Xiao Wangab,
Jiahui Zhangab,
Xiaoting Liab,
Huiwen Yuab,
Lingcao Tanab,
Qiongyao Wangab,
Wenhua Xuabc,
Baiping Xuab,
Shuping Xiao*ab and
Jiarong Huang*ab
aSchool of Mechanical and Automation Engineering, Wuyi University, Jiangmen, 529020, China. E-mail: hjr@wyu.edu.cn; xsp@wyu.edu.cn
bJiangmen Key Laboratory of Polymer Intelligent Manufacturing, Wuyi University, Jiangmen, 529020, China
cGuangdong Provincial Key Laboratory of Technique and Equipment for Macromolecular Advanced Manufacturing, South China University of Technology, Guangzhou, 510640, China
First published on 23rd July 2025
Shape memory polymers (SMPs) represent a prominent category of smart polymers that show attractive prospects in emerging fields of soft robots and biomedical devices. However, most of the existing SMPs show limitations in single-stimulus responsiveness and an imbalance between mechanical and shape memory properties. Herein, biological phytic acid served as a natural curing agent to vulcanize the biobased epoxidized natural rubber (ENR), while Fe3+ was introduced to construct a second cross-linked network based on coordination interaction. Polycaprolactone (PCL) was introduced and acted as net points to regulate the shape fixing behavior, while the dual cross-linked network provided strong resilience to achieve the shape recovery performance. Meanwhile, the Fe3+-based coordination complex not only served as sacrificial elements to realize tunable mechanical properties by effectively dissipating energy, but also acted as a photothermal agent to realize the light-induced shape memory behavior and thermoelectric power generation. The fabricated composites possess multi-stimuli-responsive shape memory properties, photothermal capabilities, and tunable mechanical properties, exhibiting outstanding potential in harvesting sunlight for outdoor portable power generation and stimuli-responsive sensors.
Various strategies have been proposed to fabricate SMPs, such as the construction of a glassy transition gradient, rubber/plastic blending, and the construction of an interpenetrating network.7–13 Among these methods, rubber/plastic blending is considered one of the most facile strategies to endow polymers with a shape memory effect.14–18 On the one hand, the plastic component can act as net-points to fix the temporary shape, improving the shape memory effect. On the other hand, the plastic component exhibits excellent thermoplasticity, providing the covalently cross-linked rubber with processability. Xu et al. prepared ethylene propylene diene monomer/polypropylene thermoplastic vulcanizate (PP/EPDM TPV) with a sea-island structure through dynamic vulcanization, in which the PP matrix could maintain the temporary shape of TPVs and the cross-linked EPDM phase supplied stress to drive the deformed shape recovery during the shape memory process.19 We have fabricated a series of shape memory polylactic (PLA)/rubber blends, in which the continuous PLA matrix acted as a controlling switch to fix/release the programmed shapes, and the rubber network drove the recovery of the permanent shape.20,21 However, the shape memory effect of rubber-based SMPs essentially stems from the entropic elasticity of rubber,22 which needs to be triggered by temperature. Therefore, most of the existing rubber-based SMPs are heat-triggered SMPs, which are limited to responding to a single stimulus, hindering their future application in the realm of smart materials.
To overcome the above restriction, various functional fillers have been utilized to fabricate multi-stimuli-responsive SMPs, whose shape memory effect can be triggered by light, moisture, electrical/magnetic fields, and so on.23–26 Among all stimulus-triggered SMPs, light-triggered SMPs have attracted much attention due to their excellent characteristic of remote activation and spatial controllability. The light-responsive capacity can be introduced to SMPs by two different mechanisms. The first is achieved via integrating intrinsic light-responsive molecular units into the matrix, while the second mechanism utilizes photothermal effects. Various fillers, such as graphene, carbon nanotubes, melanin, gold nanomaterials, and metal ion-based coordination compounds, can be used as photothermal agents to introduce the photothermal effect into the matrix.20,27–29 However, the introduction of functional fillers is often accompanied by a deterioration in mechanical properties, which is caused by the poor compatibility and aggregation of the fillers.30,31 Generally speaking, interface modification can improve compatibility. However, such improvement is always accompanied by a large amount of additional modification work and extensive use of chemical reagents, and there is a possibility that the functional properties of the filler may be lost. Therefore, there remains a critical demand for designing shape memory composites that encompass tunable mechanical properties and multi-stimuli responsiveness.
