Leonardo Severini1,2, Kevin J De France2, Deeptanshu Sivaraman3, Nico Kummer2,4, Gustav Nyström2,4. 1. Department of Chemical Sciences and Technologies, University of Rome "Tor Vergata", Via della Ricerca Scientifica 1, 00133 Rome, Italy. 2. Laboratory for Cellulose & Wood Materials, Empa-Swiss Federal Laboratories for Materials Science and Technology, Überlandstrasse 129, 8600 Dübendorf, Switzerland. 3. Laboratory for Building Energy Materials and Components, Empa, Swiss Federal Laboratories for Materials Science and Technology, Überlandstrasse 129, CH-8600 Dübendorf, Switzerland. 4. Department of Health Science and Technology, ETH Zürich, Schmelzbergstrasse 9, 8092 Zürich, Switzerland.
Abstract
Modern science is increasingly turning to nature for inspiration to design sustainable biomaterials in a smart and effective way. Herein, we describe biohybrid aerogels based on electrostatic complexation between cellulose and proteins-two of the most abundant natural polymers on Earth. The effects of both particle surface charge and particle size are investigated with respect to aerogel properties including the morphology, surface area, stability, and mechanical strength. Specifically, negatively charged nanocellulose (cellulose nanocrystals and cellulose nanofibers) and positively charged lysozyme amyloid fibers (full-length and shortened via sonication) are investigated in the preparation of fibrillar aerogels, whereby the nanocellulose component was found to have the largest effect on the resulting aerogel properties. Although electrostatic interactions between these two classes of charged nanoparticles allow us to avoid the use of any cross-linking agents, the resulting aerogels demonstrate a simple additive performance as compared to their respective single-component aerogels. This lack of synergy indicates that although electrostatic complexation certainly leads to the formation of local aggregates, these interactions alone may not be strong enough to synergistically improve bulk aerogel properties. Nevertheless, the results reported herein represent a critical step toward a broader understanding of biohybrid materials based on cellulose and proteins.
Modern science is increasingly turning to nature for inspiration to design sustainable biomaterials in a smart and effective way. Herein, we describe biohybrid aerogels based on electrostatic complexation between cellulose and proteins-two of the most abundant natural polymers on Earth. The effects of both particle surface charge and particle size are investigated with respect to aerogel properties including the morphology, surface area, stability, and mechanical strength. Specifically, negatively charged nanocellulose (cellulose nanocrystals and cellulose nanofibers) and positively charged lysozyme amyloid fibers (full-length and shortened via sonication) are investigated in the preparation of fibrillar aerogels, whereby the nanocellulose component was found to have the largest effect on the resulting aerogel properties. Although electrostatic interactions between these two classes of charged nanoparticles allow us to avoid the use of any cross-linking agents, the resulting aerogels demonstrate a simple additive performance as compared to their respective single-component aerogels. This lack of synergy indicates that although electrostatic complexation certainly leads to the formation of local aggregates, these interactions alone may not be strong enough to synergistically improve bulk aerogel properties. Nevertheless, the results reported herein represent a critical step toward a broader understanding of biohybrid materials based on cellulose and proteins.
Through
evolution and adaptation, natural biological materials
perform a variety of specific roles with high efficiency in mild conditions.[1] As a result, there is growing interest in taking
inspiration directly from nature in order to develop sustainable and
highly functional biobased materials. Due to their biocompatibility,
biodegradability, and a range of chemical functionalities, these biobased
materials have attracted significant attention in a wide range of
fields such as biomedical, renewable energy, cultural heritage preservation,
and building technology, representing a sustainable alternative to
petroleum-based resources.[2−10] Cellulose and proteins are two of the most abundant biopolymers
on Earth, playing diversified roles in many biological systems[11−14] and, as a result, are commonly used as natural building blocks in
the preparation of biobased materials such as hydrogels and aerogels.
