Beatrice
Tosetto
abc,
Roberto
Mo
c,
Candido Fabrizio
Pirri
ac and
Ignazio
Roppolo
*ac
aDepartment of Applied Science and Technology, Politecnico di Torino, Corso Duca degli Abruzzi 24, Turin 10129, Italy. E-mail: ignazio.roppolo@polito.it
bDepartment of Chemistry, Biology and Biotechnology, University of Perugia, Via Elce di Sotto 8, 06123, Perugia, Italy
cCenter for Sustainable Future Technologies, Italian Institute of Technology, Via Livorno 60, 10144 Turin, Italy
First published on 4th December 2024
Since the last century, plaster of Paris bandages have been the gold standard for orthopedic casting. Despite their extensive use, they have several drawbacks in day-to-day life, such as high weight and sensitivity to water. Moreover, they can cause skin burns, pressure sores, and other complications. Consequently, the urgency to propose alternative materials to solve these problems has emerged in the last decades, leading to the so-called soft casts, especially in pediatric orthopedics. In this context, a photocurable composite, based on the impregnation of a medical net with epoxy resins, is presented here. The impregnated medical net was rapidly transformed into a rigid device by means of visible light irradiation with an ad-hoc designed LED lamp (410–420 nm). Reaction activation was shifted to the visible range by exploiting isopropyl-9H-thioxanthen-9-one (ITX) as the photosensitizer, and the composites’ polymerization was evaluated via FT-IR analyses and thermal camera monitoring. The composites were also tested through tensile and three-point bending tests, revealing a stiffness comparable to that of soft casts already on the market. Compared to commercially available photocurable casts, this work introduces two key innovations: first, the employment of commercially available epoxy resins (monomer: 3,4-epoxycyclohexylmethyl 3,4-epoxycyclohexanecarboxylate), which enables avoiding the problems of oxygen inhibition; second, the use of a tubular medical net that is stretchable along the transversal direction, which is already used in the medical field for medication positioning. This latter advancement simplifies the application process compared to conventional techniques, making the obtained casts easy and fast to apply, light and breathable, thus maintaining promising properties for orthopedic rapid soft casts.
Consequently, the necessity of further evolution in the cast properties emerges clearly, and the required characteristics include but are not limited to, easy procedures to apply and remove the cast, fast hardening with a controllable hardening window, lightweight, radiotransparency, tunable rigidity, waterproof and breathability. Many of those characteristics were recently fulfilled by the use of photocurable casts.1
Photocurable casts are composed of a monomeric formulation that can be polymerized through light irradiation, resulting in a fast hardening. This allows the technicians to place the casts without rushing and close the cast windows when decided. Photocurable casts are already commercially available and are mainly based on combining acrylates and methacrylate with different kinds of specifically designed textile supports, made of glass fiber, nylon, PTFE, PET, rayon, or cotton.9–15 Those casts have advantages related to curing speed and lightweight, however, similar to most radical polymerization processes, suffer from oxygen inhibition, i.e. the polymerization is quenched when in contact with oxygen.16–19 This is obviously a strong limitation in view of cast application and it is necessary to confine the resins in volumes not in contact with oxygen, making the support design complex and typically leading to the subdivision of casts in sizes, limiting the customizability and the ability to fit the patient limb properly.9 Different from (meth)acrylic resins, epoxy resins may be polymerized by a cationic photoinduced mechanism, which is not prone to oxygen inhibition.16,17,20–22 In this context, the use of epoxy in casts can make the design simpler, more versatile and potentially applicable to everyday life. Moreover, epoxies give lower shrinkage during polymerization (5% vs. 10–15% for acrylates and methacrylates), which may represent a further advantage compared to more conventional photocurable casts, due to lower stresses and lower limb compression.18,19,22,23 Nevertheless, epoxy resins have other drawbacks that must be overcome in view of the development of rapid photocurable orthopedic cast. The first one is that the cationic mechanism is slower than the radical polymerization; therefore, an optimization of the formulations and the curing conditions is crucial.20,23 Furthermore, the available cationic photoinitiators can be mainly activated by UV light irradiation,24,25 which can be hazardous for the human skin; consequently, a shift to visible light is strongly recommended.26–28 To this purpose, it is necessary to shift the absorption of the formulations towards higher wavelengths, and this is possible by employing photosensitizers (PhS).17,23,24,29
