Shennan Wang1, Cheng Wang2, Qi Zhou1,3. 1. Division of Glycoscience, Department of Chemistry, School of Engineering Sciences in Chemistry, Biotechnology and Health, KTH Royal Institute of Technology, AlbaNova University Centre, Stockholm SE-106 91, Sweden. 2. Advanced Fibro-Science, Kyoto Institute of Technology, Kyoto 606-8585, Japan. 3. Wallenberg Wood Science Center, Department of Fibre and Polymer Technology, KTH Royal Institute of Technology, Stockholm SE-100 44, Sweden.
Abstract
Mechanical stability and multicycle durability are essential for emerging solid sorbents to maintain an efficient CO2 adsorption capacity and reduce cost. In this work, a strong foam-like composite is developed as a CO2 sorbent by the in situ growth of thermally stable and microporous metal-organic frameworks (MOFs) in a mesoporous cellulose template derived from balsa wood, which is delignified by using sodium chlorite and further functionalized by 2,2,6,6-tetramethylpiperidine-1-oxyl (TEMPO)-mediated oxidation. The surface carboxyl groups in the TEMPO-oxidized wood template (TO-wood) facilitate the coordination of the cellulose network with multivalent metal ions and thus enable the nucleation and in situ growth of MOFs including copper benzene-1,3,5-tricarboxylate [Cu3(BTC)2], zinc 2-methylimidazolate, and aluminum benzene-1,3,5-tricarboxylate. The TO-wood/Cu3(BTC)2 composite shows a high specific surface area of 471 m2 g-1 and a high CO2 adsorption capacity of 1.46 mmol g-1 at 25 °C and atmospheric pressure. It also demonstrates high durability during the temperature swing cyclic CO2 adsorption/desorption test. In addition, the TO-wood/Cu3(BTC)2 composite is lightweight but exceptionally strong with a specific elastic modulus of 3034 kN m kg-1 and a specific yield strength of 68 kN m kg-1 under the compression test. The strong and durable TO-wood/MOF composites can potentially be used as a solid sorbent for CO2 capture, and their application can possibly be extended to environmental remediation, gas separation and purification, insulation, and catalysis.
Mechanical stability and multicycle durability are essential for emerging solid sorbents to maintain an efficient CO2 adsorption capacity and reduce cost. In this work, a strong foam-like composite is developed as a CO2 sorbent by the in situ growth of thermally stable and microporous metal-organic frameworks (MOFs) in a mesoporous cellulose template derived from balsa wood, which is delignified by using sodium chlorite and further functionalized by 2,2,6,6-tetramethylpiperidine-1-oxyl (TEMPO)-mediated oxidation. The surface carboxyl groups in the TEMPO-oxidized wood template (TO-wood) facilitate the coordination of the cellulose network with multivalent metal ions and thus enable the nucleation and in situ growth of MOFs including copper benzene-1,3,5-tricarboxylate [Cu3(BTC)2], zinc 2-methylimidazolate, and aluminum benzene-1,3,5-tricarboxylate. The TO-wood/Cu3(BTC)2 composite shows a high specific surface area of 471 m2 g-1 and a high CO2 adsorption capacity of 1.46 mmol g-1 at 25 °C and atmospheric pressure. It also demonstrates high durability during the temperature swing cyclic CO2 adsorption/desorption test. In addition, the TO-wood/Cu3(BTC)2 composite is lightweight but exceptionally strong with a specific elastic modulus of 3034 kN m kg-1 and a specific yield strength of 68 kN m kg-1 under the compression test. The strong and durable TO-wood/MOF composites can potentially be used as a solid sorbent for CO2 capture, and their application can possibly be extended to environmental remediation, gas separation and purification, insulation, and catalysis.
Entities:
Keywords:
CO2 capture; MOFs; composites; mechanical properties; mesoporous wood template
CO2 capture technologies are of great importance to
mitigate the greenhouse gas emission and reduce its environmental
impact.[1] Enormous efforts have been previously
made to develop solid CO2 sorbents with high energy efficiency
and multicycle durability by using porous materials including zeolite,[2] silica,[3] and activated
carbon,[4,5] or amine-based sorbents with CO2-reactive polyethyleneimine (PEI),[6] 3-(triethoxysilyl)propylamine
(APTES),[7] and ethylenediamine.[8,9] Recently, metal-organic frameworks (MOFs) have attracted much attention
for applications in CO2 capture,[10−12] catalysis,[13−15] and sensing,[16] owing to their favorable
large surface area and tunable micro-/mesopore structure. Mechanical
integrity and strength are essential for the practical application
of solid sorbents to avoid pulverization and thus overcome high pressure
drop and poor mass transfer.[17] To this
end, monolithic MOF-based CO2 sorbents have been prepared
through strategies such as stepwise gelation of MOFs,[18] 3D printing,[19] and in situ growth
of MOFs in preformed inorganic network including porous carbon,[20] macro-/mesoporous silica,[21] and graphene hydrogel.[22] For
instance, graphene/zeolitic imidazolate framework-8 (ZIF-8) hybrid
aerogel showed an elastic modulus of 280 kPa and a maximum strength
of 16 kPa under compressive deformation.[22] Utilizing clay and poly(vinyl alcohol) (PVA) as the binder and plasticizer
enabled the 3D printing of a cobalt-based MOF (UTSA-16) into a channeled
monolithic structure, which showed an elastic modulus of 25 MPa and
a compressive strength of 0.55 MPa at a density of 1659 kg m–3.[19]In addition, deposition, encapsulation,
or in situ synthesis of
MOF particles such as zirconium terephthalate-based MOF (UiO-66),
copper-based MOF (MOF-199), and ZIF-8 in natural wood was developed.