In particular, due to their light weight, high specific surface area,
and porous structure, aerogels commonly find application as oil/chemical
absorbents, thermal insulators, biomedical scaffolds, and biocatalysts;
however, before reaching practical application, the fundamental properties
and interactions within biobased aerogels need to be thoroughly investigated.[15]Nanocelluloses are a class of fibril-like
nanoparticles, comprising
packed cellulose polymer chains with at least one dimension in the
nanoscale.[16] In general, nanocelluloses
exhibit good strength, stiffness, and easily tunable surface chemistry,[17] making them ideal candidates for the fabrication
of structured materials, including aerogels, finding application in
areas such as insulating materials, biomedical scaffolds, and adsorbents.[18−23] Depending on the preparation method employed, nanocelluloses can
be divided into cellulose nanofibers (CNFs, long and semiflexible
fibers with both highly regular crystalline and less well-ordered
domains, typically produced via mechanical fibrillation) and cellulose
nanocrystals (CNCs, shorter and more rigid fibers with a high degree
of crystallinity, typically produced via acid hydrolysis).[17,24] Due to the increased flexibility and high aspect ratio of CNFs,
they tend to form physically entangled gel networks at low concentrations,
while due to the increased rigidity and crystallinity of CNCs, they
are often used as mechanical reinforcing agents in composite materials.[17,25]Protein amyloid fibrils are a class of elongated ordered supramolecular
filaments, stabilized by β-sheet secondary structures, and formed
via the self-assembly of protein/peptide fragments.[26−28] Moreover, due
to their flexible structure, amyloid fibers can also form entangled
networks at relatively low concentrations, which is ideal for the
formation of aerogels.[29,30] In general, protein amyloids
are extremely versatile, due to the functional diversity in the protein/peptide
moieties they are formed from; this has led to their application in
areas such as catalysis, filtration, drug delivery, and biomimetic
functional materials.[31,32] To this end, lysozyme has gained
particular interest for its ability to rapidly form amyloid aggregates
with broad spectrum antibacterial resistance.[33−36] This is of particular interest
as lysozyme in its native form demonstrates little to no antibacterial
efficacy against Gram-negative bacteria.[37]Despite the great potential of nanocellulose and protein amyloids,
their combination to form composite materials has not been widely
investigated. Notably, the Freire group prepared composite films from
CNFs and lysozyme amyloids, demonstrating the potential of such materials
for both water purification and wound healing applications.[38,39] Here, films were formed via vacuum filtration of the mixed two-component
suspensions, whereby the presence of lysozyme amyloid fibers led to
an increase in heavy metal removal from contaminated water and increases
in antioxidant and antimicrobial activity (against Gram-positive Staphylococcus aureus) versus CNF-only films. In
all cases, the film’s mechanical properties were relatively
similar, albeit with decreased elongation at break (increased brittleness)
apparent upon lysozyme amyloid addition.[38,39] Similarly, work in our group previously investigated the preparation
of structured composite films from CNCs and lysozyme amyloids via
an evaporation-induced self-assembly.[40] Although the electrostatic complexation between negatively charged
CNCs and positively charged lysozyme amyloids led to films with a
decreased structural order, the incorporation of lysozyme amyloids
improved the film’s antimicrobial properties against Gram-positive S. aureus, again with relatively small effects on
film mechanics. Taken together, these results suggest that the incorporation
of protein amyloids into nanocellulose-based materials is an effective
method to add functionality based on the amyloid component, with the
nanocellulose component providing structural integrity. To this end,
herein, we prepare electrostatically complexed biohybrid aerogels
from nanocellulose (CNC and TO-CNF) and lysozyme amyloids [full-length
(AMY-FL) and sonicated (AMY-S)]. The effects of nanocellulose and
lysozyme morphology are investigated with respect to aerogel properties
including the porosity, stability, and mechanical strength.
