Global energy demand has been on the continuous rise and is anticipated to further increase by an astonishing 47% in the near future2. Current primary energy sources, which are still derived from non-renewable fossil fuels, are unsustainable and detrimental to the environment due to the large emissions of greenhouse gases (GHG) into the atmosphere. Hence, to curb global warming, there is an urgent need for new technologies based on renewable and sustainable energy generation sources.
Fuel cells are considered a promising sustainable technology for energy conversion to generate electricity without CO2 emissions using electrochemical reactions11. Among the various types of fuel cells, hydrogen fuel cells are particularly attractive from a decarbonization point-of-view, with efforts focusing on the production of green hydrogen as the next renewable fuel12. The heart of a fuel cell lies in the membrane electrode assembly (MEA), which consists of a proton exchange membrane (PEM) that selectively allows only the passage of protons between the electrodes. Perfluorosulfonic acid (PFSA) membranes such as NafionÔ and AquivionÒ remain the benchmark state-of-the-art PEMs used in fuel cells due to their high proton conductivity, chemical inertness, and mechanical stability. However, the production of Nafion is very expensive due to the use of fluorinated chemicals13 and pose serious environmental concerns relating to poor biodegradability and environmental toxicity of perfluorinated materials14. Moreover, the functionalization of polymers through sulfonation usually involve highly corrosive reagents, reducing their environmental friendliness,15-17 boosting the search for greener and more economical materials for large-scale applications.
Inspired by the ubiquity of proton conduction in the living world18,19 as well as their intrinsic biodegradability, studies have explored biopolymers (proteins and polysaccharides) as potential proton conductive materials20,21. The proton conductivity of naturally occurring proteins is generally too low to be useful in practical applications but has been improved with functional group modifications8,22. Alternatively, high proton conductivity can be achieved in biopolymers through de novo design of peptides utilizing nanostructure-aided conductivity23 or metal oxide-peptide composites 24, but these approaches still face challenges regarding cost and scalability.
Chicken feathers are produced at a staggering rate of 40 million tons annually as a byproduct from the poultry industry5, but have been underutilized due to their unsuitable nutritional profile. Furthermore, they face disposal challenges due to the generation of toxic sulfur dioxide from incineration. Efforts to valorize chicken feathers include their use as hydrogels25,26, biosorbents for heavy metals27,28, functional films29 and fibers30. These studies point out that feather keratin may be re-configured into highly functional materials, notably exploiting the structural properties and high cysteine (Cys) content of keratin proteins. However, no attempts have been made to date to revalue keratin into renewable energy devices. In this work, we chose chicken feathers as a starting material for fabricating proton conductive biomaterials. Keratin proteins were extracted from industrial chicken feathers using an environmentally friendly and scalable process and converted into amyloid fibrils that were subsequently processed into free-standing amyloid fibril membranes. Proton conductive properties were imparted through a post-oxidative treatment which converted Cys thiols into sulfonic acid groups, using a benign environmental process with harmless and inexpensive chemical compounds. The performance of the membrane was demonstrated in a fuel cell device capable to transform by electrochemical reaction H2 and O2 (the latter directly from air) into electrical power and mechanical work (with H2O as sole byproduct). To demonstrate the general potential of this approach, we highlight two additional applications of these materials, as protonic field-effect transistors, as well as in the generation of H2 via water splitting.
Protein extraction and isolation
An overview of the production of feather keratin proton conductive membranes is depicted in Fig. 1. Keratin was extracted and isolated from chicken feathers and heat treated to produce keratin amyloid fibrils (Fig. 1a), after which they were mixed with a crosslinker and dopant and cast onto a substrate to produce a free-standing membrane. The membrane was then heat cured followed by an oxidative treatment to produce a modified membrane with imparted proton conductive properties (Fig. 1b), which was then assembled into a fuel cell (Fig. 1c) or other devices utilizing proton conductivity.
