Open Access Article
Wentao Denga,
Yun Chao*ab,
Qian Li
*a,
Bin Chen
b,
Zhigang Liubc,
Huiming Chenbd,
Lei Yie and
Chuanli Liuc
aSchool of Energy and Mechanical Engineering, Jiangxi University of Science and Technology, Nanchang 330013, China. E-mail: chaoyun2001_09@126.com; wuli198679@163.com
bState Key Laboratory of Multiphase Flow in Power Engineering (SKLMF), Xi'an Jiaotong University, Xi'an 710049, China
cInternational Institute for Innovation, Jiangxi University of Science and Technology, Nanchang 330013, China
dSchool of Mechanical and Electrical Engineering, Jiangxi University of Science and Technology, Ganzhou 341000, China
eJiangxi Provincial Key Laboratory of Particle Technology, Jiangxi University of Science and Technology, Ganzhou 341000, China
First published on 1st June 2026
Waste wool, a protein-based waste from textile and livestock industries, represents a promising yet underexplored feedstock for clean hydrogen production. In supercritical water, its keratin structure undergoes rapid hydrolysis and depolymerization, enabling efficient conversion into hydrogen-rich gas with minimal char formation. In this study, a systematic investigation of wool SCWG was conducted by evaluating the effects of temperature, feedstock concentration, residence time, and catalyst addition. Compared with conventional biomass feedstocks, the unique protein structure of wool leads to distinct gasification behavior and high hydrogen production potential. Higher temperature, lower feedstock concentration, and moderately long residence time significantly enhance carbon conversion and gas yield. Under optimal conditions (600 °C, 2 wt% feedstock concentration, and 5 min residence time), carbon conversion efficiency reached 95.71%, hydrogen efficiency reached 119.26%, and gas yield reached 42.72 mol kg−1. Furthermore, the addition of Cu-3% Al2O3 catalyst significantly improves hydrogen production and gasification efficiency, highlighting the synergistic role of catalytic effects and feedstock characteristics. These findings provide new insights into the gasification behavior of protein-rich biomass and demonstrate that supercritical water gasification is a promising and efficient pathway for converting waste wool into clean hydrogen energy.
As the only renewable carbon-based resource, biomass is regarded as a key feedstock for green hydrogen production. Biomass gasification for hydrogen production can achieve a carbon – neutral cycle to a certain extent, but biomass has high volatile content and low energy density under conventional gasification or steam reforming conditions. It easily generates tar and coke during the conversion process, which impairs the quality of the product gas and increases the operational complexity of the system.11–14 High-temperature steam reforming further aggravates the formation of coke and polycyclic aromatic hydrocarbons (PAHs), which severely limit hydrogen yield and reaction stability.15,16 To reduce byproduct formation and improve hydrogen production performance, researchers have developed various catalyst systems, including alkali metals, alkaline earth metals, and nickel-based catalysts, and these systems have brought about partial improvements in hydrogen yield and tar conversion efficiency.17–20 For example, Zhang et al.21 used LAO and LSAO-supported nickel catalysts in toluene steam reforming, raising the hydrogen yield to 78.18%; Kuchonthara et al.22 added K2CO3/NiO/γ-Al2O3 during the steam reforming of rice husk – derived tar, cutting the tar yield. from 36.2% to 28.9% while increasing the hydrogen yield from 24.1% to 33.5%; Luo et al.23 added CaO to the steam gasification of pine sawdust, achieving a 2.39-fold increase in hydrogen yield and a 16% reduction in tar yield. Even so, catalytic gasification still faces challenges such as catalyst deactivation, carbon deposition, and complex reaction pathways, which means the core problem of tar formation has not been fundamentally solved.