Inspired by the hierarchical architectures in natural materials, various energy-dissipating strategies, such as weak interactions, dual/multi-cross-linked networks, and heterogeneous domains, have been introduced to improve the mechanical properties of rubber-based materials.32–35 Ducrot et al. synthesized tough elastomers consisting of a rigid network and a flexible second network, where the rigid network could be preferentially broken to dissipate energy, leading to toughening of the elastomers.32 Guo et al. fabricated a mechanically robust styrene-butadiene rubber (SBR) by introducing polysulfide to achieve the chemical cross-linking of SBR and grafting iron–carboxylate complexes onto SBR chains.33 The grafted iron–carboxylate complexes aggregated to form a phase-separated structure, which enhanced the mechanical properties by promoting energy-dissipating efficiency. Inspired by the current research, in this work, we intend to design a shape memory elastomer by introducing Fe3+-based coordination compounds into the rubber/plastic system, in which the coordination compounds not only act as the photothermal agent to realize light-triggered shape memory behavior, but also act as a second cross-linked network to reinforce the composites.
Here, we present a facile and effective strategy to prepare shape memory composites with tunable mechanical properties and shape memory capabilities simultaneously. Polycaprolactone (PCL) was introduced into the ENR matrix to regulate the shape fixing behavior of ENR based on the glassy state of PCL at 25 °C, and release the temporary shapes based on the melting behavior of PCL at ∼60 °C. Phytic acid, a natural plant product, was utilized as a curing agent to cross-link ENR based on esterification reactions between phosphate groups and epoxy groups.31,36 Subsequently, Fe3+ ions were utilized to construct the second cross-linked network through the coordination interaction between Fe3+ and oxygen-containing groups. On the one hand, the dual cross-linked network could construct a tunable glass transition gradient, which would help improve the shape memory performance. On the other hand, the coordination bonds serve as sacrificial elements to promote the dissipation of energy when subjected to external force, achieving the remarkable reinforcement of the composites. Additionally, the coordination compounds based on Fe3+ are available as photothermal agents because of their excellent photothermal effect, expanding the shape memory capabilities and thermoelectric power generation under near-infrared light or sun irradiation.
To eliminate the influence of moisture in PA, the PA aqueous solution was concentrated to remove most of the water, which can be found in the ESI (Fig. S1 and S2†). The ENR/PCL/PA/FeCl3 blends were obtained through a similar process, in which the enriched PA solution and FeCl3 powder were sequentially added to the ENR/PCL blends. Subsequently, the obtained ENR/PCL/PA/FeCl3 blends were compression moulded at 170 °C and 5 MPa for 5 min to obtain the composites with a thickness of 1 mm for different tests. Before the compression moulding, the blends were preheated at 170 °C for 2 min and then exhausted 8 times, which can help to further remove the residual moisture of PA. The detailed processing technique can be found in the ESI.† In the ENR/PCL/PA/FeCl3 composites, the weight ratio of ENR/PCL was fixed at 70/30 (wt%/wt%), the loading amount of PA solution was fixed at 0.5 phr (parts per hundred parts) of ENR, and the loading amounts of FeCl3 powder were 0, 0.5, 1, 2, and 3 phr of ENR, respectively. The detailed formulations of ENR/PCL/PA/FeCl3 composites are listed in Table S2.† The obtained ENR/PCL/PA/FeCl3 composites were coded as PA0.5Fz, where z represented parts of FeCl3.
Cross-link densities were measured according to equilibrium swelling experiments. In brief, the preweighed specimens were immersed in toluene under a shaded environment, and the swollen samples were periodically taken out from the toluene and weighed immediately. The weight measurements were continued until the swollen samples reached constant values. The cross-link densities were calculated according to the Flory–Rehner equation:37
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Dynamic mechanical analysis (DMA) was performed on a METTLER DMA 1 under tension mode. The DMA was performed from −70 °C to 80 °C with a heating rate of 3 °C min−1 and a frequency of 1 Hz. Tensile tests were conducted at room temperature through the CREE-8003D tensile machine (Dongguan CREE INST Rument Technology Co., Ltd, China). The crosshead speed was fixed at 500 mm min−1 according to ISO 37-2017, and five specimens were tested for each formula to obtain average values.