Results and Discussion
Nanocellulose–lysozyme
amyloid biohybrid suspensions were
formed via simple electrostatic complexation between negatively charged
nanocellulose (CNC zeta potential = −36.3 ± 2.3 mV and
TO-CNF zeta potential = −43.1 ± 3.3 mV) and positively
charged lysozyme amyloid fibrils (AMY-FL zeta potential = 48.7 ±
2.2 mV and AMY-S zeta potential = 40.9 ± 1.1 mV). This process
is shown schematically in Figure . Vortex mixing 2 wt % suspensions at a 1:1 ratio resulted
in the immediate formation of colloidal aggregates (optical photographs, Supporting Information, Figure S2), indicated
by the increase in suspension turbidity. Aggregation was also apparent
via dynamic light scattering (DLS), with z-average
diameters in the micron range (Figure ). The aggregate size followed the trend of the nanoparticle
size, whereby TO-CNF/AMY-FL suspensions showed the largest z-average diameter (apparent size larger than 10 μm)
and CNC/AMY-S suspensions showed the smallest (6.5 ± 1.3 μm).
This suggests that nanoparticle entanglement plays a large role in
the aggregate network formation via electrostatic complexation. These
biohybrid networks were visualized via scanning electron microscopy
(SEM) (Supporting Information, Figure S3),
whereby, in general, suspensions containing TO-CNFs appeared to have
a more compact pore structure with larger pores and suspensions containing
CNCs appeared to have a more open pore structure with smaller pores.
No clear differences were evidenced between samples containing AMY-FL
and AMY-S, this suggests that the nanocellulose component has a greater
impact on the network morphology than the lysozyme amyloid component.
As nanocellulose is commonly incorporated into composite materials
as a key structural component,[21,41] here it also shows
the greatest effect on the porosity/pore structure.
Figure 1
Schematic representation
of nanocellulose (TO-CNF or CNC) and lysozyme
amyloid (AMY-FL or AMY-S) components used as building blocks in the
preparation of biohybrid aerogels. Biohybrid mixtures were frozen
using liquid nitrogen and freeze-dried in order to obtain the corresponding
aerogels.
Figure 2
Suspension characterizations for the single-component
and biohybrid
mixtures: (A) z-average diameter and (B) zeta potential
values. * Apparent size larger than the maximum measurable value for
the DLS instrument.
Schematic representation
of nanocellulose (TO-CNF or CNC) and lysozyme
amyloid (AMY-FL or AMY-S) components used as building blocks in the
preparation of biohybrid aerogels. Biohybrid mixtures were frozen
using liquid nitrogen and freeze-dried in order to obtain the corresponding
aerogels.Suspension characterizations for the single-component
and biohybrid
mixtures: (A) z-average diameter and (B) zeta potential
values. * Apparent size larger than the maximum measurable value for
the DLS instrument.Aerogels were formed
via simple freeze-drying of the single-component
and biohybrid suspensions described above. Suspensions were directly
submerged in liquid nitrogen, whereby ice crystal growth compresses
the particles/biohybrid aggregates, forcing increased interactions
via hydrogen bonding, hydrophobic interactions, and physical entanglement.
In general, aerogels containing TO-CNF were relatively compact and
easy to handle, while aerogels containing CNC were fluffier and more
delicate (single-component and biohybrid aerogels can be seen in Supporting Information, Figure S4). This can
be attributed to the biohybrid aggregate morphology observed via SEM,
as discussed above. All formed aerogels demonstrated a relatively
low degree of shrinkage (calculated as the final aerogel cross-sectional
area divided by the cross-sectional area of the mold used, Supporting Information, Table S1), indicating
the maintenance of an intact internal porous structure. Interestingly,
TO-CNF/AMY-FL aerogels showed the highest degree of shrinkage (13.5
± 0.3%), while CNC/AMY-S aerogels showed the lowest (7.2 ±
0.1%), following the trend for the aggregate size discussed above.
This is intuitive as the relatively flexible nature of TO-CNF and
AMY-FL would allow for increased compression/compaction during freezing
as compared to the relatively rigid and less entangled CNC and AMY-S.