Supercritical water, defined as water above 374.3 °C and 22.1 MPa, exhibits unique physicochemical properties such as high diffusivity, low dielectric constant, and enhanced mass transfer capability.24,25 Supercritical water decreases the polarity of water and thus enhances solubility of organic compounds while the higher ion product promotes radical and ionic reactions.26,27 Biomass is rapidly hydrolyzed, pyrolyzed and reformed in homogeneous state, which inhibits formation of phenolics and tar and allows efficient and clean gasification. Recently, SCWG has been applied to various biomass feedstocks such as agricultural and forest waste, food waste, sewage sludge and oily waste.28–31 The main parameters that influence hydrogen production are reaction temperature, feed concentration, residence time, and catalyst type. Different feedstocks have different hydrogen yields under optimal conditions.32–35 For instance: Su et al.34 reported a hydrogen yield of 1.74 mol kg−1 from food waste at a concentration of 5 wt%, a temperature of 450 °C and a residence time of 20 min; Nanda et al.36 achieved a hydrogen yield of 3.37 mol kg−1 from fructose at 4 wt%, 700 °C and 1 min, and fructose is a model compound for fruit and vegetable waste. In addition, catalysts, especially noble metal and nickel-based catalyst systems, can improve hydrogen yield and selectivity.37–41 Borges et al.37 found that using NiFe2O4 in the gasification of eucalyptus sawdust increased the hydrogen content by 60%, while Huang et al.38 demonstrated that nickel nanoparticles can enhance the hydrogen yield from glucose gasification. Overall, SCWG has the advantages of high gasification efficiency, minimal coking, and high-quality product gas, which makes it highly suitable for processing complex biomass feedstock systems.
Notably, most fundamental studies on SCWG have been conducted in batch-type reactors, which provide a closed and well-controlled reaction environment. In such systems, the gradual heating process and relatively long effective residence time enable prolonged interaction between intermediates and supercritical water, thereby promoting secondary reactions such as steam reforming and water–gas shift. As a result, hydrogen yields in batch SCWG systems typically fall within the range of 1–5 mol kg−1 for carbohydrate-based feedstocks under comparable conditions, whereas significantly higher hydrogen production can be achieved for protein-rich feedstocks due to their distinct chemical composition and enhanced participation of water in hydrogen generation.42 Therefore, batch reactors are widely regarded as an appropriate platform for investigating intrinsic reaction mechanisms and gasification behavior of complex biomass.
Wool is one of the most abundant protein-based waste materials generated from the textile and livestock industries and has attracted increasing attention due to its high keratin content.43,44 Global annual wool production exceeds 1–2 million tons; however, less than 10% of waste wool is effectively recycled, with most being discarded or converted into low-value products.41,45 In China, large quantities of waste wool are generated every year, while the effective recycling rate remains relatively low.46 The accumulation and improper disposal of waste wool may lead to environmental concerns and resource waste.As a protein-rich biomass, wool keratin contains abundant peptide bonds and heteroatoms, making it a potentially valuable feedstock for hydrogen-rich gas production. Compared with conventional thermochemical processes such as pyrolysis and dry gasification, supercritical water gasification (SCWG) is more suitable for treating wet and nitrogen-containing biomass without the need for energy-intensive drying. Therefore, the utilization of waste wool through SCWG provides a promising pathway for resource recovery, clean hydrogen production, and high-value utilization of protein-based waste biomass.47,48
Compared with other protein-rich biomass such as sewage sludge, algae and animal residues, wool keratin exhibits a relatively homogeneous and well-defined molecular structure dominated by keratin, with abundant disulfide bonds and stable peptide linkages. In contrast, sewage sludge often contains high ash content and inorganic impurities that may inhibit catalytic performance, while microalgae typically present highly variable compositions and moisture content, leading to less stable gasification behavior.49,50 These differences suggest that wool may follow distinct reaction pathways during SCWG, particularly in terms of sulfur evolution, intermediate formation, and hydrogen production mechanisms. However, systematic studies on wool SCWG focusing on hydrogen production, product distribution and catalytic effects are still lacking.
