residue. This step may be due to the degradation of lignin, called passive pyrolysis [
49].
Bio-oil samples consistently lost most of their mass at lower temperatures, which began to lose mass at 150 °C, slowing systematically at 360 °C. At temperatures below 150 °C, slight degradation has been observed, possibly due to the solvent still present in the bio-oil sample. The initial thermal temperature of thermal degradation was ~150 °C and corresponds to lighter derivatives. The second stage, between 220 and 360 °C, showed an average mass loss of ~46.5%, likely corresponding to the heavier components of the bio-oil.
The third step, between 360 and 590 °C, is attributed to the formation of non-degradable ash and carbon from the slow degradation of the sample. The DTG curves show that the bio-oil reduces its weight at an early stage and confirms the presence of lighter products such as aldehydes, alcohols, and carboxylic acids than its biomass counterparts [
50]. The volatile and small organic molecules can degrade in this stage; however, non-volatile macromolecular substances decompose between 375 and 550 °C due to thermal degradation of the bio-oil as a result of the pyrolysis phenomena [
51].