Kirsten
Bell
a,
Yiwen
Guo
a,
Samuel
Barker
a,
Seong H.
Kim
abc and
Christian W.
Pester
*abc
aDepartment of Chemical Engineering, The Pennsylvania State University, University Park, PA 16802, USA. E-mail: pester@psu.edu
bDepartment of Materials Science and Engineering, The Pennsylvania State University, University Park, PA 16802, USA
cDepartment of Chemistry, The Pennsylvania State University, University Park, PA 16802, USA
First published on 15th May 2023
Synthesis and characterization of a multi-responsive micron-scale heterogeneous catalyst are described. The temperature-responsive monomer N-isopropylacrylamide (NIPAAm) is copolymerized with the photo-active dye fluorescein o-acrylate (FlA) via surface-initiated reversible addition–fragmentation chain transfer (SI-RAFT) polymerization at varying thicknesses (i.e., molecular weights). The resulting poly(FlA-co-NIPAAm) copolymer brushes were found to undergo a rapid structural change between 24 and 26 °C, which significantly alters the photocatalytic behavior of the incorporated fluorescein. A wastewater treatment application was implemented to study the effect between temperature and film thickness. Notably, increasing the reaction temperature above the lower critical solution temperature (LCST) increased the performance in the degradation of tetracycline hydrochloride (TC) with the thickest of the photocatalyst polymer brushes showing the most pronounced temperature response.
Photocatalysis has been explored as a viable option to leverage ultraviolet (UV) or visible light – as naturally abundant from the sun – to drive degradation of toxic chemicals and pharmaceuticals into harmless, small substances.16–19 Examples include the degradation of textile dyes, such as Rhodamine B and Methylene Blue, petroleum hydrocarbons, phenolic compounds, or the removal of heavy metal ions, antibiotics, pesticides, and other contaminants.14
While potent, transition metal and organic photocatalysts bear significant limitations that hinder their widespread adoption in wastewater treatment. Amongst these are (i) their expensive nature, (ii) limited solubility in aqueous media due to their aromatic skeletons, and (iii) challenges in their separation from the treated water.20 These constraints have motivated research into heterogeneous photocatalysts, which has become the most broadly studied method to leverage photocatalysts in wastewater treatment.13,14,16,17,20,21 For example, metal oxides (e.g. TiO2 or ZnO) composite photocatalysts have been extensively studied as in the removal of pollutants.22–30 These heterogeneous photocatalysts require high energy in the ultraviolet region to overcome a large band gap or complex synthetic route to increase their stability.21 In addition, such metal-based photocatalysts can contaminate the water treatment process, depending on their retrieval and separation method as well as corrode in an aqueous environment.31,32 Alternative approaches include nanoparticles,22 polymer networks,33 or metal organic frameworks24 (MOFs), which lead to complex separation and recovery steps and decrease recyclability efficiency.
Multi-responsive photoactive polymers are an intriguing and effective approach towards photocatalysis.20,34,35 Such systems provide tunable photocatalytic activity in response to a second stimulus – e.g., pH,36 addition of CO2,37 or temperature38 – which expands and/or contracts the catalyst-surrounding matrix or modifies its chemical environment. Proof-of-concept studies exist on how the activity of a network-incorporated photocatalyst can be modulated by modifying steric access to the active sites through external stimuli.33,39–44 Despite their promise, only a few limited examples of multi-responsive organic heterocatalytic photoactive materials exist.43,45 Their limitations include inadequate solubility46,47 or limited synthetic versatility. For polymer-based photocatalysts, separating a synthetic product the photocatalytic polymer often remains prohibitively challenging.