This paper uses waste wool as the feedstock to study the hydrogen production behavior by SCWG. By monitoring gaseous and liquid products simultaneously, we evaluate gasification performance in terms of CE, HE, hydrogen selectivity, gas lower heating value (LHV), molar fractions of gas components and gas yield. Carbon and hydrogen conversion pathways are investigated along with the reaction mechanism. Unlike conventional studies that primarily focus on process optimization, this work emphasizes the intrinsic relationship between protein structure and gasification behavior, and the theoretical and experimental results are presented to support clean hydrogen production from proteinbased biomass and high value resource utilization of waste wool.
| Ultimate analysis (wt%) | ||||
|---|---|---|---|---|
| C | H | N | O | S |
| 42.93 | 6.2175 | 14.305 | 28.5415 | 2.586 |
| Industrial Analysis(wt%) | ||||
|---|---|---|---|---|
| Moisture | Ash content | Volatile component | Fixed carbon | Total |
| 9.805 | 0.355 | 76.6 | 13.24 | 100 |
During the experiment, the quartz tubes in the reactor will gradually be heated to the set temperature. At this point, the timing begins. After reaching the specified residence time, the quartz tubes will be removed and allowed to cool down. After cooling is complete, the products will be collected. The gas products will be collected in a stainless steel tube. The specific collection method is as follows: first, blow high-purity nitrogen gas through the stainless steel tube to expel the internal air. Then, place the quartz tube inside and seal it with a rubber stopper. Next, use another steel tube to strike forcefully, causing the quartz tube to break. The gas was collected in the steel tube, and then connect one end of a rubber tube to the exhaust valve of the steel tube and the other end to a U-shaped tube with a scale. Open the exhaust valve and observe that the liquid level in the U-shaped tube drops. The difference between the liquid levels before and after is the volume of the produced gas. The liquid products were collected in test tubes, and the specific collection method is as follows: first, vigorously shake the quartz tube to cause the liquid to accumulate at the other end. Then, use a glass knife to make a circular cut at an appropriate position in the quartz tube, and then break the quartz tube by hand, collecting the liquid product in the test tube. All experiments were performed in triplicate, and gas composition measurements were repeated to ensure data reliability and reproducibility.
| Steam reforming: C + H2O → CO + H2 ΔH298K = 131.29 KJ mol−1 |
| Water–gas shift: CO + H2O ↔ CO2 + H2 ΔH298K = 41.17 KJ mol−1 |
| Methanation: CO + 3H2 ↔ CH4 + H2O ΔH298K = −206.10 KJ mol−1 |
| CO + 4H2 ↔ CH4 + 2H2O ΔH298K = −164.93 KJ mol−1 |
Fig. 2(b) shows the temperature dependence of gas products in gasification. Gas products consist mostly of H2, CO2, CO, CH4, C2H4, and C2H6. As the reaction temperature increases, the gas production increases to 42.72mol kg−1 at 600 °C compared to 17.02 mol kg−1 at 400 °C. High temperature favours gas formation. Major gas species form at higher temperatures. H2 and CO2 yields increase significantly from 1.59 and 2.46 mol kg−1 at 400 °C to 11.91 and 6.09 mol kg−1 at 600 °C, respectively. Notably, the yield of CO exhibits a pronounced increase between 450 °C and 500 °C, rising from approximately 8.04 mol kg−1 to 12.11 mol kg−1. This behavior arises from thermal cracking and decarboxylation of oxygenated intermediates (carboxylic acids, aldehydes, ketones) generated during initial wool keratin decomposition. The effect is reflected in an increased extent of cracking and decarboxylation of these intermediates (e.g., from 8.04 mol kg−1 to 12.11 mol kg−1). At the relevant temperatures, the intermediates acquire sufficient energy to overcome activation barriers for C–O and C–C bond cleavage, which leads to release of carbon monoxide. In addition, partial oxidation reactions and the limited extent of the water–gas shift (WGS) reaction at moderate supercritical temperature favour CO accumulation. As a result, the conversion of CO to CO2 is not complete under these conditions, leading to relatively higher CO yields. This imbalance between CO formation and its subsequent conversion contributes to the observed CO-dominant behavior in the gas products. In turn, the 450–500 °C interval is the critical time when secondary decomposition pathways are significantly accelerated. The increase in H2 yield above 500 °C can be attributed to the combined effects of primary decomposition and secondary gasification reactions. At elevated temperatures, the thermal cracking of wool keratin is significantly intensified, leading to the continuous formation of intermediate gaseous species such as CO, CH4, and light hydrocarbons. Meanwhile, steam reforming and water–gas shift reactions are also enhanced under supercritical conditions, contributing to additional hydrogen production. However, the simultaneous increase in CO and CH4 yields suggests that the formation rates of these intermediates exceed their consumption rates via secondary reactions. Therefore, the observed increase in H2 is not solely due to the consumption of CO and CH4, but rather results from a dynamic balance between rapid generation of intermediates and their partial conversion into hydrogen. Similar behavior has been reported in SCWG of other biomass feedstocks, where parallel reaction pathways dominate at high temperatures.
