Open Access Article
Xuefeng Zhu†
a,
Shikai Xue†ab,
Pingyuan Xiea,
Qingxian Xua,
Yingxin Liua,
Chengyong Li*a and
Qiujun Lu
*a
aCollege of Biological and Chemical Engineering, Changsha University, Changsha 410022, China. E-mail: lyong92@163.com; luqiujun@ccsu.edu.cn
bCollege of Chemistry and Bioengineering, Guilin University of Technology, Guilin 541004, China
First published on 27th October 2025
The advancement of industrialization has led to severe environmental challenges stemming from inadequate pollutant management. Photocatalytic technology has emerged as a research focus due to its eco-friendly nature and high degradation efficiency. However, the widespread application of photocatalysts is hindered by limitations in recoverability and reusability. Therefore, designing high-performance photocatalysts with facile recoverability has become a critical research direction. Thermo-responsive materials, which precipitate upon heating and disperse upon cooling, offer a promising solution for enhancing recovery efficiency. In this study, a composite photocatalyst with thermo-responsive properties was successfully synthesized by combining graphite carbon nitride (g-C3N4) with the thermo-responsive copolymer NIPAM-DADMAC (poly(N-isopropylacrylamide)-co-diallyl dimethylammonium chloride). Key parameters including the optimal mass ratio of g-C3N4 to DADMAC-NIPAM, and the optimal recovery conditions were systematically determined by measuring the material's lower critical solution temperature (LCST). Experimental results demonstrated that under visible light irradiation, the composite photocatalyst achieved a remarkable 98.15% degradation rate of methyl orange (MO) within 120 min. Moreover, the composite exhibited exceptional stability and reusability, retaining over 77.92% of its degradation efficiency even after eight consecutive cycles. Additionally, its inherent thermo-responsive nature enabled highly efficient recovery of the catalyst. This research provides valuable insights and a novel strategy for the development of high-performance photocatalysts with enhanced recyclability, holding significant potential for practical applications in environmental remediation.
Since Scarpa et al.24 first discovered the thermally induced phase transition behaviour of poly(N-isopropylacrylamide) (PNIPAM) in the 1960s, thermo-sensitive polymers of this type have consistently attracted substantial academic interest, particularly in the fields of pharmaceuticals and bioengineering.25 As a typical thermosensitive polymer, PNIPAM exhibits unique lower critical solution temperature (LCST) behaviour.26 Below the LCST, PNIPAM is highly soluble in water and forms a homogeneous solution; above the LCST, it undergoes a phase transition, leading to precipitation. This reversible phase transition property endows PNIPAM with excellent recyclability potential. However, the intrinsic functionality of pure PNIPAM is relatively limited, especially in terms of pollutant adsorption, which restricts its direct application in photocatalytic systems.
To further expand the functionality of PNIPAM, researchers have developed novel temperature-sensitive microgel systems through copolymerization with various hydrophilic or hydrophobic monomers.27 Among these monomers, diallyl dimethylammonium chloride (DADMAC), a cationic monomer with highly hydrophilic quaternary ammonium groups, has been widely studied. When copolymerized with PNIPAM, DADMAC can form microgels that exhibit both temperature sensitivity and charge responsiveness.28 These copolymer microgels are fully ionized in aqueous solutions, forming polymer segments with specific charge density and spacing. This charge characteristic enables them to efficiently capture charged particles or microorganisms through electrostatic interactions. Moreover, the low toxicity of these copolymers significantly enhances their advantages for applications in pharmaceutical biocompatibility and advanced drinking water treatment.
Graphite carbon nitride (g-C3N4) has attracted considerable attention as a promising visible-light-responsive photocatalyst due to its moderate bandgap, suitable electronic band structure, non-toxicity, and low cost.29–33 However, like many other powdered photocatalysts, g-C3N4 in its pure form is prone to aggregation in aqueous solutions, and its fine powder nature makes it extremely difficult to recover from the treated water. These issues severely limit its practical application in real-world water treatment scenarios.34–36 To address these challenges, the development of composite photocatalytic materials by integrating g-C3N4 with appropriate SI materials has become a current research hotspot. The goal is to combine the excellent photocatalytic performance of g-C3N4 with the favourable recoverability of the SI materials. Nevertheless, the application of NIPAM-co-DADMAC and its analogues in photocatalysis remains relatively under-explored. These copolymers have been primarily confined to adsorption applications.37–40 The integration of these thermo-sensitive copolymers with photocatalytic matrices holds great promise in terms of photocatalytic synergy. This synergy is expected to significantly enhance the dispersion and recyclability of photocatalysts.