Here, we attempt to address these limitations by engineering a dual responsive heterogeneous photocatalyst (temperature and light) based on photocatalytic polymer brushes (Fig. 1) that provides tunable photocatalytic properties while allowing facile separation from the reaction mixture. In detail, N-isopropylacrylamide (NIPAAm) is copolymerized with the photoactive fluorescein o-acrylate (FlA) to produce a multi-responsive smart material poly(FlA-co-NIPAAm) (Fig. 2a). Poly(N-isopropylacrylamide) (PNIPAAm) homopolymers are well-known to undergo a change from intramolecular (hydrophillic) to intermolecular (hydrophobic) interactions in H2O at a lower critical solution temperature (TLCST,avg = 32 °C). The LCST of poly(NIPAAm) and its copolymers has been shown to vary based on molecular weight, concentration, composition, and various other parameters.48 This was leveraged previously to produce thermoresponsive materials, coatings, and surface-tethered macromolecules (polymer brushes) that show well-controlled temperature response.49–54 PNIPAAm is commonly studied in biomedical applications48,55–58 or membrane filtration,59,60 but there has also been interest in its use for wastewater treatment.61 The described approach provides facile functionalization of inexpensive and optically transparent materials (glass beads) and the ability to tune photocatalytic activity via temperature. The resulting heterogeneous photocatalysts can easily be filtered off and separated from the reaction medium. A model degradation of tetracycline hydrochloride (TC) is studied to highlight utility of these materials in wastewater remediation and examine their dual reactivity. TC is a is a common antibiotic pollutant in aqueous systems.62,63 While other groups have shown PNIPAAm/photocatalyst systems that generally decrease their activity upon heating, our studies surprisingly show increasing TC degradation at elevated temperatures above the material's LCST.
Fig. 1 Illustration of the overall idea of combining both thermal and light responsive features on a surface. |
Table 1 summarizes the synthesized photocatalytic materials. Poly(FlA-co-NIPAAm) polymer brushes (abbreviated as FN@SiOx) were synthesized at varying monomer to free CTA ratios to control the final polymer brush thickness on the SiOx surface. Free poly(FlA-co-NIPAAm) polymer simultaneously formed in solution were used to determine molecular weight (Mn) and composition via nuclear magnetic resonance spectroscopy (1H NMR, Table 1, and Fig. S2–4†). Varying the molar ratio of NIPAAm to CDTPA allowed control over molecular weights. Good agreement was observed between the targeted and experimentally determined incorporation of FlA at an average of 11.7 mol% as determined by 1H NMR (see Fig. S2†). At a feed ratio of 10 mol% in the polymerization mixture, fluorescein incorporation into the copolymer was slightly higher (13 mol%) at lower target molecular weights and decreased incorporation (just under at 9 mol%) at higher NIPAAm:CDTPA ratios. This can be attributed to mass transfer limitations observed by gelation of the reaction mixture at increasing target polymer molecular weights.
Entry | Experimental conditionsa [NIPAAm]:[FlA]:[CDTPA] | Thicknessb (d, nm) | Water contact angle (θ, °)c | M n (g mol−1) | FlA incorporation |
---|---|---|---|---|---|
a NIPAAm = N-isopropylacrylamide, FlA = fluorescein o-acrylate, CDTPA = 4-cyano-4-[(dodecylsulfanylthiocarbonyl)sulfanyl] pentanoic acid. The thermal SI RAFT polymerization was carried out in inert atmosphere with ABIN (0.25 molar ratio) as initiator at 75 °C for 24 hours in DMF. The wafers were cleaned with DCM and MeOH, followed by a stream of nitrogen. b Thickness determined through J.A. Woollam RC2-D VASE. c WCA measurements determined via an in-house setup (Fig. S8†). d Molecular weight determined through chain-end analysis using 1H NMR in DMSO-d6. e Pure PNIPAAm polymer brush wafer cleaned only with MeOH and molecular weight determined through chain end analysis using 1H NMR in CDCl3. | |||||
1 FN@SiOx-5 | [250]:[25]:[1] | 7.5 ± 0.03 | 65.2 ± 2.8 | 7000 | 13% |
2 FN@SiOx-15 | [500]:[50]:[1] | 13.1 ± 0.4 | 65.8 ± 1.2 | 13000 | 13% |
3 FN@SiOx-25 | [1000]:[100]:[1] | 22.9 ± 0.5 | 64.8 ± 1.1 | 22900 | 9% |