Note that the poorer shape fidelity of the CNC-containing aerogels
likely also leads to an over-estimation of the cross-sectional area
due to the fluffy nature of these samples. Correspondingly, a biohybrid
aerogel morphology was assessed via SEM (Figure ), whereby aerogels containing TO-CNF exhibited
a more compact pore structure than aerogels containing CNC. SEM images
of the single-component aerogels can be seen in the Supporting Information (Figure S5).
Figure 3
SEM images of biohybrid
aerogels: (A) TO-CNF/AMY-FL, (B) TO-CNF/AMY-S,
(C) CNC/AMY-FL, and (D) CNC/AMY-S. All scale bars are 500 μm.
SEM images of biohybrid
aerogels: (A) TO-CNF/AMY-FL, (B) TO-CNF/AMY-S,
(C) CNC/AMY-FL, and (D) CNC/AMY-S. All scale bars are 500 μm.In all cases, aerogels exhibited a relatively low
specific surface
area, as expected due to the freeze-drying process used (Supporting Information, Table S2).[22,25] Because the process for the gel matrix and aerogel production involve
freezing and immobilization of the amyloid fibers and CNFs with electrostatic
forces and not chemical/physical bonding, we expect to see larger
pores (see Figure for SEM images) in comparison to other freeze-dried aerogels and
supercritically dried aerogels.[42,43] This kind of pore structure
and processing traditionally results in lower Brunauer–Emmett–Teller
(BET) surface areas, as they are outside the mesoporous range (2–50
nm). Here, TO-CNF-containing aerogels showed the highest BET specific
surface area (∼20 m2/g) as compared to CNC-containing
aerogels (∼3 m2/g). This is most likely attributed
to the pore collapse of the relatively fluffy CNC-containing aerogels
during both the freeze-drying process and aerogel handling/BET sample
preparation. Here again, relatively minimal effects of the amyloid
component were evidenced on aerogel porosity, supporting the hypothesis
of the nanocellulose component acting as the key structural building
block in these biohybrid composites. Sorption isotherms for all aerogel
samples can be seen in the Supporting Information (Figure S6), whereby a type IV H2/H1 isotherm with large macropores
but some mesoporosity dominates for CNF-containing aerogels, while
an isotherm more of type II with large macropores and almost no mesopores
dominates for CNC-containing aerogels.[44,45]The
aerogel chemical composition was assessed via Fourier transform
infrared (FTIR) (Figure ); pure nanocellulose aerogels displayed broad peaks at ∼3340
cm–1 and ∼2900/∼1430 cm–1, which are attributed to O–H stretching vibrations and C–H
stretching/bending vibrations, respectively. A characteristic carbohydrate
fingerprint is also apparent between 900 and 1280 cm–1.[46,47] Additionally, TO-CNF aerogels displayed
a peak at ∼1600 cm–1, related to the presence
of carboxylate moieties from the 2,2,6,6-tetramethyl-1-piperidinyloxyl
(TEMPO) oxidation process. Pure lysozyme amyloid aerogels also displayed
broad peaks at ∼3340 cm–1 due to O–H
and N–H stretching vibrations[48,49] but in addition
showed strong vibrational bands attributed to amide I (∼1650
cm–1) and amide II (∼1540 cm–1) modes, which are very sensitive to protein secondary structure/conformational
changes. Here, the amide I band is mainly attributed to C=O
stretching vibrations belonging to backbone polypeptide chains; the
amide II band arises from a combination of N–H in-plane bending,
C–N stretching, and other amide group vibrations.[50−53] The deconvolution of AMY-FL and AMY-S aerogel spectra was performed
in order to evaluate the effects of sonication on the protein secondary
structure (Supporting Information, Table
S3).[54] In both cases, a high content of
the β-sheet structure, as expected
for protein amyloids,[40,55−57] was evidenced,
with almost no variation before and after sonication. This suggests
that sonication is an effective method for tuning amyloid fibril length
without affecting its protein conformational state. Expectedly, biohybrid
aerogels displayed peak characteristic for both nanocellulose and
lysozyme amyloids, indicating the successful incorporation of both
components.