The multi-stimuli-responsive shape memory properties were evaluated according to Fig. S3,† which was described in the ESI† in detail. During the light-triggered shape memory test, a sun simulator (PLS-SXE300+, Beijing Perfectlight Technology Co., Ltd) and a near-infrared laser (NIR, 808 nm, 0–4 W, HW808AD4000-100F, Shenzhen Infrared Laser Technology Co., Ltd, China) were used as light sources. And the temperature of the sample surface was recorded using an infrared imager (R60, Hangzhou Meisheng Infrared Photoelectric Technology Co., Ltd, China). The photo-thermoelectric generator (PTEG) system consisted of a Seebeck thermoelectric generator (SP1848-27145), a heat sink, and an ENR/PCL/PA/FeCl3 composite film. The temperature of PTEG was recorded using an infrared imager, and the output voltage was recorded with a digital multimeter (Keithley DMM 7510, USA).
To verify the above assumption, the rheological behaviors of ENR/PCL blend (E7P3), ENR/PCL/PA blend (PA0.5F0), and ENR/PCL/PA/FeCl3 blend (PA0.5F2) were carried out and are shown in Fig. 2a and S4.† The viscosity (η) of E7P3 remained almost constant throughout the test time range, while the η of PA0.5F0 increased with time, revealing that PA could realize the vulcanization of ENR without any accelerators or additives. Moreover, the η value of the ENR/PCL system could be further improved by introducing Fe3+, ascribed to the coordination interaction between Fe3+ and the oxygen-containing group of ENR.
To explore the mechanism of the dual cross-linked network, FTIR spectra of pure ENR, E7P3, PA0.5F0, and PA0.5F2 were characterized and shown in Fig. 2b. In addition, the enlarged spectra were compared in Fig. 2c. The neat ENR shows an absorption peak at 870 cm−1, which is attributed to the epoxy ring.13,31 The FTIR spectrum of the ENR/PCL simple blend (E7P3) shows absorption peaks at 1720 cm−1, representing the ester groups of PCL (Fig. S5†).7 When PA is introduced into the ENR/PCL system, the intensity of the epoxy peak at 870 cm−1 is decreased, demonstrating the ring-opening reaction of ENR. And another obvious peak at 1064 cm−1 corresponded to the formation of C–O–P bonds,31,36,38 which was overlapped by the C–O–C bonds of PCL. Meanwhile, a new absorption peak appeared at 3450 cm−1, caused by the formation of hydroxyl groups during the ring-opening reaction.13,20 According to the FTIR results, the mechanism of the covalent cross-linked network was proposed in Fig. 2d. ENR could be cured by PA via the ring-opening of the epoxy group, accompanied by the formation of phosphonate ester bonds.
Subsequently, when Fe3+ was introduced into the ENR/PCL/PA system, the absorption peaks of hydroxyl groups shifted to lower wavenumbers, indicating the association between Fe3+ and hydroxyl groups. Besides, for the FTIR spectrum of ENR, the peak around 1064 cm−1 has been demonstrated to be the stretching vibration of the tetrahydrofuran ring, which is the inevitable by-product of ENR with high epoxy content. And the peak around 1110 cm−1 should be ascribed to the tetrahydrofuran ring associated with hydrogen bonds.39 Interestingly, the hydrogen interaction was disrupted by Fe3+–O coordination, resulting in the merging of the two peaks for the tetrahydrofuran ring into one broad band at 1064 cm−1. The XPS results provide additional implications for the Fe3+–O coordination interaction (Fig. 2e). For PA0.5F0, a peak with a binding energy of 531.78 eV can be observed in the O1s spectra, corresponding to C–O–C or C–O–H.13 For PA0.5F2, a shoulder peak with a binding energy of 532.88 eV emerges with the introduction of Fe3+. This emerged peak is ascribed to the more electron-deficient oxygen, disclosing the coordination interaction between Fe3+ and oxygen-containing groups. Based on the above results, the mechanism of the coordination cross-linked network was proposed in Fig. 2d. After the esterification reaction between ENR and PA, the tetrahydrofuran ring, the residual epoxy group, and the generated hydroxyl groups could interact with Fe3+ to form a second cross-linked network.40,41 Thereby, a dual cross-linked network consisting of covalent phosphonate ester bonds and non-covalent coordination interaction was constructed in the ENR/PCL/PA/FeCl3 composites.