The corresponding wood/MOF composites were demonstrated to have high
removal efficiency for organic pollutants,[23] superior selectivity toward CO2 adsorption against N2,[24] and good antibacterial activities.[25] Furthermore, carbonization of wood-/cobalt-based
MOF composites produced a high-power 3D monolithic reactor for improved
mass transfer and CO conversion during Fischer–Tropsch synthesis.[26] These composites have combined the functionalities
of MOFs and mechanical robustness of wood. Particularly, beech wood
with in situ synthesized ZIF-8 showed a high compressive strength
of 100 MPa, which outperformed polymer-based MOF composites.[24] However, insufficient coordination sites in
cell lumen surfaces of natural wood resulted in the low loading of
MOFs around 2 wt %, limiting wood/MOF composites to be used for the
large capacity adsorption of CO2.[23,24] The binding and adhesion of MOFs to the cellulosic substrate can
be enhanced by introducing surface functional groups such as carboxyl
groups. High loading of MOFs (>30 wt %) has been previously reported
when using 2,2,6,6-tetramethylpiperidine-1-oxyl (TEMPO)-oxidized cellulose
nanofibers (TO-CNFs) with surface carboxyl groups as the substrate
for the interfacial synthesis of MOFs toward pollution remediation,[27] thermal insulation,[28] energy storage,[29] and volatile organic
compound separation.[30] However, the potential
of using surface carboxylated CNFs for developing strong and durable
sorbents for CO2 capture has not yet been explored.In our previous study, a hierarchical 3D network of cellulose microfibrils
was prepared from wood through a top-down delignification process,
followed by TEMPO-mediated oxidation at neutral conditions.[31] This TEMPO-oxidized wood (TO-wood) showed a
highly mesoporous cell wall structure with fibrillated but naturally
aligned cellulose microfibrils and demonstrated high mechanical performance.
Herein, we report a facile approach to fabricate foam-like cellulose/MOF
composites with prominent mechanical properties, good thermal stability,
and high CO2 adsorption capacity using TO-wood structure
as the template. The carboxyl groups in the fibrillated cell wall
of TO-wood facilitated interfacial coordination to copper (Cu2+)-, zinc (Zn2+)-, and aluminum (Al3+)-based MOFs and promoted their growth in situ, thus increasing the
loading of MOFs. The specific surface area, CO2 adsorption
capacities, multicycle durability under temperature swing adsorption,
and compressive mechanical properties of the TO-wood/MOF composites
were studied to demonstrate their potential application as a strong
and durable sorbent for efficient CO2 capture.
Experimental Section
Chemicals
and Materials
Balsa wood
(Ochroma pyramidale) was purchased
from Materials AB, Sweden. Cu(NO3)2·(H2O)3, Al(NO3)3, Zn(NO3)2·(H2O)6, benzene-1,3,5-tricarboxylic
acid (H3BTC), 2-methylimidazole, TEMPO, sodium chlorite,
and sodium hypochlorite were purchased from Sigma-Aldrich, Germany
and used as received.
Preparation of the TO-Wood
Template
As shown in Scheme , a balsa wood block with a dimension of 10 ×
10 × 10 mm3 was delignified with 1 wt % sodium chlorite
in sodium acetate
buffer (pH 4.6) at 80 °C for 12 h. The delignified wood was then
oxidized with a TEMPO/NaClO2/NaClO system at pH 6.8 for
48 h following the method reported in our previous work.[31] After TEMPO-mediated oxidation, the wood blocks
were further washed in an ethanol/water mixture (1:1, v/v) to remove
residue chemicals and minimize swelling in water, producing the TO-wood.
Scheme 1
Schematic Diagram of the Synthesis Procedure for the Foam-like TO-Wood/MOF
Composite Using Copper Benzene-1,3,5-tricarboxylate [Cu3(BTC)2]
Synthesis
of TO-Wood/MOF Composites
The in situ synthesis of copper
benzene-1,3,5-tricarboxylate [Cu3(BTC)2] in
TO-wood was carried out in one pot (Scheme ). The wet TO-wood
samples (150 mg dry mass) were preincubated in 50 mL of 95% (v/v)
ethanol containing 0.145 mol L–1 Cu(NO3)2·(H2O)3 for 3 h to
allow the adsorption of the Cu2+ ion. Subsequently, the
organic ligand (H3BTC, 0.08 mol L–1)
was added into the incubation solution and kept at 80 °C overnight
to produce the TO-wood/Cu3(BTC)2 composite.