Fig. 2(c) shows the distribution of the fractions and lower heating value of product gases at different temperatures. Reaction temperature changes the composition of gas and energy quality: if temperature increase from 400 °C to 600 °C, gas composition shifts dramatically from a temperature increase from 2.41 to 5.84 MJ Nm−3 (significantly up). H2 fraction changes with temperature (9.35% increase from 400 °C to 27.87% increase from 600 °C), CO and CH4 fractions decrease (44.30% decrease from 31.01% and 21.08% increase to 18.84%, respectively). C2H6 and C2H4 fractions decrease with temperature increase. At 400 °C, product gas is predominant by CO2 and CH4, low H2 and CO fractions, which results in LHV of only 2.41–2.59 MJ Nm−3, suggesting wool first thermal cracking with limited water reforming, leading to low combustible gas proportions and low energy density. As the temperature reached 500 °C, H2 and CO fractions increased significantly, LHV reaching 3.77 MJ Nm−3, reflecting the increase of steam reforming and water–gas shift reactions in supercritical water, which further convert wool-cracking intermediates (oxygenated organics, tar and light hydrocarbons) into small molecules combustible gases, improving gas energy quality. At 550–600 °C, H2 and CO became the main gas components (with significant increases), while CH4 and other light hydrocarbons were stable or decreased. LHV reached 5.13–5.84 MJ Nm−3, suggesting that high temperatures favor hydrogen-rich high-energy-density syngas production due to water reactivity at high temperatures which promote deep reforming of tar and solid carbon and inhibiting methanation, shifting reaction system toward H2 and CO production.
As shown in Fig. 3(b), feedstock concentration affects individual gas component yields in wool SCWG. H2 yield drops from 11.91 mol kg−1 at 2 wt% to 1.16 mol kg−1 at 9 wt%. The drop is particularly steep between 2 wt% and 5 wt%. CO and CO2 yield drop from 13.25 mol kg−1 and 6.09 mol kg−1 to 3.35 mol kg−1 and 2.07 mol kg−1, respectively. This drastic decrease in H2 and CO2 yields is mainly attributed to the reduced water-to-carbon ratio at higher feedstock concentrations. At low concentrations (2–5 wt%), excess supercritical water promotes steam reforming and water–gas shift reactions, enabling efficient conversion of keratin-derived intermediates into gaseous products. However, as the concentration increases, the relative water availability decreases, limiting these water-mediated reactions. As a result, intermediate products are not fully converted and may instead undergo condensation, polymerization, or char formation, thereby suppressing the formation of gaseous species such as H2, CO, and CO2. Therefore, the limited water availability also suppresses the formation of CO, leading to its decreasing trend with increasing feedstock concentration. However, at the highest concentration (11 wt%), a slight increase in CO yield is observed. This may be attributed to enhanced thermal cracking under high organic loading, which promotes the formation of CO from intermediate species, partially offsetting the limitation imposed by reduced water availability. As shown in Fig. 3(c), the H2 fraction of the product gas generally decreases with increasing feedstock concentration from 2 wt% to 9 wt%, due to the reduced water-to-carbon ratio that limits steam reforming and water–gas shift reactions. However, when the concentration further increases to 11 wt%, this trend is no longer strictly followed. This deviation may be attributed to enhanced thermal cracking and secondary reactions at high organic loading, which promote the formation of gaseous products and partially offset the limitation of water availability. Gas lower heating value (LHV) is decreasing, then increasing. At low concentrations, large water participation favors steam reforming and water–gas shift reactions, promoting H2. As concentration increases, the effective water-to-carbon ratio decreases, making organic intermediates more susceptible to methanation and condensation, thus increasing CH4 and reducing H2 fraction. The largest decline in H2 fraction occurs between 2 and 5 wt% feedstock concentrations (from 27.87% to approximately 14.94%), while the decrease is more moderate at higher concentrations (for example, from 5 wt% to 11 wt%). This pattern indicates a critical threshold in the hydrodynamics and reaction chemistry: at 2 wt% the water-to-carbon ratio is sufficient to sustain near-complete steam reforming and water–gas shift activity, maximizing H2 selectivity. At higher feedstock loadings, the greater CH4 mass fraction compensates for reduced H2 production and contributes to the observed rebound in gas LHV.