In this study, g-C3N4 was prepared by calcination. Leveraging the electrostatic interaction between g-C3N4 and the PNIPAM copolymer containing cationic DADMAC, a thermo-responsive g-C3N4/NIPAM-DADMAC composite material was synthesized, aiming to fully exploit the complementary advantages of both components. Furthermore, we investigated the mass ratio of DADMAC-NIPAM to g-C3N4 in the composite and the LCST of the material to determine the optimal loading ratio and recovery conditions.
:
0.05, 1
:
0.1, 1
:
1, and 1
:
2 were synthesized accordingly.
706 and a polydispersity index (PDI, Mw/Mn) of 2.9068, indicative of moderate chain-length uniformity.
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| Fig. 1 (A) Nuclear magnetic resonance hydrogen spectrum and (B) gel chromatography diagram of NIPAM-DADMAC. | ||
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| Fig. 2 (A) SEM image of g-C3N4, and (B and C) g-C3N4/NIPAM-DADMAC; (D–F) EDS image of g-C3N4/NIPAM-DADMAC. | ||
N–C at 288.1 eV; N–(C)3 at 400.8 eV).44–46 FTIR analysis (Fig. 3D) provided complementary evidence, with the composite spectrum exhibiting diagnostic absorption bands assignable to g-C3N4 (e.g., 806 cm−1 for triazine ring modes; 1250–1650 cm−1 for C–N/C
N stretching) and NIPAM-co-DADMAC (e.g., 2953 cm−1 for –CH2; 3400 cm−1 for N–H bending). These collective results unambiguously validate the successful synthesis of the g-C3N4/NIPAM-co-DADMAC composite.
:
NIPAM-co-DADMAC ratio of 0.1
:
1, the zeta potential reached a maximum of +23.2 mV. Further increases in polymer content yielded no significant potential change, indicating saturation of g-C3N4 surface sites. This charge reversal phenomenon confirms effective electrostatic adsorption of NIPAM-co-DADMAC onto g-C3N4, achieving successful surface modification through charge density modulation.
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| Fig. 5 (A)Comparison of the dispersibility of g-C3N4 and g-C3N4/NIPAM-DADMAC; (B) low critical transition temperature analysis diagram of NIPAM-DADMAC. | ||
In contrast, the g-C3N4/NIPAM-DADMAC composite suspension maintained a homogeneous turbidity even after 3 days of standing. No obvious sedimentation was observed, indicating that the composite has excellent dispersibility in aqueous solutions. This significant improvement in dispersibility is attributed to the presence of the NIPAM-co-DADMAC copolymer on the surface of g-C3N4. The copolymer chains, which are highly soluble in water below the LCST, form a steric stabilization layer around the g-C3N4 particles. This layer prevents the aggregation of g-C3N4 particles by reducing the van der Waals forces and increasing the repulsive forces between the particles. The excellent dispersibility of the composite ensures that the photocatalytic active sites are fully exposed to the pollutant molecules and light, thereby enhancing the photocatalytic performance.
The thermo-responsive transition of NIPAM-co-DADMAC was quantified by temperature-dependent transmittance analysis (Fig. 5B). As the temperature increased, the transmittance of the solution began to decrease gradually. This decrease in transmittance is due to the phase transition of the copolymer. Above the LCST, the copolymer chains undergo a conformational change, transitioning from an extended, hydrophilic state to a collapsed, hydrophobic state. The hydrophobic copolymer chains then aggregate together, forming large particles that scatter light, resulting in a decrease in transmittance. The inflection point in the transmittance–temperature curve, which corresponds to the temperature at which the transmittance decreases by 50%, is defined as the LCST of the copolymer. From Fig. 5B, it can be determined that the LCST of the NIPAM-DADMAC copolymer is approximately 45 °C.
Fig. S1A shows the UV-DRS spectra of the pristine g-C3N4 and g-C3N4/NIPAM-DADMAC composite. It can be observed that the UV-DRS spectrum of the composite closely resembles that of the pristine g-C3N4. Fig. S1B shows that the bandgap energy of the composite is virtually identical to that of the pristine g-C3N4. This indicates that the hybridization of g-C3N4 with the NIPAM-co-DADMAC copolymer does not appreciably perturb the electronic structure of the g-C3N4 framework. In addition, the photoluminescence (PL) spectra of g-C3N4 and g-C3N4/NIPAM-DADMAC composites were also determined. As shown in Fig. S1C, there was no significant intensity difference in the PL spectra of g-C3N4 and g-C3N4/NIPAM-DADMAC composites, further indicating that the hybridization of g-C3N4 with NIPAM-co-DADMAC copolymer had no obvious effect on the electronic structure of the g-C3N4 framework and still maintained a similar charge separation efficiency. Overall, the results of UV-DRS and PL analysis indicated that the combination of NIPAM-DADMAC copolymer with g-C3N4 did not weaken the light absorption ability of g-C3N4. These optical properties laid a good foundation for the excellent photocatalytic performance of the composites.