The molar ratio between Cu2+ and H3BTC and their
concentration in ethanol were adopted from a previously reported synthesis
method for TO-CNF/MOF aerogel.[27] The total
reaction volume was chosen to ensure that the wood samples were completely
submerged in ethanol in order to achieve a rather homogeneous growth
of MOFs inside the wood template. Thus, an excessive amount of Cu2+ (more than 50 times higher than the amount of carboxylate
in TO-wood) was applied. Following the above procedure and strategy,
0.2 mol L–1 Al(NO3)3 and 0.2 mol L–1 H3BTC were used to
prepare the TO-wood/aluminum benzene-1,3,5-tricarboxylate (AlBTC)
composite.[18] For the synthesis of TO-wood/zinc
2-methylimidazolate [Zn(MeIm)2] composite, 0.08 mol L–1 Zn(NO3)2·(H2O)6 and 1.6 mol L–1 2-methylimidazole
were used for the synthesis.[24] The above
as-prepared TO-wood/MOF composites were washed thoroughly with methanol
and dried with supercriticalCO2 to obtain the respective
composites. Delignified wood/MOF composites were also prepared using
the same procedure for comparison. For neat MOF synthesis, an identical
method was used in the absence of TO-wood. After the synthesis, suspensions
of neat MOFs were washed with methanol several times to remove unreacted
chemicals and then dried under vacuum.
Characterizations
The microstructure
of the composites was studied by using field emission-scanning electron
microscopy (FE-SEM, S-4800, Hitachi, Japan). The cross section perpendicular
to the fiber axial direction was trimmed with a sliding microtome
(Leica SM2010 R) prior to synthesis for ease of observation. The cross
section parallel to the fiber axial direction was observed on the
interior of the peeled open TO-wood/MOF composites. Fourier transform
infrared (FT-IR) spectra were recorded on a Spectrum 100 FT-IR Spectrometer
(PerkinElmer, USA). X-ray diffraction (XRD) patterns were obtained
on a PANalytical X’Pert PRO powder diffractometer (Malvern
Panalytical, UK) equipped with a Cu Kα source. N2 physisorption test was carried out on 3Flex (Micromeritics, USA).
The specific surface area was measured from the adsorption isotherm
in the relative pressure range between 0.01 and 0.2 according to the
Brunauer–Emmett–Teller (BET) method. The mass contents
(wt %) of copper, aluminum, and zinc in the composites were measured
with an inductively coupled plasma–optical emission spectroscopy
(ICP–OES) method by a Thermo Scientific iCAP 600 series instrument.
Prior to ICP–OES measurements, 0.1 g of dry powder of each
sample was hydrolyzed with 72% (w/w) H2SO4 assisted
with an autoclave. Typical wavelengths were used to determine the
concentration of Cu: 204.3 nm, 219.9 nm, and 224.7 nm; Al: 308.2,
394.4, and 396.1 nm; and Zn: 202.5, 206.2, and 213.8 nm. The average
concentration obtained at different wavelengths was taken for the
evaluation of MOF loading contents in the composites. Thermal stability
of dried neat MOFs and the TO-wood/MOF composites was measured on
a Mettler Toledo TGA/DSC1 (Switzerland). Samples were heated from
50 to 800 °C under a nitrogen atmosphere at a heating rate of
10 °C min–1. Gravimetric CO2 adsorption
capacity and temperature swing cyclic CO2 adsorption/desorption
test were carried out on a thermogravimetric analysis (TGA) instrument
(Discovery TGA, TA instruments Co. Ltd., America) equipped with both
CO2 and N2 gas tanks at atmospheric pressure.
The sample was first outgassed under a N2 flow at 105 °C
for 1 h to drive out adsorbed CO2 and then cooled down
to 25 °C. The CO2 adsorption process was then carried
out in a CO2 flow at 25 °C for 150 min. Cyclic adsorption/desorption
was performed by repeating the abovementioned two steps. The compression
test was performed on a universal mechanical tester (Instron-5566,
Instron, USA) equipped with a 10 kN loading cell at a strain rate
of 10% min–1, 23 °C, 50% relative humidity.
Elastic modulus was determined from the initial linear deformation
region of stress–strain curves.
Results
and Discussion
Synthesis of the TO-Wood/MOF
Composites
Through TEMPO-mediated oxidation in neutral condition,
C6 hydroxyls
on the surface of cellulose microfibrils in the delignified wood cell
wall were selectively oxidized to carboxyl groups. To avoid extensive
fibrillation during the washing step and maintain the structural integrity
of the natural wood structure, the TO-wood sample was washed in an
ethanol/water mixture (1:1. v/v) after the TEMPO oxidation. The content
of carboxyl groups in the TO-wood was 0.66 mmol g–1 as determined by conductometric titration. FE-SEM revealed that
the cross-sectional surface perpendicular to the fiber axial direction
of TO-wood showed a honeycomb-like cellular structure similar to native
balsa wood, indicating good structural integrity (Figure a).[32] The hexagonal cells were slightly transformed into a round shape
due to the reduced cell wall rigidity.[31] Mesopores (2–50 nm) and macropores (>50 nm) were observed
in the cell wall of TO-wood (Figure b). N2 adsorption/desorption isotherms of
TO-wood showed a combination of type II and IV isotherms,[33] with a type H3 hysteresis loop and no limiting
adsorption at high p/p0 (Figure a), indicating
the presence of both macro- and mesoporous structures with slit-like
pores, similar to the TO-CNF/silica aerogel.[34] The BET specific surface area (SBET)
of the TO-wood was 172 m2 g–1 (Table
S1, Supporting Information), about 30%
lower than that reported in our previous work (249 m2 g–1).[31] This is due to the
lack of extensive washing step with water, which limited the separation
of individualized cellulose microfibrils and swelling of the cell
wall.
Figure 1
FE-SEM micrographs of the surfaces perpendicular (cross section)
and parallel (cell wall surface) to the fiber axial direction for
(a,b) TO-wood and (c,d) TO-wood-Cu2+.