Figure 4
Normalized absorbance ATR–FTIR spectra in the range of 3600–800
cm–1: (A) single-component and (B) biohybrid aerogels.
Several characteristic peaks are highlighted.
Normalized absorbance ATR–FTIR spectra in the range of 3600–800
cm–1: (A) single-component and (B) biohybrid aerogels.
Several characteristic peaks are highlighted.Aerogel stability was assessed both thermogravimetrically (Supporting Information, Figure S7 and Table S4)
and in water (Supporting Information, Figure
S8). In all cases, thermogravimetric profiles (Figure S7A) follow a classic two-stage trend for biological
materials; in the first stage (generally below 200 °C) relatively
minimal mass-loss is evidenced, corresponding mainly to the evaporation
of absorbed and intermolecular H-bonded water. In the second stage
(generally above 200 °C), depolymerization and degradation of
biopolymer chains are prevalent and result in considerable mass loss.[57] The onset of thermal degradation values (Table S4) shows that CNC aerogels are the most
thermally stable (287 °C), while TO-CNF aerogels are the least
stable, with the onset of thermal degradation beginning at 224 °C.
This difference in thermal stability can be attributed to the surface
charge density and degree of crystallinity; previous studies have
shown that nanocellulose functionalized with sulfate groups exhibits
greater thermal stability than nanocellulose functionalized with carboxylic
groups. Moreover, previous studies have also demonstrated that nanocellulose
with a higher degree of crystallinity (which is the case for CNC vs
TO-CNF) shows a higher onset of thermal degradation.[58−60] The onset of thermal degradation for both AMY-FL and AMY-S is intermediate
to that of TO-CNF and CNC, but importantly both AMY-FL and AMY-S exhibit
an identical degradation behavior, indicating that the sonication
process does not affect the thermal stability of the resulting amyloid
fibers. Expectedly, biohybrid aerogels exhibited intermediate thermal
degradation profiles compared to their single-component counterparts.
Notably, only aerogels containing TO-CNF showed any stability in water;
this suggests that TO-CNF network entanglement is crucial, and electrostatic
complexation alone cannot guarantee aerogel stability. Intuitively,
AMY-FL fibrils are also long and flexible, and therefore should be
able to form entangled network structures similar to TO-CNF, however
little stability in water was observed for these aerogels. This likely
has to do with the overall conversion of native lysozyme into its
amyloid state; previous research has demonstrated that mature lysozyme
amyloid fibers still contain a significant portion of the non-structured
lysozyme,[36] as the entire peptide sequence
does not become involved in amyloid fiber formation.[55,61] Therefore here, the presence of the native/non-structured lysozyme
likely hinders network formation as there is a lower concentration
of the structured fibers within the aerogels.In order to study
and compare aerogel mechanical performance, compressive
stress–strain testing was performed (Supporting Information, Figure S9), whereby Young’s modulus values
were calculated from the initial linear viscoelastic region (Figure ). For single-component
aerogels, Young’s modulus values for TO-CNF aerogels (191 ±
5 kPa) were an order of magnitude larger than for any of the other
single-component aerogels, again demonstrating the importance of network
entanglement. Conversely, aerogels deriving from rigid CNCs show a
lamellar internal structure, which generally yields poor mechanical
properties.[62] Similarly for AMY-FL and
AMY-S, the resulting aerogels are relatively weak and fragile due
to an internal plate-like morphology. Biohybrid aerogels showed intermediate
Young’s modulus values between their respective single-component
counterparts, demonstrating simple additive performance. This lack
of synergistic reinforcement via electrostatic complexation perhaps
indicates that although the formation of local aggregation occurs
between negatively charged nanocellulose and positively charged lysozyme
amyloids, this does not necessarily lead to a globally complexed structure.