Fig. 4(b) shows the distribution of gaseous products (H2, CO2, CH4, CO, and light hydrocarbons C2H6 and C2H4) under different residence times. Total gas yield increased from 11.88 mol kg−1 to 27.87 mol kg−1 when residence time was extended to 7 min, and then decreased significantly to 21.08 mol kg−1 at 9 min. This suggests that 7 min is sufficient for complete wool gasification, while longer residence time accelerates the loss of reaction intermediates and triggers competitive side reactions. Gas production characteristics show that CH4 and CO dominate the product gas. Yields of H2 and CO2 were increased continuously in the first 7 min. C2H4 was only at trace levels at 1 min, while C2H6 was suppressed in the reaction. The sharp increase in CH4 and CO2 yields occurs between 5 min and 7 min, the period of maximum gas production. This is due to the completion of primary thermal cracking and intensive secondary reforming reaction. By 5 min, most of the keratin macromolecules have been decomposed into oxygenated organic intermediates (carbon acids, aldehydes, ketones, tar-like substances) through hydrolysis and pyrolysis. These intermediates are not fully converted into gaseous products yet. Extending the residence time to 7 min provides enough time for these reactive species to undergo further transformation via steam reforming, water–gas shift, and gasification reactions in a supercritical water environment.
Fig. 4(c) shows the variation of gas fractions and lower heating value as a function of residence time. As residence time increased from 1 to 7 min, CO2 and H2 fractions increased to different degrees while the CO proportion decreased. At 1 min, CO, CO2, and H2 fractions were 34.26%, 14.26%, and 8.98%, respectively. Gas composition reached quasi-equilibrium after 7 min, CO and CO2 stabilizing at 22.37% and 22.07%, respectively, H2 reached 10.46% at 5 min. Energy density increased significantly after 5 min to a maximum of 4.48 MJ Nm−3 at 7 min. In the first reaction phase, oxygen groups in wool cracking with decarboxylation and carbonyl cleavage reactions produced rapid CO and CO2 production; however incomplete water–gas shift reaction produced high CO molar fractions. As the residence time extended to 5–7 min, CO was consumed by water–gas shift reaction and converted into H2 and CO2 with reduced CO content and continuous H2 increase. This improved gas system reducibility and energy density, leading to maximum LHV at 7 min.
:
1. Copper-containing catalysts are generally considered to facilitate the decomposition of large organic structures, while Al2O3 may contribute to improved dispersion and structural stability.54–56 Based on these considerations, Cu and Cu–Al2O3 composite catalysts were employed in this work.