Figure 2
N2 adsorption/desorption isotherms of (a) TO-wood, TO-wood
adsorbed with Cu2+ (TO-wood–Cu2+), TO-wood/Cu3(BTC)2 composite, and neat Cu3(BTC)2 and (b) neat AlBTC, TO-wood/AlBTC composite, neat Zn(MeIm)2, and TO-wood/Zn(MeIm)2 composite samples.
FE-SEM micrographs of the surfaces perpendicular (cross section)
and parallel (cell wall surface) to the fiber axial direction for
(a,b) TO-wood and (c,d) TO-wood-Cu2+.N2 adsorption/desorption isotherms of (a) TO-wood, TO-wood
adsorbed with Cu2+ (TO-wood–Cu2+), TO-wood/Cu3(BTC)2 composite, and neat Cu3(BTC)2 and (b) neat AlBTC, TO-wood/AlBTC composite, neat Zn(MeIm)2, and TO-wood/Zn(MeIm)2 composite samples.The in situ synthesis of MOFs using the wood cell
wall as the template
was carried out in one pot, and TO-wood was first incubated with Cu2+ to form the TO-wood–Cu2+ complex (TO-wood–Cu2+) through chelation. To characterize the TO-wood adsorbed
with Cu2+, the sample was collected, washed with methanol,
and dried by supercritical drying. The adsorbed amount of Cu2+ in TO-wood was 1.23 mmol/g, as measured by ICP–OES. This
value is higher than the carboxylate content of TO-wood, indicating
the unspecific binding of Cu2+ ion to cellulose, as reported
previously.[35] The ionic crosslinking of
carboxylated cellulose microfibrils in TO-wood cell wall with divalent
Cu2+ has led to a well-preserved native cellular structure
(Figure c). Interconnection
of microfibril bundles through thin fibrils was observed from the
FE-SEM micrograph of the cell wall surface (Figure d). The SBET of
the TO-wood–Cu2+ sample was increased to 197 m2 g–1 (Table S1) with the mesoporous type IV isotherms preserved (Figure a). This is due to the introduction
of multivalent ions that strengthened the interfibrillar interaction
between cellulose microfibrils, and thus, aggregation of cellulose
microfibrils and collapse of the cellulose network during supercriticalCO2 drying were minimized. A similar effect was also reported
for the TO-CNF network, in which the SBET of TO-CNF xerogel increased from 340 to 410 m2 g–1 after crosslinking with Al3+.[36]The never-dried TO-wood was preincubated
with Cu2+ for
3 h, and the organic ligand H3BTC was then added in the
same pot and kept at 80 °C overnight. Thus, Cu3(BTC)2 was synthesized in situ inside the TO-wood structure. After
washing with methanol and drying with supercriticalCO2, the foam-like TO-wood/Cu3(BTC)2 composite
with an uniform turquoise color intrinsic to Cu3(BTC)2[37] was obtained. The loading of
Cu3(BTC)2 in the composite was 44.2 wt %, as
calculated from the copper mass content measured by ICP–OES.
The N2 adsorption/desorption isotherm of the composite
(Figure a) showed
a typical type I isotherm for microporous solid with small external
surface,[33] which was contributed by the
highly microporous Cu3(BTC)2. Neat Cu3(BTC)2 exhibited a high SBET of 1368 m2 g–1 (Table S1). After the in situ growth of Cu3(BTC)2 in TO-wood, a high SBET value
of 471 m2 g–1 was obtained for the TO-wood/Cu3(BTC)2 composite. As a comparison, the delignified
wood/Cu3(BTC)2 composite showed a SBET value of 136 m2 g–1 (Figure
S1, Supporting Information) due to the
much lower loading of Cu3(BTC)2 crystals (10.0
wt %) (Table S1).In addition to Cu2+, the carboxyl
groups in the TO-wood
template can easily chelate with a series of multivalent ions including
Al3+, Pb2+, Ba2+, Mg2+, Ca2+, Fe3+, Zn2+, and so forth.[27,38−40] Thus, besides
Cu3(BTC)2, in situ syntheses of Zn(MeIm)2 and AlBTC in TO-wood were also successfully performed via
a similar procedure using different metal salts and organic ligands.
Structure of the TO-Wood/MOF Composites
The FT-IR spectra of TO-wood/Cu3(BTC)2, TO-wood/Zn(MeIm)2, TO-wood/AlBTC composites, neat TO-wood, and corresponding
neat MOFs are compared in Figure a. All TO-wood/MOF composites showed an absorption
peak of C=O stretching vibration mode at 1730 cm–1 originated from the hemicellulose in TO-wood.[31] The band appeared at 1645 cm–1 in all
three composites can be attributed to the following: (1) the asymmetric
stretching vibration of carboxylate from BTC chelating with Cu2+ and Al3+ or (2) the C=C stretching vibration
mode of the imidazole ring in Zn(MeIm)2, which were identified
in the spectra of neat MOFs but not in the spectrum of neat TO-wood.[41−43] The symmetric vibration peak of the carboxyl group of TO-wood in
the carboxylate form shifted from 1605 cm–1 in neat
TO-wood to around 1580–1570 cm–1 in the composite
due to its chelation with multivalent metal ions.[24,44,45] In addition, peaks at 729 and 759 cm–1 in all three TO-wood/MOF composites were assigned
to the out-of-plane bending vibrations of the ring structure in either
BTC or 2-methylimidazole, which were also observed for neat MOFs.[42,46] Besides, the peak at 1147 cm–1 was attributed
to the ring C–N stretching that is associated with 2-methylimidazole
in Zn(MeIm)2.[47] A unique band
at 770 cm–1 emerged in the IR spectrum of TO-wood/AlBTC
was related to the formation of the Al3+–COO– chelation complex.[28,48]
Figure 3
(a) FTIR spectra
and (b) XRD patterns of neat MOFs, neat TO-wood,
and various TO-wood/MOF composites.