Due to the ring-opening reaction between ENR and PA, and the coordination interaction between Fe3+ and oxygen-containing groups, many cross-linking centers were formed in the matrix, which could help resist solvent permeation. For the ENR/PCL blend, the PCL component could be dissolved by toluene quickly, and the linear ENR phase of the ENR/PCL blend first became swollen and then dissolved, resulting in a turbid solution after 60 min (Fig. 3a). However, PA0.5F0 exhibited only swelling behavior without dissolution, visually demonstrating the formation of a phosphonate ester-based cross-linked network. Compared with PA0.5F0, PA0.5F2 maintained its integrated shape better after immersing for 5 days, further disclosing the formation of the Fe3+-based coordination complex. Meanwhile, the dried PA0.5F2 gel still maintained its rectangular shape, which could be stretched to a large deformation and then recovered to its original shape, demonstrating that PCL did not break the continuous structure of the ENR matrix.
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Fig. 3 (a) Swelling experiments, (b) cross-link densities, (c) DSC curves and (d) DMA curves of the ENR/PCL/PA/FeCl3 composites; TEM images: (e) PA0.5F0, (f) PA0.5F1, and (g) PA0.5F2. |
Based on the above swelling experiment, the cross-link densities of the ENR/PCL/PA/FeCl3 composites were calculated and shown in Fig. 3b. An improved cross-link density was observed with increasing Fe3+ content. With the incorporation of 3 phr Fe3+, the cross-link density of the composites (PA0.5F3) reached 18.48 × 10−4 mol cm−3, nearly 19.37 times that of PA0.5F0. The increased cross-link density effectively revealed the consistently developed network architecture, which made it difficult for the solvent to permeate into the matrix.
The increased cross-link density indicates the restricted mobility of the ENR chains, which is consistent with the change in glass transition temperature (Tg), as shown in the DSC curves. As shown in Fig. 3c, the platform around −46 °C and the peak around 45–60 °C represent the glass transition and the melting behavior of the PCL phase, respectively. For the ENR phase, its Tg value increased from −18.56 °C of the ENR/PCL simple blends to −13.44 °C of PA0.5F0 with the incorporation of PA, because the phosphonate ester-based cross-linked network would make chain segmental motion more challenging and demand more energy to activate. The Tg values could be further improved with increasing Fe3+ content. As shown in the DMA curves (Fig. 3d), increased Tg values and decreased tanδ peak values were also observed with increasing Fe3+ content, revealing the further restricted mobility of rubber chains due to the higher cross-link density of the composites with higher Fe3+ content. Additionally, the last rising areas of the DMA curves were ascribed to the melting behavior of the PCL phase (Fig. S6†).
TEM tests were carried out for the ENR/PCL/PA/FeCl3 composites to analyze the structure of the composites and the distribution of FeCl3, as shown in Fig. 3e–g. For PA0.5F0, the light phase is considered the PCL phase, while the dark phase is the ENR phase, which is consistent with the ENR/PCL ratio. When incorporating FeCl3, the interface between the ENR phase and the PCL phase gradually becomes blurred, which is caused by the migration of Fe3+ within the ENR and PCL phases with the help of high temperature and shear force. The black dots in PA0.5F1 are FeCl3, which are uniformly distributed in the matrix (Fig. 3f1). Interestingly, a distinct phase-separated structure can be observed in PA0.5F2 (Fig. 3g). The darker regions represent the dispersed phase, which is overlapped by many loosely packed spherical-shaped domains with diameters of tens of nanometers. With the increase of Fe3+ content, individual coordination bonds within the ENR/PCL matrix aggregate to form segregated phases, which is similar to the formation of ion clusters.29,33
Subsequently, the mechanical properties could be further improved by constructing the second cross-linked network based on the coordination interaction. The mechanical properties of the composites were gradually improved by increasing Fe3+ content. Interestingly, the tensile behavior of the composites changed dramatically when the Fe3+ content reached 2 phr. For example, PA0.5F2 showed the highest tensile strength and tensile toughness of 16.99 MPa and 28.43 MJ m−3 (Fig. S9†), which were 6.56 times and 2.32 times that of the ENR/PCL simple blend. The outstanding reinforcing efficiency of the coordination cross-linked network is mainly due to the improved energy dissipation,33 which will be further discussed in the subsequent section. When further increasing the Fe3+ content, a yield point could be found in the stress–strain curve of PA0.5F3, which was accompanied by the obvious improvement in the stress at 100% strain and E′ (Fig. S10†). A cross-linked network with a fairly high cross-link density (Fig. 3b) would cause the rigidification of the composites; thus, PA0.5F3 fractured quickly with the lowest elongation at break of 250%. Overall, PA0.5F2 exhibited better comprehensive mechanical properties, as it possesses a decent tensile strength without sacrificing its elasticity. The mechanical properties of the ENR/PCL/PA/FeCl3 composites exceed those of other reported ENR-based composites8–11,33,42–44 (Fig. 4b).