To further test this hypothesis, biohybrid aerogels containing a 10:1
ratio of nanocellulose to lysozyme amyloids (a ratio that we have
previously shown to be synergistic in other materials)[40] were prepared, and Young’s modulus values
were determined (Supporting Information, Figure S10). Here again, a simple additive performance between
the two network components was observed with no evidence of synergistic
enhancements in the network strength. This likely indicates that internal
regions containing a higher concentration of lysozyme amyloids act
as weak points within the gel network, which are more susceptible
to compression. Note that in all cases, the aerogels demonstrate poor
shape recovery, suggesting that additional (chemical) cross-linking
may be required for applications where cyclic loading and unloading
cycles are foreseen.
Figure 5
Young’s modulus values for aerogel samples as determined
via compression. The results are presented as the average with error
bars representing the standard deviation, whereby at least four samples
were measured for each aerogel. Representative stress–strain
curves are presented in the Supporting Information (Figure S9A).
Young’s modulus values for aerogel samples as determined
via compression. The results are presented as the average with error
bars representing the standard deviation, whereby at least four samples
were measured for each aerogel. Representative stress–strain
curves are presented in the Supporting Information (Figure S9A).Finally, the effects of the freezing
process were investigated
on aerogel formation via the preparation of directionally frozen single-component
and biohybrid aerogels (Figure ). Directional freezing—or ice-templating—is
a process whereby a solidifying solvent (water) progresses uniaxially
through a dispersed phase, which is excluded to form an organized
and anisotropic pore wall structure after sublimation.[63,64] Here, SEM images of single-component aerogels sectioned parallel
to the ice crystal growth direction reveal a typical and relatively
homogeneous aligned pore morphology, consistent with other biobased
aerogels prepared via similar techniques (CNC shown in Figure , all others in the Supporting Information, Figure S11).[65,66] For all single-component aerogels, as seen in Figure , this enhanced pore orientation leads to
enhanced mechanical reinforcement along this axis (vertical) with
respect to the perpendicular one (horizontal). This is due to the
aligned/lamellar pore structure providing increased resistance in
the direction of applied stress. Interestingly, directionally frozen
biohybrid aerogels do not exhibit a regular aligned pore morphology
(SEM image for CNC/AMY-FL shown in Figure , all others in Supporting Information, Figure S11); this is likely due to the formation
of local electrostatically complexed aggregates hindering ice-crystal
growth. It is well known that the formation of a regular anisotropic
pore morphology depends heavily on the effective rejection of particles
in the dispersed phase by the advancing ice front.[63,64] As the particle size increases, the ability to effectively exclude
these particles and form a homogeneous pore morphology decreases;[63] here, we hypothesize that the locally formed
aggregates likely act as larger particles themselves, disrupting the
freezing process and leading to a more heterogeneous pore morphology.
Correspondingly, these biohybrid aerogels do not exhibit any prominent
mechanical anisotropy, with Young’s modulus values similar
in both horizontal and vertical directions (Figure ). Taken together, these results suggest
that locally, electrostatic complexation can be a prominent contributor
to aggregate formation; however, across larger length scales, these
interactions are insufficient to produce robust biohybrid aerogels
and can even hinder bulk material properties.[67]
Figure 6
(A)
Schematic illustration of the ice-templating process to prepare
single-component and biohybrid aerogels via liquid nitrogen-induced
directional freezing. (B) SEM images of directionally frozen aerogels:
(1) CNC and (2) CNC/AMY-FL respectively. (C) Young’s modulus
values in the vertical (parallel to the freezing direction) and horizontal
(perpendicular to the freezing direction) directions for ice-templated
aerogel samples. The results are presented as the average with error
bars representing the standard deviation, whereby at least four samples
were measured for each condition.
(A)
Schematic illustration of the ice-templating process to prepare
single-component and biohybrid aerogels via liquid nitrogen-induced
directional freezing. (B) SEM images of directionally frozen aerogels:
(1) CNC and (2) CNC/AMY-FL respectively. (C) Young’s modulus
values in the vertical (parallel to the freezing direction) and horizontal
(perpendicular to the freezing direction) directions for ice-templated
aerogel samples. The results are presented as the average with error
bars representing the standard deviation, whereby at least four samples
were measured for each condition.