(a) FTIR spectra
and (b) XRD patterns of neat MOFs, neat TO-wood,
and various TO-wood/MOF composites.The successful synthesis of MOFs was also confirmed by XRD analysis.
Both neat TO-wood and TO-wood/MOF composites showed two broad peaks
centered at 2θ = 14.8–16.8 and 22.5° (Figure b), corresponding to the diffraction
of (11̅0), (110), and (200) planes of cellulose I crystals,
respectively. In addition, peaks at 2θ = 5.9, 6.8, 9.7, 11.9,
13.8, 17.8, and 19.4° in TO-wood/Cu3(BTC)2 and neat Cu3(BTC)2 (Figure b) were the characteristic peaks of regular
(111), (200), (220), (222), (400), (333), and (440) planes of Cu3(BTC)2, respectively.[24,49,50] Peaks at 2θ = 7.2, 13.0, 16.8, and
18.4° that can be attributed to (110), (211), (310), and (222)
planes of Zn(MeIm)2 were also identified for both TO-wood/Zn(MeIm)2 and neat Zn(MeIm)2.[24,27] The characteristic
peaks of AlBTC were difficult to be identified in TO-wood/AlBTC except
for the weak and broad peak at 2θ = 11.0°. This was due
to the large structural diversification typical for micro- and mesoporousAlBTC, showing broad and weak diffraction patterns for neat AlBTC.[18] A similar XRD pattern has been previously reported
when the synthesis of AlBTC was carried out in the presence of ethanol,
where mainly the MIL-100 phase was formed.[51−53] Compared to
the simulated XRD pattern of MIL-100 (Figure S2, Supporting Information), the major broad peaks in the patterns
of as-synthesized AlBTC and TO-wood/AlBTC composite were shown to
closely relate to MIL-100 crystals. These results suggested that the
chelation of carboxyl groups of TO-wood with multivalent ions substantially
enhanced the nucleation and in situ growth of MOFs homogeneously
inside TO-wood.[28]Indeed, all three
types of MOFs were homogeneously synthesized
inside the TO-wood cell wall, leaving the lumen spaces empty for efficient
mass conduction, as observed from the cross-sectional surfaces perpendicular
to the fiber axial direction of the composites by FE-SEM (Figure a–c). The
major difference was the localization and distribution of different
MOF crystals due to their sizes. Image analysis revealed that the
crystal sizes of Cu3(BTC)2, Zn(MeIm)2, and AlBTC were in the range of 0.5–5 μm, 0.5–2
μm, and 20–100 nm, respectively (Figure S3, Supporting Information). The Cu3(BTC)2 crystals were found in both inner lumen surface and intercellular
region (middle lamella) (Figure a). The Zn(MeIm)2 crystals were embedded
partially in the inner lumen cell wall (Figure b). On the other hand, the AlBTC crystals
were much smaller and mainly in the form of agglomerated conformation
(Figure c). The TO-wood
cell wall was monolithically and homogeneously covered with nanoscale
AlBTC crystals.
Figure 4
FE-SEM micrographs of low (×600) and high (×10k)
magnifications
showing the cellular structure and cell wall corner region in the
cross-sectional surfaces perpendicular to the fiber direction and
the cell wall surfaces parallel to the fiber axial direction for (a,d)
TO-wood/Cu3(BTC)2, (b,e) TO-wood/Zn(MeIm)2, and (c,f) TO-wood/AlBTC composites, respectively. The inset
photographs show the physical appearance of the composites.
FE-SEM micrographs of low (×600) and high (×10k)
magnifications
showing the cellular structure and cell wall corner region in the
cross-sectional surfaces perpendicular to the fiber direction and
the cell wall surfaces parallel to the fiber axial direction for (a,d)
TO-wood/Cu3(BTC)2, (b,e) TO-wood/Zn(MeIm)2, and (c,f) TO-wood/AlBTC composites, respectively. The inset
photographs show the physical appearance of the composites.The distribution of MOFs within the wood structure
was further
characterized on interior surfaces of composites parallel to the fiber
direction. The samples were peeled to expose the cell wall surface
of the fiber cells inside the composites and observed by FE-SEM (Figure d–f). The
Cu3(BTC)2 crystals were grown on the entire
surface of fiber cells of TO-wood (Figure d). FE-SEM micrograph with higher magnification
for the cross section of the TO-wood/Cu3(BTC)2 composite revealed that cellulose microfibrils were attached on
the surface of Cu3(BTC)2 crystals that were
grown inside the cell wall (Figure S4, Supporting Information), indicating the coordination between TO-wood and
Cu3(BTC)2.[28] The
distribution of Zn(MeIm)2 crystals was rather heterogeneous
and scattered along the fiber cell surface with large cell wall surface
areas exposed (Figure e). The particle size of AlBTC crystals was below 100 nm and AlBTC
nanocrystals were embedded in the cellulose microfibril network (Figure f). The reason for
high loading of Cu3(BTC)2 (44.2 wt %) in TO-wood
can be attributed to the higher affinity of Cu2+ to the
C6 carboxyl groups of TO-CNFs compared to Zn2+.[35] Therefore, more metal ions were adsorbed and
served as nucleation sites for the synthesis of MOFs. Indeed, the
adsorbed amount of Zn2+ to TO-wood was 0.31 mmol/g, as
measured by ICP–OES, much lower than that for Cu2+ (1.23 mmol/g). Thus, it resulted in a lower loading of Zn(MeIm)2 in the composite (11.3 wt %). Interestingly, the adsorbed
amount of Al3+ to TO-wood was 0.30 mmol/g, but the loading
of AlBTC crystals in the composites was remarkably high (42.7 wt %).