The corresponding hydrogen conversion efficiency (HE), carbon conversion efficiency (CE), and hydrogen selectivity obtained with Cu, Cu-3% Al2O3, and Cu-7% Al2O3 are summarized in Fig. 5(a), with the non-catalytic case serving as the reference. Compared with the non-catalytic run, the addition of Cu slightly increased hydrogen selectivity, while the carbon conversion efficiency (CE) remained nearly unchanged and the hydrogen efficiency (HE) showed a slight decrease. The addition of Cu-3% Al2O3 increased wool CE and HE from 38.32% and 48.17% to 77.95% and 99.23%, respectively, but with lower hydrogen selectivity. Cu-7% Al2O3 led to decreases in CE, HE, and hydrogen selectivity. These results suggest that different Cu-based catalysts may influence the reaction pathways during wool SCWG.
Cu species may facilitate reactions such as CO hydrogenation and water–gas shift, thereby contributing to enhanced hydrogen selectivity. However, their ability to promote deep cracking of macromolecular organic structures and aromatic intermediates may be limited, which could explain the relatively small improvement in CE and HE observed with Cu alone. The presence of Al2O3 in Cu-3% Al2O3 may contribute to increased surface area and provide sites that could facilitate chain scission, reforming, and gasification of keratin-derived intermediates, leading to improved carbon and hydrogen conversion efficiencies. However, enhanced cracking and reforming may also increase the formation of CO and CO2, thereby reducing hydrogen selectivity. When the Al2O3 content is further increased to 7%, the proportion of non-selective reactions may increase, which could explain the observed decrease in hydrogen selectivity. These observations suggest that the metal-support ratio in the Cu–Al2O3 system may play an important role in determining the gasification performance.53–55
Fig. 5(b) shows individual component gas yields and total gas yields under different catalysts. Cu addition slightly lowered the total gas yield compared to the non-catalytic control, whereas Cu-3% Al2O3 and Cu-7% Al2O3 increased total gas yield. All three catalysts slightly increased H2 yields and influenced gas-phase reactions. Cu species may promote hydrogenation or equilibrium conversion of specific CO/CO2 species, thereby adjusting gas composition with limited impact on total gas production. In contrast, Cu–Al2O3 composite catalysts may enhance overall gas formation due to the combined effects of Cu species and the Al2O3 support. Al2O3 may act as a thermally stable support and could help maintain the dispersion of Cu-containing species under supercritical conditions.53–55 In addition, its surface properties may facilitate interactions with intermediates and water, which could contribute to enhanced gasification reactions. As a result, increases in CH4, CO, and CO2 yields are observed with composite catalysts, suggesting a shift toward more extensive gasification pathways.
Fig. 5(c) presents the gas mole fractions and LHV under different catalysts. The gas composition and LHV vary significantly with catalyst type. The Cu-only catalyst increases the H2 molar fraction while slightly reducing LHV. This behavior may be associated with reactions such as water–gas shift, which increase H2 production but may suppress the formation of higher-heating-value hydrocarbons such as CH4 and C2H6. In contrast, Cu–Al2O3 composite catalysts may exhibit dual catalytic functions, where Cu species contribute to reforming and water–gas shift reactions, and the Al2O3 support may influence the adsorption and transformation of organic intermediates. This combined effect could promote the formation of light hydrocarbons and improve LHV.
Preliminary experiments showed that Cu-3% Al2O3 promotes wool SCWG; therefore, its loading effect was further investigated at 600 °C, 9 wt% feedstock concentration, and 5 min residence time. The specific catalytic masses are shown in Table 2.