4e PNIPAAm | [1000]:[0]:[1] | 24.3 ± 1.8 | 55.6 ± 0.6 | 16700 | — |
5 PFlA | [0]:[100]:[1] | 10.8 ± 1.2 | 46.6 ± 3.4 | 12700 | 100% |
The resulting FN@SiOx glass beads and flat silicon wafers were characterized with X-ray photoelectron spectroscopy (XPS). Fig. 2c and Fig. S5 and 6† show survey and high-resolution scans of the C 1s carbon environment for FN@SiOx catalysts of varying thicknesses. Increasing polymer brush thickness was evidenced for both glass beads and silicon wafers through the decreasing intensity of the Si 2p silicon peak at BE = 102 eV (see survey spectra). In the case of the soda-lime beads, the Na KLL Auger peak at BE = 497 eV decreased with increasing copolymer brush film thickness. High resolution C 1s curve fits further verified individual carbon environments on all substrates: –C (285 eV), –(N,O) (286.4 eV), and both carbonyl O and amide N–O carbon atoms (288.0 eV). The nitrogen/carbon signal ratio (N 1s:C 1s) was used to elucidate the fluorescein o-acrylate incorporation. N 1s:C 1s ratios for the functionalized FN@SiOx beads were experimentally determined to 0.13, 0.13, and 0.12 for films of 5 nm, 15 nm, and 25 nm targeted thickness, respectively. This matches well with the anticipated ratio of N 1s:C 1s = 0.12 that was calculated based on a 10 mol% feed of fluorescein o-acrylate monomer (Table S2†). In addition, the similar nitrogen to carbon ratios confirmed the random copolymerization between the NIPAAm and FlA monomers.
The photoactive FN@SiOx films produced hydrophilic coatings (at room temperature) as apparent from their water contact angles (θ, Fig. S9† and Table 1). The CDTPA initiating monolayer exhibited hydrophobic properties (θ ≈ 94.9 ± 2.4°) prior to SI-RAFT polymerization. In comparison to pure PNIPAAm coatings (θ ≈ 55.6 ± 0.6°) and a PFlA films (θ ≈ 46.6 ± 3.4°) the copolymerized FN@SiOx polymer brushes exhibited a slightly increased hydrophobicity at θ ≈ 65.2 ± 0.5°. Notably, there was no appreciable water contact angle difference between the distinct film thicknesses.
Further, Fig. 2d shows how the overall concentration of fluorescein increases with FN@SiOx polymer brush film thickness as determined via ultraviolet-visible (UV/vis) diffuse reflectance (DR) spectroscopy. An emission spectrum was collected via multiphoton microscopy of FN@SiOx in H2O (Fig. S7†) to determine the fluorescence of the photocatalyst when polymerized on a surface. When excited, the beads emitted fluorescence at λmax = 500 nm and an observed lifetime of 3.3 ns, which is comparable to reports on fluorescein as a small molecule in solution.66 Consequently, copolymerizing fluorescein into a surface-tethered polymer appears to not significantly influence its photophysical properties.
Vibrational sum frequency generation (SFG) spectroscopic analysis of the FN@SiOx films showed that the polymer brush surface undergoes substantial changes (Fig. 3b and Fig. S10†). The ratio of the 2878 cm−1 peak in the ssp polarization spectrum to the 2970 cm−1 peak in the ppp polarization spectrum is ∼3.4 below LCST and becomes ∼0.22 above LCST. This implies that CH3 groups at the brush end are tilted about 35° from the surface normal when the brush is extended below LCST and reoriented nearly parallel to the surface when the brush is collapsed above LCST.67 Also, the –N(H)– and –OH groups appear to be nearly normal to the surface below LCST (strong in the ssp spectrum) and become more parallel to the surface above LCST (stronger in the ppp spectrum).
Fig. 4a shows FN@SiOx-catalyzed TC degradation kinetics for the three distinct FN@SiOx polymer brush catalysts synthesized. UV/Vis spectroscopy was used to measure how [TC] concentration changes with time (C/C0, see Fig. 4b for an example of raw UV/vis data). Experiments were performed by irradiating a solution of TC in deionized water (DIW) with white LEDs (Fig. S11 and S17† for irradiation of natural sunlight). To interrogate the influence of temperature, experiments were performed below LCST (T = 22 °C) and at elevated temperature above LCST (T = 50 °C, Fig. S11†). Before any data collection, the molar absorptivity coefficient was determined via a calibration curve of TC at varying concentrations (ε = 1.62 × 107 M−1 cm−1 at λ = 356 nm, Fig. S12†).
