Jian
Liu
*a,
Tong
An
b,
Zhihan
Chen
b,
Zizhao
Wang
b,
Han
Zhou
*b,
Tongxiang
Fan
b,
Di
Zhang
b and
Markus
Antonietti
*c
aKey Laboratory of Green Printing, Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100190, P. R. China. E-mail: liujian@iccas.ac.cn
bState Key Lab of Metal Matrix Composites, Shanghai Jiaotong University, Shanghai, 200240, P. R. China. E-mail: hanzhou_81@sjtu.edu.cn
cDepartment of Colloid Chemistry, Max Planck Institute of Colloids and Interfaces, Potsdam 14424, Germany. E-mail: markus.antonietti@mpikg.mpg.de
First published on 24th April 2017
Graphitic carbon nitride (g-C3N4) has emerged as an active visible-light-driven photo(electro)catalyst. However, the rediscovery of g-C3N4 has also spurred enormous interest in other, very versatile applications beyond catalysis. Herein, graphitic carbon nitride nanosheets could be used as photocatalytic initiators and cross-linking sites for the temperature responsive poly(N-isopropylacrylamide) hydrogel without any sacrificial agents or co-initiators. A prototype of a temperature controlled smart window based on the hydrogel composite was made by coating the hydrogel composite onto glass. It is believed that the combination of g-C3N4 chemistry and conventional hydrogel or polymer chemistry can lead to further promising applications.
Graphitic carbon nitride (g-C3N4) features a more suitable bandgap of 2.7 eV and is thereby capable of being excited by visible light.12 It has emerged rapidly and established its role as a highly active visible-light-driven photo(electro)catalyst for hydrogen evolution and even overall water splitting.12–27 In the meanwhile, the rediscovery of g-C3N4 has also spurred enormous interest in other, very versatile applications beyond catalysis.28–32 In particular, g-C3N4 based composites are made by coupling it with a variety of oxides and sulfides or with pure metals and graphene, which opened additional possibilities for exploratory applications.27 Few studies have been reported on g-C3N4/polymer composites, and only in a couple of cases has its application as a visible-light-driven photoinitiator been explored.33,34 Yagci in his pioneering work reported one of the few clear cases of mesoporous g-C3N4 as a heterogeneous visible light photoinitiator for radical polymerization, however relying on amines as co-initiators.33 The amine co-initiators in these experiments were indispensable for polymerization. Woźnica et al. found out that mesoporous g-C3N4 was an efficient heterogeneous photocatalyst for the radical cyclization of 2-bromo-1,3-dicarbonyl compounds to functionalized cyclopentanes under mild conditions.34 Tetrahydrofuran played the dual role of solvent and a crucial proton and electron donor in this study. In these two cases, triethanolamine or tetrahydrofuran was needed as the sacrificial agent or co-initiator to terminate the light-driven radical initiation step, which we want to avoid here for some practical applications.35
In this work, we demonstrate that the exfoliated layered g-C3N4 nanosheets (abbreviated to CNSs) themselves under visible light illumination can directly initiate the radical polymerization and crosslinking of N-isopropylacrylamide (abbreviated to NIPAm) monomers in aqueous solution, generating a thermoresponsive hydrogel without involving any co-initiators. The well-dispersed CNSs – due to multisite binding – act as a crosslinker in the final hydrogel which also enhances its mechanical strength. The hydrogel composite could serve as a prototype of a temperature controlled smart window coating based on the reversible thermal response around the lower critical solution temperature. The combination of g-C3N4 chemistry and conventional hydrogel or polymer chemistry suggests promising applications.
In a typical polymerization experiment, 10 wt% of NIPAm was dissolved in the CNS colloidal solution (0.03 wt%), which was then irradiated with visible light emitted from a xenon lamp equipped with a 420 nm cutoff filter. The molecular structure of NIPAm and the tri-s-triazine structure of g-C3N4 as the building block are illustrated in Fig. S2 of the ESI.† The NIPAm-containing CNS colloidal solution is depicted in Fig. 1b. Upon exposure to visible light, the solution started to turn viscous and finally gelated after 50 minutes under static conditions, as illustrated by the upside-down tube in Fig. 1c. The translucent character was retained and was almost the same as that of the starting solution. In the control experiment, the NIPAm solution without CNSs could not be crosslinked to the gel even after prolonged illumination, which suggested the indispensable role of CNSs in initiating and cross-linking the polymer chains. UV light was also employed to induce polymerization, as shown in Fig. S3 of the ESI.† However, further tests with bulk g-C3N4 and mesoporous g-C3N4 didn't give satisfactory gelation results, due to the missing colloidal character in these two cases avoiding the connection between the single carbon nitride entities which are macroscopic. The morphologies of the composite gel after supercritical CO2 drying and freeze drying were investigated. In the SEM experiments (Fig. S4 of the ESI†), no structural features of CNSs could be identified, which was thought to be due to the tight embedding of the CNSs and binding in the gel network. The schematic illustration of the hydrogelation process is depicted in Fig. 1d. The electrostatic repulsion within the negatively charged carbon nitride framework maintained the distribution of CNSs in the dispersion while avoiding their agglomeration. The NIPAm/CNS dispersion was finally transformed into a hydrogel composite using visible-light-triggered in situ vinyl polymerization.