| Cu-3% Al2O3 loading ratio | Cu-3% Al2O3 mass/mg | Wool mass/mg |
|---|---|---|
| 0.5 | 4.5 | 9 |
| 1 | 9 | 9 |
| 1.5 | 13.5 | 9 |
Fig. 6(a) presents CE, HE, and hydrogen selectivity under different catalyst loadings. The catalyst loading is defined as the mass ratio of catalyst to biomass (wool), excluding water. Compared to the non-catalytic control, all loadings improved CE and HE, whereas hydrogen selectivity increased only at the highest loading. At a catalyst loading of 1, CE and HE reached their maximum values of 77.95% and 99.29%, respectively, while hydrogen selectivity slightly decreased. This improvement may be associated with a more favorable distribution of active sites, which could enhance the interaction between catalyst surfaces and reactive intermediates without significant mass transfer limitations. At moderate loading, catalytic sites may be sufficient to promote hydrolysis, reforming, and water–gas shift reactions, enabling efficient conversion of organic carbon and hydrogen into gaseous products.53,55
At higher loading (1.5), CE and HE decreased, while hydrogen selectivity increased. This behavior may be related to possible particle aggregation or mass transfer limitations, which could reduce the accessibility of active sites and hinder the conversion of intermediates. As a result, fewer secondary reactions may occur, allowing a larger fraction of hydrogen to remain as H2, thereby increasing selectivity.
Fig. 6(b) shows gas yields under different Cu-3% Al2O3 loadings. All loadings increased total gas yield, with the highest value observed at loading 1. This may be attributed to a balance between active site availability, dispersion, and mass transfer. At lower loading, limited catalytic sites may restrict gasification, whereas at higher loading, possible aggregation and diffusion limitations may reduce catalytic efficiency.53–55
As shown in Fig. 6(c), catalyst loading of 1 yields the highest CH4 molar fraction and favorable gas composition for improved LHV. The higher CH4 yield may be associated with enhanced methanation-related reactions, possibly facilitated by the availability of H2 and CO/CO2 intermediates. Meanwhile, the Al2O3 support may influence the transformation of oxygenated intermediates, contributing to the formation of CO, CO2, and light hydrocarbons.
| No. | RT/min | Compound name | Peak area percentage/% | ||||
|---|---|---|---|---|---|---|---|
| 1 min | 3 min | 5 min | 7 min | 9 min | |||
| 1 | 5.24 | Pyrrole | 100 | 100 | 58.36 | 100 | 100 |
| 2 | 5.44 | Toluene | 85.01 | 67.8 | 100 | 73.48 | 99.52 |
| 3 | 8.27 | Bicyclo[2.2.1]hept-2-ene, 1-methy | — | 11.33 | — | — | — |
| 4 | 8.29 | Ethylbenzene | — | — | 8.04 | 2.83 | — |
| 5 | 8.47 | 1,2-Cyclononadiene | — | 4.42 | — | — | — |
| 6 | 8.48 | 1,3-Cyclopentadiene, 5-(1-methylethylidene) | — | — | 4.12 | — | — |
| 7 | 8.49 | 1,7-Octadiyne | — | — | — | 2.83 | — |
| 8 | 11.74 | Phenol | — | — | 0.7 | 1.7 | 7.06 |
| 9 | 14.99 | Azulene | — | — | 5.13 | — | — |
| 10 | 15 | Naphthalene | — | — | — | 1.87 | — |
| 11 | 18.49 | m-Aminophenylacetylene | — | — | — | 2.86 | — |
Fig. 7 shows the evolution of chromatographic peaks in liquid-phase products as a function of reaction time. At 1–3 min, low-retention-time compounds such as pyrrole and toluene exhibit high peak intensities, which may suggest rapid primary cracking of protein structures and the formation of nitrogen-containing and aromatic intermediates. At 5 min, the increase in aromatic compounds such as ethylbenzene and phenol may indicate the accumulation of secondary liquid-phase intermediates. At 7–9 min, the peak intensities of toluene and pyrrole decrease, while high-retention-time compounds (e.g., naphthalene and m-aminophenylacetylene) appear. This trend could suggest further aromatization and condensation of liquid-phase intermediates. In addition, cracking and reforming of aromatic intermediates may occur simultaneously, which could contribute to reduced liquid accumulation and enhanced gasification efficiency.51,56,57
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| Fig. 7 GC-MS chromatograms of liquid products from wool SCWG at various residence times (600 °C, 9 wt%). | ||