This is probably due to the reason that an excess amount of AlBTC
was synthesized in the bulk solution and trapped inside the cell wall
because of its small particle size (20–100 nm). The TO-wood/Zn(MeIm)2 and TO-wood/AlBTC composites also showed enhanced BET surface
areas of 92 and 361 m2 g–1 (Figure b and Table S1) as compared to 37 and 38 m2 g–1 for delignified wood/Zn(MeIm)2 and
delignified wood/AlBTC (Figure S1 and Table S1), respectively. The higher loading of MOFs and large surface area
thus can endow TO-wood/MOF composites with competitive CO2 adsorption performance.The decomposition behavior of the
TO-wood/MOF composites was studied
by TGA. As shown in Figure , the decomposition of TO-wood started at around 240 °C
due to the thermal degradation of cellulose. The structural decomposition
of neat Cu3(BTC)2 took place at a higher temperature,
in the range of 320–400 °C, after a first stage of water
evaporation (∼100 °C) and a second stage of decomposition
of low-quality crystals (∼220 °C).[54] The TO-wood/Cu3(BTC)2 composite showed
an enhanced thermal stability as compared to TO-wood. It showed two
main decomposition stages at 270–330 and 330–370 °C
due to the decomposition of TO-wood and Cu3(BTC)2, respectively. Similarly, the incorporation of Zn(MeIm)2 and AlBTCalso improved the thermal stability of TO-wood. Neat Zn(MeIm)2 is highly thermally stable and showed a profile of nearly
constant weight up to 570 °C. The in situ growth of Zn(MeIm)2 in TO-wood led to the increase of the initial decomposition
temperatures of TO-wood/Zn(MeIm)2 to 250 °C. Neat
AlBTC showed a multistage decomposition profile in the range of 275–650
°C. Compared to TO-wood, the decomposition of TO-wood/AlBTC started
at a higher temperature of 255 °C, with a second decomposition
stage in the range of 320–620 °C due to the high loading
of AlBTC in the composite.
Figure 5
(a) Thermogravimetric curves and (b) corresponding
first derivative
weight loss curves of neat MOFs, TO-wood, and the TO-wood/MOF composites.
(a) Thermogravimetric curves and (b) corresponding
first derivative
weight loss curves of neat MOFs, TO-wood, and the TO-wood/MOF composites.
CO2 Adsorption/Desorption
Performance
CO2 adsorption/desorption isotherms
of neat wood template,
neat MOFs, and TO-wood/MOF composites were recorded using TGA equipped
with gas tanks containing pure dry CO2 and N2, respectively. The adsorption of CO2 was performed at
25 °C and atmospheric pressure after an initial drying with N2 at 105 °C. Moreover, desorption was conducted right
after adsorption with a constant flow of N2 at 105 °C.
Neat Cu3(BTC)2MOFs exhibited the highest CO2 adsorption capacity of 2.49 mmol g–1, which
is equivalent to 11.0 wt % CO2 uptake (Figure a). This is consistent with
the previously reported result that the maximum CO2 adsorption
to Cu3(BTC)2 at 295 K and 0.1 MPa was 2.46 mmol
g–1 through physical trapping of CO2 molecules.[55] Neat TO-wood also showed a CO2 adsorption
capacity of 0.2 mmol/g, which was caused by the binding of CO2 to the carboxyl group through dipolar interaction.[56] As a result of in situ growth of MOFs inside
TO-wood, the TO-wood/Cu3(BTC)2 composite showed
a high CO2 adsorption capacity of 1.46 mmol g–1. Cu3(BTC)2 contains coordinatively unsaturated
metal sites for CO2 adsorption, which is greatly beneficial
when used for cyclic CO2 adsorption.[57] This enables Cu3(BTC)2 to be the
favored MOF material for CO2 capture and storage. On the
contrary, the CO2 adsorption capacities of neat Zn(MeIm)2 and AlBTC at 25 °C and atmospheric pressure were 0.30
and 0.87 mmol g–1, about 8 and 3 times lower than
that of neat Cu3(BTC)2. These results were in
line with the literature result where ZIF-8 showed CO2 capacity
around 0.4 mmol g–1 at 25 °C and 1 bar.[58] Therefore, the TO-wood/Zn(MeIm)2 and
To-wood/AlBTC composites showed lower CO2 adsorption capacities
of 0.25 and 0.43 mmol g–1, respectively.
Figure 6
(a) CO2 adsorption/desorption isotherms of neat MOFs,
neat TO-wood, and various TO-wood/MOF composites. (b) Temperature
swing cyclic CO2 adsorption/desorption isotherms of the
TO-wood/Cu3(BTC)2 composite (adsorption under
CO2 at 25 °C and desorption under N2 at
105 °C).