Conclusions
In conclusion, biohybrid aerogels were
successfully prepared via
electrostatic complexation between negatively charged nanocellulose
(TO-CNFs and CNCs) and positively charged lysozyme amyloid fibrils
(AMY-FL and AMY-S). In general, the nanocellulose component appeared
to play the biggest role in a biohybrid aerogel morphology and mechanical
properties, with CNF-based aerogels having a more compact and organized
pore structure and CNC-based aerogels showing a more open and plate-like
pore morphology. Additionally, the mechanical properties were much
better for the CNF-based biohybrid aerogels than the CNC-based biohybrid
aerogels; however, in both cases, these aerogels demonstrated a simple
additive performance as compared to their respective single-component
aerogel counterparts. This indicates that although electrostatic complexation
was evidenced between the nanocellulose component and the lysozyme
amyloid component, these interactions alone are not strong enough
to result in any bulk synergistic effects. This is supported by SEM
images of directionally frozen aerogels, whereby single-component
gels exhibit a typical anisotropic pore morphology and mechanical
properties, whereas biohybrid aerogels exhibit a much more disorganized
structure and relatively isotropic mechanical properties, attributed
to local electrostatic aggregates hindering ice crystal growth during
the freezing process. Taken together, the results presented here represent
a meaningful step toward a broader understanding of biohybrid aerogels
based on nanocellulose and protein amyloid fibrils and the interactions
therein.
Experimental Section
Materials
CNCs (prepared via sulfuric
acid hydrolysis of bleached softwood kraft pulp) were purchased in
a freeze-dried form from CelluForce (Montreal, Canada). CNCs were
probe-sonicated (10 min, 60% amplitude, Digital Sonifier 450, Branson
Ultrasonics) at a concentration of 2 wt % in distilled water and refrigerated
until use. Never-dried elemental chlorine-free cellulose fibers from
bleached softwood pulp (Picea abies and Pinus app.) were obtained from
Stendal GmbH (Berlin, Germany) and used for the preparation of TEMPO-oxidized
CNFs (TO-CNFs) following our previously published protocol.[67] The prepared TO-CNFs were concentrated to 2
wt % and refrigerated until further use. Hen egg white lysozyme (HEWL,
>90%), (3-aminopropyl)triethoxysilane (APTES), and sodium hydroxide
(NaOH) were purchased from Sigma-Aldrich. TEMPO, sodium hypochlorite
(NaClO) solution (12–14% chlorine), hydrochloric acid (HCl),
and sodium chloride were purchased from VWR. Sodium bromide (NaBr
≥99%) was supplied by Carl Roth GmbH & Co. All chemicals
were used as received.
Preparation of Lysozyme
Amyloid Fibrils (Full
Length and Sonicated)
Lysozyme amyloid fibrils were prepared
via our previously published protocol.[40] Briefly, the HEWL powder was dissolved in a Falcon tube at a concentration
of 2 wt % in distilled water, and the pH was adjusted to 2.0 using
1.0 M HCl. The HEWL solution was then placed in a thermomixer (Eppendorf
AG) set to 90 °C and mixed at 400 rpm for 24 h to produce full-length
amyloid fibrils (AMY-FL).[40] Optionally,
AMY-FL were then sonicated (10 min, 2 s pulse, 30% amplitude) to generate
shorter fibers (AMY-S).[36] The lysozyme
amyloid fibril suspensions were stored at 4 °C in a fridge until
use.