Fig. 6A compares the MO degradation performance of g-C3N4/NIPAM-DADMAC composites at varying mass ratios under visible light irradiation. It can be clearly observed that the mass ratio has a significant impact on the photocatalytic activity of the composite. After 20 min of visible light irradiation, the composite with a mass ratio of 1
:
0.1 (g-C3N4
:
NIPAM-DADMAC) exhibited the fastest degradation rate of MO, with a degradation rate of approximately 54.01%. In contrast, the composites with other mass ratios (1
:
0.05, 1
:
1, and 1
:
2) demonstrated relatively slower degradation rates, with degradation rates of around 39.66%, 42.10%, and 46.43%, respectively. With the extension of the irradiation time to 120 min, the composite with the 1
:
0.1 mass ratio achieved the highest degradation efficiency of 98.15%. The composites with the 1
:
0.05, 1
:
1, and 1
:
2 mass ratios reached degradation efficiencies of 97.45%, 96.28%, and 89.58%, respectively. These results clearly indicate that the composite with the 1
:
0.1 mass ratio has the best photocatalytic activity among all the tested samples.
To further analyze the photocatalytic kinetics, the degradation data were fitted using the pseudo-first-order kinetic model, which is commonly used to describe the photocatalytic degradation of organic pollutants.47–50 The pseudo-first-order kinetic equation is expressed as:
| −Ln(C/C0) = kt |
Fig. 6B shows the corresponding pseudo-first-order kinetic curves for the composites with different mass ratios. The composite with the 1
:
0.1 mass ratio has the highest rate constant of 0.03336 min−1, which is significantly higher than those of the other composites (0.03106 min−1 for 1
:
0.05, 0.02813 min−1 for 1
:
1, and 0.01839 min−1 for 1
:
2). This further confirms that the 1
:
0.1 mass ratio is the optimal ratio for the composite to exhibit the best photocatalytic performance.
The reason for the optimal mass ratio can be explained as follows: when the amount of NIPAM-DADMAC copolymer is too low (mass ratio 1
:
0.05), the copolymer cannot fully cover the surface of g-C3N4. As a result, the dispersibility of the composite is poor, and the adsorption capacity for MO is limited, leading to lower photocatalytic activity. When the amount of copolymer is too high (mass ratios 1
:
1 and 1
:
2), the excess copolymer may cover the active sites of g-C3N4, blocking the light absorption and reducing the number of available photogenerated electron–hole pairs. Additionally, the excess copolymer may form a thick layer on the surface of g-C3N4, increasing the charge transfer resistance and promoting the recombination of photogenerated charges. Therefore, the composite with the 1
:
0.1 mass ratio has the optimal balance between the dispersibility, adsorption capacity, and active site exposure, resulting in the highest photocatalytic activity.
The reaction temperature is another important parameter that can affect the photocatalytic activity of the composite. Fig. 6C shows the degradation rate curves of MO at different temperatures. It can be observed that the reaction temperature has a significant impact on the degradation efficiency, and the degradation efficiency decreases as the temperature rises. The corresponding pseudo-first-order kinetic curves are shown in Fig. 6D. The rate constants gradually decrease with the increase of temperature, being 0.00400 min−1 at 35 °C, 0.00400 min−1 at 45 °C, and 0.00147 min−1 at 50 °C, respectively.
The decrease in photocatalytic activity at higher temperatures can be attributed to the phase transition and precipitation of the NIPAM-co-DADMAC copolymer above the LCST (45 °C). This precipitation leads to the aggregation of the composite material, thereby reducing the specific surface area and the exposure of active sites.
To further confirm that the degradation efficiency decreases with the increase in temperature, additional experiments on the degradation of rhodamine B (another common dye pollutant) at different temperatures were conducted. The results (Fig. S2) showed a similar trend.
To evaluate the performance of the g-C3N4/NIPAM-DADMAC composite in comparison with other reported photocatalytic materials, a comprehensive comparison was conducted based on key parameters such as photocatalyst dosage, pollutant concentration, degradation time, removal rate, and recyclability. The results are summarized in Table 1.
| Sample | Catalyst dosage (g L−1) | Pollutant | Pollutant concentration (mg L−1) | Light source | Photocatalytic degradation time (min) | Removal rate | Recyclability | Ref. |
|---|---|---|---|---|---|---|---|---|
| Co/P–C3N4 | 1.00 | Methyl orange | 10 | 300 W mercury lamp | 120 | 70% | — | 51 |
| C3N4/AlFeO3 | 1.00 | Methyl orange | 20 | 500 W xenon lamp | 60 | 97% | 91% (5th) | 52 |
| Bi@BiOCl/C3N4-DPY | 0.67 | Methyl orange | 10 | 500 W xenon lamp | 180 | 84.5% | 82% (4th) | 53 |
| BiO–Ag(0)/C3N4@ZIF-67 | 1.0 | Congo red | 40 | Solar | 150 | 90.0% | 78.2% (4th) | 54 |
| g-C3N4/NIPAM-DADMAC | 0.5 | Methyl orange | 25 | 100 W deuterium lamp | 120 | 98% | 77.92% (8th) | This work |
:
0.1 mass ratio) was evaluated by repeating the photocatalytic degradation experiment of MO for multiple cycles.