Among protein-containing industrial waste byproducts, chicken feathers have the highest protein content (ca. 90%) and are most abundant in Cys amino acid (ca. 8%, Fig. 2a)5. However, the extraction and isolation procedure of feather keratin on a large scale has faced challenges, notably the use of harsh toxic solvents (e.g. sodium sulfide) and reducing agents such as b-mercaptoethanol and dithiothreitol, or long isolation dialysis treatments31. Here, we extracted feather keratin using a basic solvent consisting of urea and thioglycolate. Urea acted as a chaotropic solvent disrupting the hydrogen bonds within the compact structure of feathers, while thioglycolate served as a reducing agent to reduce intra- and intermolecular disulfide bonds, resulting in the separation of protein inter-chains and eventually dissolution. The supernatant was then precipitated and washed to obtain a crude keratin isolate. We re-extracted this isolate in ammoniacal solution and precipitated it to obtain a pure keratin isolate, which displayed only a single protein band around 10 kDa as analyzed by electrophoresis (Fig. 2b), demonstrating minimal protein degradation during the entire process. An amino acid analysis of the obtained keratin isolate revealed 7 mol.% of Cys (Supplementary Fig. S1), in agreement with the expected 8 mol.% from earlier reports32. Our process produced a feather keratin isolate almost fully soluble in dilute acid, in contrast to keratin isolates obtained from other extraction procedures, which require concentrated acids33. Furthermore, the process does not require dialysis, enabling scalability and fast production rates.
Protein fibrillization
Within the family of keratin proteins, hair and wool keratins belong to a-keratins composed of a-helix intermediate filaments, while keratin from feathers, claws, and beaks belong to b-keratins dominated by b-sheet secondary structures34,35. While early x-ray diffraction (XRD) studies on feather barbs suggested the presence of amyloid-like fibrils36, the self-assembly of regenerated feather keratin into amyloid fibrils has not yet been reported to date. Sequence analysis of feather keratin from the UniProt database (P02450) using a variety of protein structure prediction algorithms (Supplementary Fig. S2) indicated that feather keratin could be assembled into amyloid fibrils. The structure of feather keratin has been reported to consist of a central region with predominantly hydrophobic residues adopting a b-sheet conformation32, with Cys residues primarily located at the N- and C-termini37. The highest propensity for b-sheet aggregation was predicted to occur between residues Val32–Leu43, which lie within this central region and have also been identified as a hotspot for amyloidogenic aggregation. Thus, we postulated that feather keratin could be self-assembled into amyloid fibrils, which was verified by the facile self-assembly of keratin monomers into amyloid fibrils after heat treatment at 90°C under acidic conditions. Using thiazole orange as a molecular probe for amyloid fibrils38, the fibrillization process proceeded relatively quickly and reached a plateau after only 2h, exhibiting a faster kinetic than that of animal-derived b-lactoglobulin39 or plant-derived proteins40 (Fig. 2c). Solutions of feather keratin amyloid fibrils also exhibited birefringence under cross-polarized light, corroborating the presence of amyloid fibrils (inset of Fig. 2c), which were found to be several micrometers in length after 5h as imaged by Atomic Force Microscopy (AFM) and Transmission Electron Microscopy (TEM) (Fig. 2d and 2i). The nanofibrils exhibited an average height of about 7 nm (Fig. 2e), a semiflexible behavior with comparable contour (Fig. 2f) and persistence (Fig. 2g) lengths in the range, and periodic pitches of 90 nm along the fibril axis (Fig. 2h), as expected for most amyloid fibrils.
Membrane fabrication
We then mixed feather keratin amyloid fibrils with glyoxal and mercaptosuccinic acid and cast the solution to obtain a clear free-standing flexible membrane (Supplementary Fig. S3a), followed by thermal curing (Supplementary Fig. S3b). As we hypothesized that proton conduction could be imparted into the membrane upon conversion of thiol groups into sulfonic acids, we immersed the membranes in peracetic acid to oxidize thiols and disulfide bonds to sulfonic acids (Supplementary Fig. S3c)10,41. The final membrane is denoted as Keratin-M.
Oxidation into sulfonic acid was corroborated by both Fourier Transform Infrared Spectroscopy (FTIR) and Raman Spectroscopy, with the appearance of the S=O peak at 1040 cm-1 42 (Fig. 3a) in the FTIR spectrum, and the disappearance of the Raman shift peak at 2550 cm-1 assigned to the thiol43 (Fig. 3b). This was further supported by XPS measurements, which showed the major peaks of -SO3- 2p3/2 and 2p1/2 doublets at 168.2 and 169.6 eV, respectively, after deconvolution44-47. Peaks of sulfone and sulfate groups were also observed, possibly due to side reactions in the fabrication process (Fig. 3c). As the modification of thiols into sulfonic acids confers a negative charge, the difference in surface potential before and after modification was detected by Kelvin Probe Force Microscopy (KPFM). Before modification, the keratin casting solution deposited onto the Highly Oriented Pyrolytic Graphite (HOPG) substrate exhibited a relative positive potential, which likely arose from positively charged amino acids Arg and Lys. Upon oxidative treatment, the membrane exhibited a relative negative potential that may have resulted from the conversion of neutral thiols into negatively charged sulfonic acids (Fig. 3d and Supplementary Fig. S5).