Further optimization of the polymerization conditions (such as reaction time and concentration) is the subject of current experiments. The monomer concentration and CNS concentration are determining factors of the hydrogelation of PNIPAm in this specific structure. The concentration of the NIPAAm monomer (8, 10 and 12 wt%) was first varied while maintaining the CNS concentration at 0.03 wt%. It turned out that the gelation did not occur for 8 wt% monomer concentration after 50 minutes' illumination. With 10% monomer concentration, complete gelation of the starting solution was realized after 50 minutes' illumination. Further increase of the monomer concentration to 12 wt% did not improve the gelation behavior (Fig. 2a) and the switching behavior. While maintaining the concentration of NIPAm at 10 wt%, varying the CNS concentration in the reaction solution also resulted in different gel structures (Fig. 2b). The lower the CNS concentration (0.02, 0.03, and 0.04 wt%), the longer it took to accomplish the gelation. CNS colloidal solutions with concentrations higher than 0.04 wt% appeared to be unstable under the given set of conditions. We further performed one control experiment to exclude the heating effect of the lamp during irradiation. As shown in Fig. S5,† heating alone without irradiation can't induce the gelation of the NIPAm monomer in the presence of the CNS colloidal solution, which suggested that light instead of heat is the energy source for the hydrogelation. Therefore, we choose 10 wt% NIPAm monomer concentration and 0.03 wt% CNSs in aqueous solution as standard conditions to obtain the special gel structure. It is no surprise that a macroreticular behavior is obtained both near the gelation point of the polymer network and the point of colloidal stability of the CNSs.
The rheological properties of the hydrogel composite were measured. The results of viscosity, storage modulus (G′) and loss modulus (G′′) as a function of temperature are shown in Fig. 3a. The viscosity, G′ and G′′ of the hydrogel can be seen to decrease as the temperature is increased from 15 to 29 °C. This result may be due to the viscous effects of the hydrogel with increasing temperatures. However, the viscosity, G′ and G′′ are found to increase above 29 °C, which is related to the LCST of the branched chain. When the temperature is close to the LCST of the hydrogel, the hydrogen bonding gradually decreases while the hydrophobic interactions between the molecular chains enhance, resulting in the hydrophobic and contractive chains. Excess water was discharged from the network structure. Therefore, the size of the micelles may become smaller, and viscosity and modulus begin to rise. From 10 to 60 °C, G′ is always larger than G′′, which indicates that the hydrogel tends to be an elastic solid. The LCST behavior of the hydrogel composite is investigated using a differential scanning calorimeter, as shown in Fig. 3b. Thermal analyses were performed on the swollen sample from 15 to 45 °C at a heating rate of 2 °C min−1 under a dry nitrogen atmosphere. The temperature corresponding to the endothermic peak is the LCST of the synthesized hydrogel composite. This indicates that the LCST of the hydrogel is around 29 °C, which matches with the rheological result shown above. 1H-Nuclear magnetic resonance (NMR) measurement of the PNIPAm/CNS hydrogel composite was performed (see Fig. S6 of the ESI†). The 1H-NMR spectrum of PNIPAm has the same peaks at 5.61 ppm and 6.05 ppm as that of NIPAm, suggesting that it's an incomplete reaction. Since the monomers are more soluble in D2O or DMSO-d6 than the polymers, the real conversion ratio is difficult to obtain in the current case. More quantitative characterizations and analysis will be performed to further investigate and apply the hydrogel composite to real applications.