(a) CO2 adsorption/desorption isotherms of neat MOFs,
neat TO-wood, and various TO-wood/MOF composites. (b) Temperature
swing cyclic CO2 adsorption/desorption isotherms of the
TO-wood/Cu3(BTC)2 composite (adsorption under
CO2 at 25 °C and desorption under N2 at
105 °C).The CO2 adsorption
capacities and conditions of several
wood- or cellulose-based sorbents are summarized in Table . At ambient condition, the
CO2 adsorption capacity of TO-wood/Cu3(BTC)2 in this work is superior to that of the wood- or cellulose-based
CO2 sorbents loaded with PEI,[59] acetylated CNCs,[60] and zeolite[61] and is comparable to that of the APTES-grafted
TO-CNFs/silica aerogels.[34] Although the
TO-CNFs/PEI foam showed a high CO2 adsorption capacity
of 2.22 mmol g–1 at 80% RH, contribution from water
is negligible. The same material tested at a lower humidity of 20%
RH showed only one-fourth of its maximum capacity.[62] Moreover, CO2 sorption sites, primarily amine
groups, in amine-grafted sorbents are often gradually deactivated
after the cyclic regeneration process, that is, thermal-driven desorption
at higher temperature.[62−64] As a consequence, the maximum CO2 capacity
of TO-CNFs/PEI foam decreased 27% after five cycles of adsorption/desorption
at 25 and 85 °C.[62] 7% capacity loss
after 10 cycles was also reported on PEI crosslinked cellulose triacetate
aerogel when desorption was conducted at 105 °C.[65] MOFs are generally thought as thermally stable with thermal
decomposition temperatures higher than 300 °C.[66] To have a better understanding of the reversibility and
thermal stability of CO2 adsorption by the TO-wood/Cu3(BTC)2 composite, cyclic CO2 adsorption/desorption
test was performed. The CO2 adsorption capacity during
the first cycle was 1.46 mmol g–1. After six cycles
of adsorption/desorption at 25 and 105 °C, 1.47 mmol g–1 CO2 capacity was measured (Figure b), demonstrating the excellent multicycle
durability.
Table 1
CO2 Adsorption Capacity
of Various Wood- or Cellulose-Based CO2 Sorbents
capacity mmol g–1
pressure
temperature
(°C)
humidity
TO-wood/Cu3(BTC)2
1.46
atmospheric
pressure
25
dry
delignified wood/PEI[59]
1.11
atmospheric pressure
25
dry
CNFs/acetylated CNCs[60]
1.14
101 kPa
0
dry
TO-CNFs/gelatin/zeolite[61]
∼1.3
750 mmHg
35
dry
TO-CNFs/silica/APTES[34]
1.49
atmospheric pressure
25
dry
TO-CNFs/PEI[62]
2.22
ambient
25
80% RH
TO-CNFs/PEI[62]
0.5
ambient
25
20% RH
Compressive Mechanical
Properties
Typical compressive stress–strain curves
of the TO-wood/Cu3(BTC)2 composites and TO-wood
are shown in Figure . The TO-wood/Cu3(BTC)2 composite and TO-wood
had low densities
of 107.4 ± 5.5 and 61.1 ± 4.3 kg m–3,
respectively. When the loading was parallel to the fiber axial (longitudinal)
direction, both TO-wood/Cu3(BTC)2 composite
and TO-wood showed initial linear elastic deformation with rapid increase
of compressive stress at compressive strain lower than 2% (Figure a). After the yielding
point, both materials showed plastic deformation plateaus at moderate
strain before entering a final densification phase, during which the
stress increased exponentially. The deformability of TO-wood/Cu3(BTC)2 was considerably better than those of inorganic
monolithic sorbents since no catastrophic failure of materials was
observed, demonstrating good mechanical integrity. Compared to neat
TO-wood, the elastic modulus of the TO-wood/Cu3(BTC)2 composite was increased from 125.4 ± 26.2 to 326.2 ±
7.5 MPa, indicating the positive effect of ionic crosslinking by Cu2+ on the stiffness of the TO-wood template, which was also
reported on the TO-CNF hydrogel crosslinked with multivalent ions.[36] The yield strain of the TO-wood/Cu3(BTC)2 composite was about 3.5%, higher than 2.2% for
TO-wood, which is owing to the enhanced energy dissipation with the
addition of MOFs. The compressive yield strength of the TO-wood/Cu3(BTC)2 composite was 7.3 ± 0.1 MPa, 3 times
higher than that of the neat TO-wood (2.4 ± 0.4 MPa). This is
due to (1) the crosslinking effect of Cu2+, which led to
the improved resistance to yield the TO-wood/Cu3(BTC)2 composite, and (2) the reinforcing effect of MOFs on the
TO-wood/Cu3(BTC)2 composite through a strong
interfacial interaction with the TO-wood cell wall, which was also
reported for the ZIF-8 reinforced wood composite.[24]
Figure 7
Typical compressive stress–strain curves of the TO-wood/Cu3(BTC)2 composite and TO-wood with the loading (a)
parallel to the fiber axial direction, i.e., longitudinal direction
and (b) perpendicular to the fiber axial direction, i.e., transverse
direction. The insets are the corresponding stress–strain curves
in the strain range of 0–10%.