Fig. 8 presents a proposed reaction pathway based on the analysis of liquid-phase products obtained during wool SCWG at different residence times. It should be noted that this mechanism is inferred from product distribution and should be interpreted as a possible pathway rather than a definitive reaction scheme. The gasification of wool in supercritical water may involve several sequential and parallel steps, including macromolecular depolymerization, aromatization, and secondary cracking reactions. In the initial stage (1 min), keratin may be rapidly hydrolyzed into amino acid intermediates, which could undergo deamination and decarboxylation reactions, leading to the formation of nitrogen-containing heterocycles (e.g., pyrrole) and monocyclic aromatic compounds (e.g., toluene).51 At intermediate stages (3–5 min), compounds such as ethylbenzene and phenol begin to appear, which may indicate that alkyl rearrangement, dehydrogenation, and partial condensation reactions become more significant, resulting in a more complex mixture of liquid intermediates.56 At longer residence times (7–9 min), early intermediates may decrease or stabilize, while polycyclic aromatic hydrocarbons (PAHs, such as naphthalene) are formed. This could suggest further aromatization and condensation reactions, leading to the growth of aromatic ring structures. Meanwhile, the decrease in certain liquid intermediates may imply that they are further converted into gaseous products through C–C bond cleavage and possible free radical reactions under supercritical water conditions.57
Based on the experimental observations and literature reports, the gasification of wool in supercritical water is likely to involve multiple parallel and consecutive reactions. Initially, wool keratin undergoes hydrolysis and thermal cracking to form smaller intermediates such as amino acids, peptides, oxygenated compounds, and light hydrocarbons. These intermediates may subsequently participate in steam reforming, decarboxylation, methanation, and water–gas shift reactions under supercritical conditions, leading to the formation of H2, CO, CO2, CH4, and light hydrocarbon gases. The final gas composition is therefore considered to result from the dynamic competition between intermediate formation and secondary conversion reactions. In particular, reaction temperature, residence time, feedstock concentration, and catalyst composition may influence the relative contribution of these pathways. It should be noted that the proposed reaction pathways are mainly inferred from product distribution trends and literature reports, while detailed kinetic and mechanistic investigations remain subjects for future study.
In addition, the gaseous products from wool SCWG were mainly composed of H2, CO, CO2, and CH4, which is generally consistent with previous SCWG studies on biomass feedstocks. However, compared with conventional biomass systems where CO2 is usually dominant, relatively higher CO yields were observed in this work. This behavior may be related to the unique keratin structure of wool and the complex decomposition pathways of protein-derived intermediates under supercritical conditions. Overall, the results demonstrate that waste wool exhibits considerable potential as a protein-rich feedstock for hydrogen-rich gas production through SCWG.
The results showed that increasing temperature significantly promoted gas formation and improved gasification performance. Under the optimal conditions of 600 °C, 2 wt% feedstock concentration, and 5 min residence time, the carbon conversion efficiency (CE) and hydrogen efficiency (HE) reached 95.71% and 119.26%, respectively, with a maximum H2 yield of 11.91 mol kg−1. The gaseous products were mainly composed of H2, CO, CO2, and CH4.
Among the tested catalysts, Cu-3% Al2O3 exhibited the best catalytic performance. Compared with the non-catalytic condition, the catalyst increased CE by 39.63%, HE by 51.13%, and total gas yield by 13.35 mol kg−1 under suitable conditions, indicating that Cu-based catalysts can effectively promote the gasification of wool-derived intermediates under supercritical conditions.
Liquid-phase analysis indicated that pyrrole, phenolic compounds, alkylbenzenes, and polycyclic aromatic hydrocarbons were important intermediates during wool SCWG, suggesting that hydrogen production is closely associated with the progressive conversion of keratin-derived organic compounds into gaseous products.
Overall, the results demonstrate that waste wool has considerable potential as a feedstock for hydrogen-rich gas production via SCWG. However, detailed catalyst characterization, kinetic analysis, and complete elemental balance analysis were not conducted in the present study. Future work will focus on catalyst structure-performance relationships, nitrogen/sulfur transformation behavior, and more comprehensive thermodynamic and mechanistic investigations.
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