Preparation of Single-Component and Biohybrid
Aerogels
Aerogels were prepared from single-component and
mixed (1:1 by weight) biohybrid suspensions, having a total solid
content of 2 wt % in all cases. For the single-component aerogels,
2 wt % suspensions were directly frozen in liquid nitrogen and stored
in a −80 °C freezer overnight prior to freeze-drying (FreeZone
4.5, Labconco, USA). For the biohybrid aerogels, HEWL amyloid fibrils
(AMY-FL or AMY-S) were vortex-mixed for 1 min with equal volumes of
nanocellulose (TO-CNFs or CNCs) to obtain four different biohybrid
combinations. These mixtures were then directly frozen and freeze-dried
following the same procedure as for single-component aerogels. This
process is shown schematically, along with aerogel nomenclature, in Figure . As a comparison,
directional freezing was also performed for all cases, whereby suspensions
were poured into Teflon molds and placed on a stainless-steel plate
partially submerged in liquid nitrogen to induce gradient ice crystal
growth. As before, samples were then placed in a −80 °C
freezer overnight prior to freeze-drying. Prepared aerogel samples
were stored at room temperature prior to use/characterization.
Characterization
Single-component
and biohybrid suspensions were characterized via DLS (0.025 wt % in
water) and zeta potential measurements (0.25 wt % in 10 mM NaCl) using
a ZetaSizer Nano ZS (Malvern). AFM measurements (Supporting Information, Figure S1, Bruker ICON3) were performed
in the tapping mode (0.05 mg/mL in pH 2 Milli-Q for AMY-FL and AMY-S
on mica substrates; 0.005 mg/mL in Milli-Q for TO-CNFs and CNCs on
0.05% APTES-coated mica substrates). Single-component and biohybrid
aerogels were characterized via FTIR spectroscopy in the attenuated
total reflectance (ATR) mode (Bruker Switzerland AG). Spectra were
recorded between 4000 and 400 cm–1 with a resolution
of 4 cm–1 and 32 scans per sample. Deconvolution
was performed in the 1360–1800 cm–1 region
on normalized absorbance ATR-FTIR spectra by means of Voigt bands
of full width at half height (FWHH) of 25 cm–1 maximum,
using OMNIC software. Aerogel cross sections and internal porosity
were assessed via SEM (FEI NanoSEM 230). Samples were coated with
a thin layer of platinum (∼2 nm) before imaging (5.0 mm working
distance and 5.0 kV accelerating voltage). Compression testing was
performed using a Z010 device (Zwick) equipped with a 20 N load cell.
A compression rate corresponding to ∼10% of the initial specimen
height per min was used for all measurements. The samples were compressed
to 80% strain, whereby Young’s modulus was calculated from
the initial linear portion of the stress–strain curves. Compression
testing was repeated in at least quadruplicate, with results presented
as the average ± standard deviation. Thermal properties of aerogels
were analyzed using a Netzsch TG 209F1 thermogravimetric analyzer
operating at 10 K min–1. Nitrogen adsorption–desorption
isotherms were carried out on a Micromeritics 3 Flex (Micromeritics,
USA) device, and the surface areas were calculated by the BET method.
A sample of the measured mass (30–40 mg) was placed in a special
glass sample tube and degassed to 0.016 mbar for 15 h at 85 °C
prior to the measurements. The samples were weighed again, and the
nitrogen sorption isotherms were analyzed at 77 K from P/P0 ranging from 0.001 to 0.998 in 50
steps, with a maximum equilibration time of 600 s for each incremental
nitrogen addition, for a total run time of ∼6 h.
Authors: Nuno H C S Silva; Patrícia Garrido-Pascual; Catarina Moreirinha; Adelaide Almeida; Teodoro Palomares; Ana Alonso-Varona; Carla Vilela; Carmen S R Freire Journal: Int J Biol Macromol Date: 2020-10-05 Impact factor: 6.953
Authors: Pu Chun Ke; Ruhong Zhou; Louise C Serpell; Roland Riek; Tuomas P J Knowles; Hilal A Lashuel; Ehud Gazit; Ian W Hamley; Thomas P Davis; Marcus Fändrich; Daniel Erik Otzen; Matthew R Chapman; Christopher M Dobson; David S Eisenberg; Raffaele Mezzenga Journal: Chem Soc Rev Date: 2020-07-07 Impact factor: 54.564