To understand the energy dissipation mechanism of the coordination cross-linked network, cyclic tensile tests were carried out on the samples of PA0.5F0, PA0.5F2, and PA0.5F3, as shown in Fig. 4c. The energy dissipation capability of the composites can be characterized through the hysteresis loop enclosed by the loading–unloading curve, in which the hysteresis energy is obtained by calculating the hysteresis loop area, as depicted in Fig. 4d. It can be found that the hysteresis energy increased with increasing Fe3+ content, disclosing that an impeccable second cross-linked network based on a coordination complex was formed to promote energy dissipation. On the one hand, the cross-link density of the composite was improved through the introduction of the coordination cross-linked network, resulting in a rigid network that resists the destructive effects of external force. On the other hand, the Fe3+-based coordination complex could act as a sacrificial component to dissipate energy more efficiently. When suffering external force, the coordination complex underwent reversible deformation and breaking-reformation processes, which could help dissipate energy and alleviate the stress concentration, preventing the premature failure of the covalent cross-linked network (Fig. 4e). Therefore, PA0.5F2 showed a hysteresis energy of 0.90 MJ m−3, which was nearly 4.29 times that of PA0.5F0. When further increasing Fe3+ content, the coordination bonds may be aggregated to form aggregations,33 inducing the plastic deformation and the mechanical “tough-brittle” transition of ENR/PCL components.
The fractured surfaces of the stretched PA0.5F0, PA0.5F2, and PA0.5F3 were observed via SEM and shown in Fig. 4f. As an elastomer with a single cross-linked network, PA0.5F0 would break quickly when the covalent cross-linked network fails, resulting in a relatively smooth fractured surface for PA0.5F0. However, a rough morphology could be found in the fractured surface of PA0.5F2, which was due to the Fe3+-based coordination preventing the premature failure of the covalent cross-linked network. A dramatic change could be found in the fractured surface of PA0.5F3, in which many stretched elastic microfibrils and obvious plastic deformation were formed during stretching. Meanwhile, the morphology along the tensile direction was also observed. Similar to the fractured surfaces, a rough morphology could be observed in the homoaxial surface of the composites (PA0.5F2), which was considered the typical morphology of reinforced elastomers.31 Furthermore, many obvious microfibrils with considerable length along the stretching direction could be found in PA0.5F3, providing the composites with enhanced modulus and improved tensile strength. Although this orientation of microfibrils could improve the tensile strength of PA0.5F3 to some extent, the mechanical “tough-brittle” transition would also deteriorate its elasticity (Fig. 4a) and increase its residual strain (Fig. 4c and S11†), which was contrary to our design target. Considering the best comprehensive mechanical properties of PA0.5F2, we will further explore its shape memory performance in the next section, aiming to design a composite with decent elasticity and shape memory properties.
The shape memory parameters, such as shape fixing ratio (Rf) and shape recovery ratio (Rr), were calculated according to our previous works, which are detailed in the ESI (Fig. S3†). Since the PCL phase was in a glassy state at room temperature, it could act as net points to hold the temporary shape, thereby restricting the elastic retraction of deformed ENR chains. Therefore, the shape fixing effect was significantly enhanced with the incorporation of PCL (Fig. S13†). For example, the Rf value increased from 31.00% of ENR vulcanizate to 81.33% of PA0.5F0 (Fig. 5c). The shape fixing effect could be further improved by introducing Fe3+. When adding 2 phr Fe3+, the Rf value of PA0.5F2 reached 96.30%, which was because the coordinate bonds could act as a second type of net point to restrict the mobility of ENR chains.
The ENR/PCL simple blends showed an inferior shape recovery effect with Rr of 83.33% (Fig. S13†), as the unvulcanized ENR relaxed during deformation and was insufficient to drive the recovery of the original shape. In comparison, the ENR/PCL elastomers demonstrated excellent shape recovery performance, with Rr exceeding 95% (Fig. 5d).