Typical compressive stress–strain curves of the TO-wood/Cu3(BTC)2 composite and TO-wood with the loading (a)
parallel to the fiber axial direction, i.e., longitudinal direction
and (b) perpendicular to the fiber axial direction, i.e., transverse
direction. The insets are the corresponding stress–strain curves
in the strain range of 0–10%.Due to the inherent anisotropy of wood, TO-wood/Cu3(BTC)2 showed different deformation behaviors in the transverse
direction (Figure b). Both TO-wood/Cu3(BTC)2 composite and TO-wood
showed good compressibility. The TO-wood/Cu3(BTC)2 composite showed a short linear elastic region up to a compressive
strain of 5%, followed by a stress plateau in the range of 5–60%
compressive strain, in which the cell wall was collapsed gradually.[67] Thereafter, a rapid densification region appeared,
indicating the elimination of cell wall porosity. Similar compressive
stress–strain behavior was also reported for the ultralight
TO-CNF/MIL-53 aerogel.[28] The elastic modulus
and yield strength of the TO-wood/Cu3(BTC)2 composite
were 3.5 ± 0.4 and 0.20 ± 0.04 MPa, respectively, which
are still considerably high. As a comparison, the neat TO-wood barely
showed a yielding phenomenon and was gradually densified as the compressive
strain increased to 90%, with a 10 times lower elastic modulus recorded
at 0.36 ± 0.05 MPa.The mechanical properties of the TO-wood/Cu3(BTC)2 composite were exceptional as compared with
various monolithic
CO2 sorbents summarized in Table . Although the compressive elastic modulus
and yield strength of the TO-wood/Cu3(BTC)2 composite
in the axial direction were ca. 40% of those of the
delignified wood/PEI composite,[59] the density
of TO-wood/Cu3(BTC)2 was only 30% of that of
delignified wood/PEI (343.6 ± 15.3 kg m–3).
The specific elastic modulus (Es: 3034
kN m kg–1) and specific yield strength (σs: 68 kN m kg–1) of TO-wood/Cu3(BTC)2 in the axial direction were remarkably high. These
values were also higher than those for cellulose-based CO2 sorbents such as APTES-grafted TO-CNF/silica aerogel,[34] anisotropic CNF aerogel impregnated with acetylated
CNC,[60] and anisotropic foam of TO-CNFs/gelatin/zeolite.[61] Moreover, in comparison to MOF-loaded monolithic
CO2 sorbents, the TO-wood/Cu3(BTC)2 composite was 2 orders of magnitude stronger than the graphene/ZIF-8
aerogel[22] and 3D-printed MOF/clay/PVA monoliths,[19] suggesting TO-wood as a much more robust template
for structuring MOFs into a monolith than using an inorganic substrate
or polymer-based binders.
Table 2
Compressive Mechanical
Performance
of Various CO2 Monolithic Sorbentsa
test direction
elastic modulus
(MPa)
yield strength
(MPa)
specific
elastic modulus (kN m kg–1)
specific
yield strength (kN m kg–1)
TO-wood/Cu3(BTC)2
axial
326.2 (7.5)
7.3 (0.1)
3034
68
TO-wood/Cu3(BTC)2
transverse
3.5
(0.4)
0.20 (0.04)
33
2
delignified wood/PEI[59]
axial
756
18
2200
52
CNF/silica aerogel[34]
isotropic
0.18
0.03
22
4
CNF/acetyl-CNCs aerogel[60]
axial
0.30
0.02
20
2
TO-CNFs/gelatin/zeolite[61]
axial
2.2
147
Graphene/ZIF8 aerogel[22]
isotropic
0.28
0.02
12
1
PVA/clay/MOF-74(Ni)[19]
axial
12
0.48
13
0.5
PVA/clay/UTSA-16(Co)[19]
axial
25
0.55
15
0.3
The values in parentheses
are the
sample standard deviations.
The values in parentheses
are the
sample standard deviations.
Conclusions
In summary, foam-like TO-wood/MOF
composites were successfully
prepared by the in situ synthesis of Cu3(BTC)2, Zn(MeIm)2, and AlBTC in a TO-wood template. The surface
carboxyl group on the cellulose microfibrils in the TO-wood facilitated
the interfacial coordination of multivalent metal ions and subsequent
MOF nucleation and growth in the wood cell wall. The TO-wood/Cu3(BTC)2 composite had a high loading (44.2 wt %)
of Cu3(BTC)2, a large BET surface area of 471
m2 g–1, and a high CO2 adsorption
capacity of 1.46 mmol g–1 at 25 °C and atmospheric
pressure, higher than those for the TO-wood/Zn(MeIm)2 and
TO-wood/AlBTC composites. Besides, the TO-wood/Cu3(BTC)2 composite maintained the maximum capacity during the temperature
swing cyclic CO2 adsorption test, demonstrating good multicycle
durability. Moreover, the TO-wood/Cu3(BTC)2 composite
was exceptionally strong in the longitudinal direction (fiber axial)
with a remarkably high specific elastic modulus of 3034 kN m kg–1 and a high specific yield strength of 68 kN m kg–1 ever reported for solid CO2 sorbents.
This study introduced a facile strategy to address the interfacial
coordination of MOFs to the wood cell wall and significantly increased
the loading of MOFs in the wood structure and therefore achieved the
foam-like composites combining the versatile functionalities of MOFs
and the mechanical robustness of wood. The TO-wood/MOF composites
are also promising for various possible applications in environmental
remediation, gas separation and purification, insulation, and catalysis
and will be further investigated in the future.