At room temperature (T < LCST), little difference in degradation rates was observed between the photocatalytic brushes of different thicknesses (Fig. 4a). We found this surprising, considering that UV/vis DR spectroscopy (see Fig. 2d) clearly indicated an increased fluorescein concentration with the brush thickness. Approximately 50% of the TC is degraded after 2 hours of reaction time, corresponding to an average 0.0065 min−1 rate constant (k) as determined by a pseudo-first order reaction rate from ln(C/C0) with respect to time (t, Fig. S13 and Table S4†).
(1) |
In contrast, elevating the temperature to 50 °C, i.e., above T > LCST, improves degradation rates for all catalysts (see Fig. S13 and Table S4† for summary of rate constants). Notably, thicker poly(FlA-co-NIPAAm) brushes lead to faster TC degradation rates (Fig. 4 and S13†). The catalytic efficiency increases from ∼50% to ∼68% for both FN@SiOx-5 nm and FN@SiOx-15 nm with an average of 0.0102 min−1 rate constant. Interestingly, the thickest brush (FN@SiOx-25 nm) demonstrates the most response to temperature – while at room temperature it does not significantly stand out when compared to thinner photocatalytic films. For FN@SiOx-25 nm, the degradation of TC almost doubled in efficiency increasing from 49% (RT) to 81% (50 °C), with an increased 0.0175 min−1 rate constant. This suggests a conformational rearrangement of the polymer brushes above LCST (Fig. 3b and Fig. S10†), which would affect the availability of fluorescein for photocatalysis either by being exposed at the outermost surface or the chain end conformations allowing more ingress of TC into the brush.
Control experiments in the absence of photocatalysts (but under irradiation) or in the dark showed no significant degradation of the TC antibiotics and negligible temperature effects or thermal degradation were observed (see Fig. 4c and Fig. S14†).
Based on these findings, the dual thermo- and photo-active heterogeneous catalysts show improved performance at elevated temperatures. We hypothesize that the conformational collapse of the PNIPAAm backbone above LCST leads to an increased accessibility of TC to the fluorescein photocatalysts. This would improve catalytic performance for all films but be most pronounced for thicker films. As such, this hypothesis aligns well with our experimental findings.
Notably, this result contrasts with previous work on thermoresponsive photocatalysis.68–71 For example, Huo et al. used PNIPAM@AgBr/CSs nanocomposites for the degradation of tetracyline for a dual-responsive purpose. They found that above the LCST and higher temperatures, the degradation rate decreased.72 In another multi-responsive study, Yoon et al. observed with a hybrid Au-PNIPAM film with ZnO nanoparticles, an increase in performance at elevated temperatures in the degradation of p-nitrophenol for thin films and low molecular weights.73 However, at high molecular weights and thicker films they noticed a decrease in catalyst efficiency at a temperature above the LCST.73 Initially, their studies are in agreement with our findings at FN@SiOx-5,15 nm; however, the higher molecular weight and thicker films are contrasting our investigation with a fully organic dual responsive heterogeneous catalyst.
Preliminary studies show similar results for other compounds in water remediation efforts. For the removal of the dye methylene blue (MB), FN@SiOx-25 nm degraded 79% of MB at room temperature (Fig. S18b†). The catalytic efficiency increased to 97% at elevated temperatures, which is complementary to what we are observing in the degradation of TC. Further studies are going towards the study of other substrates and whether this is a universal trend for different compounds.
We further tested the stability of the FN@SiOx substrates by recycling them in three consecutive degradations of TC at the two different temperatures (Fig. S16†). Recovery through simple filtration successfully allowed the reusability of FN@SiOx-25 nm beads with negligible difference in catalytic performance over each reaction cycle. While Mao et al. recycled their dual responsive nanoparticles (ZnPC-g-TiO2-g-PNIPAAm) in the removal of the dye Rhodamine B (RhoB) at room temperature for three cycles, their separation process included a high-speed centrifugation and elevated temperatures of 45 °C.69 The size of our supports eliminates the time and effort it takes to recovery the heterogeneous catalysts typically needed for such processes, increasing recyclability efficiency.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3py00248a |
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