The ENR chains were cured by PA to form a three-dimensional cross-linked network, preventing stress relaxation during shape fixing, thus providing enough resilience to drive shape recovery when heated to its transformation temperature. With the incorporation of Fe3+, a dual cross-linked network consisting of phosphate esters and coordination bonds was constructed in the matrix, further improving the Rr value of ENR/PCL/Fe3+ composites. The composites maintained relatively high Rf and Rr with increasing strains, with all samples showing Rf over 95%, disclosing the stability in the shape recovery effect and a broad response strain range of the composites (Fig. S14†).
In our previous work, we found that the photothermal effect of NIR irradiation could only be generated at the irradiating region.20,31 Therefore, PA0.5F3 was taken as an example to record the temperatures of different spots under NIR irradiation. As shown in Fig. 6d, the irradiated focus (spot A) could be heated to 67.90 °C, while no obvious change in temperature could be found at spot C and spot D. The multistage shape recovery performance of the composites could be realized based on this characteristic. A ginkgo leaf-shaped specimen of PA0.5F2 was first folded at 60 °C and cooled to fix the temporary shape (Fig. 6e and Movie S1†). When the leaf was irradiated by NIR, it was heated to a temperature above the Tm of PCL to realize the blooming of this leaf, while other leaves without irradiation could maintain their closed shape. Other leaves could bloom sequentially when independently irradiated by NIR, displaying the multistage shape memory behavior of the composites. As shown in Fig. 6f, the shape recovery test of the composites under NIR irradiation was conducted, and the Rr values of the composites were calculated to evaluate the NIR-induced shape memory performance quantifiably. With the construction of the Fe3+-based coordination compounds, the composites could be heated above the Tm of PCL quickly to achieve shape recovery, realizing the Rr values of more than 86.00%. The composites maintained a high Rr value as the number of shape recovery cycles increased. For example, PA0.5F2 showed an Rr of 97.08% even after the third shape recovery cycle, demonstrating good reproducibility in the NIR-induced shape memory behavior.
Similarly, the ENR/PCL/PA/FeCl3 composites can also be indirectly heated by sunlight, which is beneficial for realizing the shape recovery behavior. As shown in Fig. 6g, the composite sheet was custom-made as a fish and stretched to a temporary shape, and then the fish was heated by a sun simulator to induce shape recovery (Movie S2†). The Rr values of the composites under sunlight irradiation were also calculated and shown in Fig. 6h. It could be found that the tendency of the Rr values under sunlight was similar to the Rr values under NIR irradiation. PA0.5F2 showed an Rr of 93.57% under a stretched shape (100% strain) and 98.48% under a folded shape, demonstrating the outstanding light-induced shape memory behavior of the composites.
Based on the outstanding photothermal effect of the ENR/PCL/PA/FeCl3 composites, a PTEG integrated with a Seebeck thermoelectric generator, a heat sink, and a PA0.5F2 film was designed to explore the potential application in photo-thermoelectric conversion, as shown in Fig. 7d. When exposed to the sun simulator, PA0.5F2 film quickly generated heat and transferred it to the upper surface of the thermoelectric generator, leading to a temperature difference between the different sides of the generator. Therefore, an open circuit voltage was generated based on the Seebeck effect (Fig. 7e). The output voltage of the PTEG system increased rapidly to reach its stable value of ∼0.41 V under exposure to sun irradiation (0.20 W cm−2). Similar to the repeatability of the temperature curve (Fig. 7b), the output voltage maintained good reproducibility after 5 cycles of switching sun irradiation (Fig. 7f). Meanwhile, the output voltage upon sun irradiation could be controlled by varying the power of the sun simulator (Fig. 7g). The above results disclosed a highly efficient photo-thermal-electrical conversion system based on the ENR/PCL/PA/FeCl3 composites. Subsequently, the fabricated photo-thermoelectric generator was utilized to rotate a small fan (Fig. 7h and Movie S3†), which could be applied to improve the working environment for couriers (Fig. 7i).
Footnote |
† Electronic supplementary information (ESI) available: Supporting tables, and figures. See DOI: https://doi.org/10.1039/d5ta03812j |
This journal is © The Royal Society of Chemistry 2025 |