Throughout the fabrication process, the membrane maintained its shape and mechanical integrity while still possessing birefringence arising from amyloid fibrils under cross-polarized light (Supplementary Fig. S3d), suggesting that the amyloid fibrils were preserved without significant alteration. The XRD pattern of the membranes displayed two dominant peaks at 9.3° and 19.6°, corresponding to d-spacings of 4.5 Å and 9.5 Å, respectively, that reflect the signature cross-b structure of amyloid fibrils48,49 (Fig. 3e). A smooth surface was observed under SEM for keratin-M membranes (Supplementary Fig. S6), whereas at higher magnification a fibrillar network morphology was identified on the surface with pore sizes of 7–20 nm (Fig. 3f). In contrast, neat keratin membranes showed a denser morphology with lower porosity (Supplementary Fig. S7).
Membrane properties
The modification of neutral thiols into negatively charged sulfonic acids was also indicated by the increase in ion exchange capacity (IEC) from 0.18 meq g-1 to 0.84 meq g-1 after oxidative treatment, while a further increase to 1.56 meq g-1 was achieved with the addition of MSA due to the contribution of additional thiol groups (Table 1). The boost in IEC also resulted in a higher water uptake due to enhanced hydration and charge repulsion from the anionic sulfonic acid groups, which could possibly explain the larger pore size from keratin-M due to higher swelling compared to neat keratin membranes. Keratin-M membranes maintained good barrier properties despite the presence of nanopores, demonstrating almost no permeability to dye molecules such as Rhodamine B (Supplementary Fig. S8). They also exhibited 3-fold less permeability to small molecules such as methanol compared to Nafion (Supplementary Fig. S9), demonstrating their potential in direct methanol fuel cells in which Nafion performs less efficiently due to its high methanol permeability50. The membranes were mechanically robust and could be readily manipulated without damaging them. Their thermo-mechanical characterization is reported in the supplementary information (Young’s Modulus and tensile strength in Supplementary Table S1 and Fig. S10; thermal behavior and glass transition in Fig. S11). Supercritical CO2-dried keratin membranes measured with TGA displayed a 10% decrease in weight until 100°C attributed to the evaporation of water, followed by thermal degradation and deamidation with drastic weight loss (~ 60%) between 300°C to 400°C51 (Supplementary Fig. S12).
Table 1. Feather keratin membrane properties before and after treatment
Membrane
|
IEC (meq g-1)
|
Water Uptake (%)
|
Pre-treated
|
0.18 ± 0.03
|
55.3 ± 6.7
|
Neat keratin
|
0.84 ± 0.05
|
131.3 ± 17
|
Keratin-M
|
1.56 ± 0.03
|
215.9 ± 31
|
Nafion 117
|
1.10 ± 0.02
|
17.0 ± 1.2
|
The main parameter in a fuel cell is the proton conductivity (s), which is essential for any polymer electrolyte membrane. After the successful conversion of thiols into sulfonic acids, feather keratin membranes exhibited an enhanced proton conductivity that increased with the MSA content from 0.02 mS cm-1 to 6.3 mS cm-1 in water (Fig. 4a). The appearance of the semi-circle in the Nyquist plot of neat membranes indicate a more capacitive behavior (Fig. 4b), as also evidenced in the large phase angle from the Bode plot (Supplementary Fig. S13a). This characteristic shifted towards a membrane with a resistor-type behavior for keratin-M membranes, as seen from an almost absent semi-circle in the Nyquist plot (Fig. 4c) and a phase angle approaching 0° at high frequencies in the Bode plot (Supplementary Fig. S13b). Comparing across biomaterials reported to date, the proton conductivity of keratin-M is the highest among all biopolymers, with the exception of specifically engineered peptides (Supplementary Table S2 and S3). But in contrast to the latter, feather keratin membranes are processed from low-value waste materials with a strong potential for scaling-up. Remarkably, because this comes from a waste stream intended for incineration (and CO2 emissions), this process takes place with an overall negative carbon footprint, adding value to both sustainability and environmental friendliness. Furthermore, the proton conductivity of the membranes could still be further improved by doping with acid electrolytes, notably with sulfuric acid which provided the most significant increment to 22.8 mS cm-1, and which may find applications in vanadium redox flow batteries.