Fig. 7 shows the schematic diagram of the cyclic photocatalytic process and the degradation efficiency of the composite over 8 consecutive cycles. After each photocatalytic cycle, the composite was recovered through a simple thermo-responsive precipitation process: the temperature of the reaction solution was raised to LCST of the copolymer, causing the composite to precipitate. The precipitated composite was then separated from the solution by centrifugation at 5000 rpm for 5 min, washed thoroughly with deionized water three times to remove any residual MO molecules and by-products, and then reused in the next cycle under the same experimental conditions. As shown in Fig. 7, the composite exhibited excellent reusability, even after eight successive cycles, the photocatalytic efficiency of the composite was still as high as 77.92%.
This gradual decline in degradation efficiency is a common phenomenon in cyclic photocatalytic experiments and can be attributed to cumulative occupation of active sites, partial catalyst leaching, and structural changes. To exclude structural alteration as the primary cause of the activity loss, the FTIR spectra of the fresh and used composite (after 8 cycles) were compared. Fig. S3 shows the FTIR spectra of the two samples. It can be observed that there are no discernible changes in the characteristic absorption bands of the composite. The peaks corresponding to g-C3N4 (806 cm−1 for triazine ring bending, 1250–1650 cm−1 for C–N/C
N stretching) and the NIPAM-DADMAC copolymer (2953 cm−1 for C–H stretching, 3400 cm−1 for N–H stretching) are still present and have the same intensity and position in both spectra. This indicates that the framework structure of the composite remains intact throughout the 8 cycles of photocatalytic reaction and recovery. Therefore, the main cause of the loss of activity might be the cumulative occupation of active sites by pollutants and the loss of some catalysts, rather than structural decomposition.
The excellent reusability of the g-C3N4/NIPAM-DADMAC composite, combined with the simple and energy-efficient thermal recovery protocol, makes it a highly promising candidate for practical and sustainable water treatment applications. The ability to reuse the composite for multiple cycles not only reduces the cost of the photocatalytic process but also minimizes the environmental impact associated with the disposal of used photocatalysts.
As shown in Fig. S4, within 120 min of illumination, the removal efficiency of this composite material for rhodamine B was approximately 94.2%, for tetracycline hydrochloride was 70.1%, and for Congo red was 45.2%, highlighting its wide applicability to various water pollutants. These results clearly demonstrate the versatility of the g-C3N4/NIPAM-DADMAC composite in degrading diverse aquatic pollutants. This broad applicability significantly enhances the practical value of the composite in environmental remediation.
Three common trapping agents were used in the experiments: isopropanol (IPA) was used to trap hydroxyl radicals (˙OH), para-benzoquinone (PBQ) was used to trap superoxide radicals (˙O2−), and ethylenediaminetetraacetic acid disodium salt (EDTA) was used to trap photogenerated holes (h+). The trapping experiments were carried out under the same optimal conditions as the photocatalytic activity evaluation.
Fig. 8 shows the results of the trapping experiments. When IPA was added to trap ˙OH, the degradation rate of MO slightly decreased to approximately 79.20%. This indicates that ˙OH plays a minor role in the photocatalytic degradation process. When EDTA was added to trap h+, the degradation rate further decreased to around 76.53%, suggesting that h+ contributes more to the degradation than ˙OH.
In contrast, when PBQ was added to trap ˙O2−, the degradation rate of MO was almost completely inhibited, with a degradation rate of only about 30.93%. This significant inhibition clearly indicates that ˙O2− is the primary active radical responsible for the photocatalytic degradation of MO by the composite.
:
0.1, achieved 98.15% degradation in 120 min at 25 °C. It exhibited excellent stability and retained 77.92% efficiency after eight cycles. The composite demonstrated broad applicability in degrading various pollutants, including rhodamine B, tetracycline hydrochloride, and Congo red. Active species trapping experiments indicated that ˙O2− were the primary active radicals responsible for the photocatalytic degradation process. This work establishes that strategic integration of thermosensitive polymers with semiconductor photocatalysts effectively reconciles the traditional trade-off between high catalytic activity and practical recoverability. The demonstrated synergy of electrostatic assembly and LCST-mediated recovery presents a viable design strategy for next-generation smart photocatalytic systems in sustainable water remediation.
Supplementary information is available. See DOI: https://doi.org/10.1039/d5ra05141j.
Footnote |
| † Co-first authorship. |
| This journal is © The Royal Society of Chemistry 2025 |