Fig. 3 (a) Dynamic temperature ramp curves of the PNIPAm/CNS hydrogel composite. (b) Differential scanning calorimeter (DSC) thermogram of the PNIPAm/CNS hydrogel composite. |
g-C3N4 was previously employed for the photocatalytic degradation of pollutants even in the absence of sacrificial agents.39–41 In such applications, some of the photogenerated reactive oxygen species (abbreviated to ROS, including O2−˙, HO2˙ and H2O2) are regarded as the active species for decomposing the organics. The generation of ˙OH radicals by g-C3N4 under visible light irradiation was proven by various authors.36,42,43 For the elucidation of the polymerization mechanism, the involvement of ˙OH radicals in the process was corroborated by the common terephthalic acid (TA) assay.44 TA is a well-known ˙OH scavenger, generating 2-hydroxy terephthalic acid (HTA), which does not react with other ROS, such as O2−˙, HO2˙ and H2O2. When the solution containing TA and HTA molecules is irradiated by UV light (λ = 310 nm), HTA molecules emit fluorescent at λ = 425 nm, while TA molecules do not emit. As shown in Fig. 4a and b, the presence of ˙OH radicals could be confirmed, and HTA concentration increases with irradiation time. As shown in eqn (1) below, the ˙OH radical converts TA into HTA through the following reaction:45
C6H4(COOH)2 + 2˙OH → C6H3(COOH)2OH + H2O | (1) |
Under illumination, g-C3N4 could be excited to generate electrons and holes. The electrons and holes could be used for the formation of the ˙OH radical, which could initiate the polymerization of NIPAm.46 It has been reported that the potential of the photoelectron at the conduction band of CNSs at −1.1 V (potential versus the standard hydrogen electrode, abbreviated to SHE) is thermodynamically favorable to reduce O2 to form O2−˙ (E0 O2/O2−˙ = −0.33 V),47 which is possibly the first step of the sequential reduction for reactive oxygen species production. The potential of the photogenerated hole in the valence band at 1.8 V is not favorable to oxidize H2O to hydroxyl radicals ˙OH (E0 ˙OH/H2O = 2.33 V vs. the SHE).43,47 The detected ˙OH is thought to be derived from the pathway O2 → O2−˙ → H2O2 → ˙OH. The hole in the valence band of the excited g-C3N4 was thought to react with the H2O to form O2 or H2O2.14 The confirmed existence of the ˙OH radical, however, doesn't preclude the involvement of other radicals in the polymerization reaction. In the current study, the CNSs acted as the crosslinker as well as the initiator. The preliminary hydrogelation mechanism is illustrated in Fig. 4c. The hydrogelation process is divided into three key steps: (1) photocatalytic generation of a hydroxyl radical by CNSs from water; (2) in situ polymerization of vinyl monomers by the photogenerated hydroxyl radical; (3) physical crosslinking of polymer chains by CNSs via noncovalent interactions.
PNIPAm is well-known for its thermoresponsive properties with a lower critical solution temperature (LCST).48 At temperatures below the LCST, the PNIPAm hydrogel is hydrophilic and adopts a transparent swollen state.11 When the temperature increases above the LCST, the gel becomes hydrophobic and collapses. The PNIPAm/CNS composite could be easily processed into desired patterns such as a monolith disk in Fig. 5a. We can clearly observe a special LCST phenomenon with the PNIPAm/CNS composite, showing only very minor macroscopic deswelling, but a significant increase of turbidity above the LCST. At elevated temperatures (up to 40 °C), the monolith disk could transform into a white demixed state, which is only weakly macroscopically deswollen (Fig. 5b). After cooling down to room temperature, the less turbid hydrogel state was easily restored, demonstrating the fast reversibility of the PNIPAm/CNSs in this special textural state. This is attributed to a special hybrid network morphology where phase demixing occurs only on a local, micron-sized structure in a so-called macroreticular structure, while ordinary PNIPAm gels would only macroscopically deswell. For the later employed optical response this is highly wanted, as such local structural rearrangements are much faster due to the smaller length scales involved in the phase transition, i.e. switching is faster.
For better visibility of the switchable hybrid opaqueness, a mixture of the PDMS prepolymer and curing agent (Dow Corning® Sylgard 184) was poured on the ‘MPIKG’ metal mold and cured at 70 °C for 1 h. After peeling off the mold, the PDMS which has the pattern of ‘MPIKG’ was formed, demonstrating the flexibility of the composite hydrogel (Fig. 5c and d). The reversible transition from the translucent to the opaque status of the temperature-responsive PNIPAm/CNS composite with short response times can make it potentially applicable as a smart window coating (Fig. 5e and f). When the temperature increases above the LCST, the hydrogel composite turned opaque. When the temperature returns to room temperature, the hydrogel composite will recover its translucent state. The process is reversible, demonstrating the possibility to protect sensitive objects, such plants in greenhouses, from too high temperatures and peak sunlight.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ta02923c |
This journal is © The Royal Society of Chemistry 2017 |