Fuel cell performance
Having demonstrated a suitable proton conductivity for the ensued amyloid keratin membranes, we then tested their in-situ performance as a polymer electrolyte membrane in a hydrogen fuel cell (Supplementary Fig. S14). The open circuit voltage (OCV) of a fuel cell has been reported to provide a useful indication of the integrity and degradative behavior of the membrane such as thinning and pinhole formation52. The cell assembled with keratin-M membrane displayed an OCV between 0.95 – 1 V –comparable to Nafion – and polarization curves were obtained at increasing temperature. With air at the cathode, the cell generated an increased power density with temperature, reaching up to 20 mW cm-2 at 65°C (Fig. 4d). Similarly, the peak power of 25 mW cm-2 was generated with pure oxygen at 55°C, after which it decreased to 21 mW cm-2 at 65°C (Fig. 4e). This could be due to an increase in reactive oxygen species generated with increased oxygen concentration, leading to the formation of free radicals such as OH×, H×, and HOO× that have been reported to initiate membrane degradation53,54. Further increase in temperature to 80°C resulted in a drop in OCV to 0.85 – 0.9 V along with a decreased power density lower than that at 65°C. To ensure a high OCV and optimal performance, a membrane of low hydrogen permeability is desired. Utilizing staircase voltammetry with N2 at the cathode (Supplementary Fig. S16), the hydrogen permeability of the keratin membrane was assessed and calculated using the intercept, yielding 3.8 ± 0.3 ´ 10-10 mol cm-2 s-1, (compare to Nafion - 3.8 ´ 10-9 mol cm-2 s-1)55 while the electrical resistance obtained from the slope was approximately 3200 ± 140 Ohm cm2 (Supplementary Fig. S17)56,57.
To demonstrate the applicability of the keratin-M membrane in hydrogen fuel cells, we assembled the membrane into a commercial test fuel cell setup. With hydrogen and air as the respective fuels at the anode and cathode, the cell was able to generate power to turn on both red and white LED lamps (Supplementary Fig. S18). In addition, the cell was responsive to the presence of fuel, turning the LED lamp on and off with the introduction and absence of hydrogen (Supplementary Movie S1). Most importantly, the fuel cell could perform mechanical work, e.g. drive a fan setup driven by a motor (Supplementary Movie S2) as well as a fuel cell toy car ((Supplementary Movie S4 and Fig. 4f). Furthermore, the keratin-M PEM membranes could be further used as an electrolyzer for the production of hydrogen and oxygen from water when applying an electric bias, as observed by the formation of bubbles at the respective outlets (Supplementary Movie S4 & Supplementary Fig. S19).
Transistor performance
Finally, we demonstrate the application of keratin-M as a solid-state film for the fabrication of protonic field-effect transistors (H+-FETs). Devices were fabricated by casting keratin-M film between two gold/palladium hydride (PdHx) electrodes pre-deposited using e-beam evaporation process on a 50 nm hafnium oxide (HfO2) gate dielectric layer (Fig. 4g). The conductivity of the keratin-M film was observed to be dependent on relative humidity (RH), displaying a surge in current when the RH increased from 50% to 90% (Fig. 4h and Supplementary Fig. S20), as a result of the increase in proton conductivity with increased hydration, which is commonly observed in most proton conductive materials20,22,58. The transfer characteristics of the FET device (Fig. 4i) measured for negative and positive gate voltages (VGS) at a source to drain voltage (VSD) of 0.5 V exhibited a ON-to-OFF ratio of ~ 1.4 with a low leakage current (Supplementary Fig. 21). The output characteristics of the device displayed a similar trend whereby the channel conductivity increased upon application of negative VGS (Supplementary Fig. 23 and 24). Biasing the device with negative VGS induced positive charges into the channel proportional to VGS as the keratin-M and Si gate form a capacitor with HfO2 as the dielectric. This resulted in an increased positive charge carrier concentration and thereby channel conductivity. The electrostatic gating effect highlights the potential use of keratin-M in H+-FETs.