In this work, an innovative strategy is reported to develop photocurable soft casts employing a medical elastic and tubular net impregnated with epoxy resins. Among the possible monomers, cycloaliphatic epoxy resins (CE) are well-known for their good mechanical performance, high polymerization rate and lower tendency to yellowing when exposed to sunlight.23,30,31 Furthermore, it does not contain bisphenol A. To obtain fast and visible-induced curing, as well as suitable mechanical properties, different photoinitiators (PhI) and photosensitizers (PhS) were studied, and the optimized formulation was then used to impregnate a medical net to obtain a rigid mesh after irradiation.32–36 In this sense, the elastic medical net employed is already used for medication and consequently assures conformability when applied to human skin. Moreover, thanks to its tubular and transversally stretchable design, an easier application is guaranteed, compared to the standard cast application, which in turn leads to the possibility of dressing the net without requiring it to be wrapped around the limb. Finally, a desired number of net layers can be applied to the injured part, allowing better control of the mechanical properties of the soft cast.
In this study, photocurable composites were developed, showing promising results for the application of orthopedic rapid soft casts, and two main innovations are proposed: employing (i) epoxy resins and (ii) a tubular medical net stretchable along the transversal direction. These innovations facilitate the cast design compared to other photocurable casts and will simplify the application process compared to conventional techniques, making the obtained composites, light, breathable, and easy and fast to apply.
Final width = initial width × (1 + stretching level) | (1) |
PhI | PhS | Single layer composite | |||
---|---|---|---|---|---|
Name | phr | Name | phr | Irradiation timea | Stiffnessb |
a Irradiated with white broad band light (Hamamatsu lamp) with an intensity of 130 mW cm−2. b Composites’ stiffness describes the PhI/PhS class, and the stiffer composite for each combination is reported in bold. | |||||
Iod I | 6 | ITX | 2 | 90 s | Not self-standing |
6 | ITX | 4 | 90 s | ||
9 | ITX | 4 | 90 s | ||
9 | ITX | 6 | 90 s | ||
Solf | 4.6 | ITX | 2 | 4.5 min | Not self-standing |
4.6 | ITX | 4 | 4.5 min | ||
6.9 | ITX | 4 | 4.5 min | ||
BTB | 3 | ITX | 2 | 230 s | Not self-standing |
3 | ITX | 4 | 280 s | ||
5 | ITX | 2 | 100 s | ||
5 | ITX | 4 | 100 s | ||
T67 | 2.1 | ITX | 2 | 50 s | Self-standing (stiff) |
2.1 | ITX | 4 | 130 s | ||
4.2 | ITX | 2 | 50 s | ||
4.2 | ITX | 4 | 150 s | ||
Solf | 4.6 | C | 2 | 6 min | Self-standing (quite stiff) |
4.6 | C | 4 | 9 min | ||
6.9 | C | 4 | 9 min |
When multi-layer specimens were prepared, the desired number of soaked medical net layers were deposited. Finally, all the polymeric and composite samples were cured using light irradiation according to the parameters described in the text. Four different lamps were employed: UV(-01A) and broadband white light (-03) Hamamatsu LC8 lamps, Solar Simulator (Newport, Oriel Instrument U.S.A., 91191A-1000), and an ad-hoc designed lamp operating with LS-XC06-S410-SD111 LEDs (Intelligent LED Solutions). Further details on the LED lamp design are reported in the ESI.† In the case of cylindrical samples cured with the ad-hoc design lamp, photocuring was performed in three irradiation steps, rotating the lamp around the specimens. These steps overlap subsequent curing areas to avoid low polymerized transitions.
(2) |
The temperatures developed during light irradiation were monitored with a thermal camera on the irradiated surface and through thermal probes on the opposite side. The thermal camera employed is FLIR E6-XT (thermal resolution: 240 × 180 pixel; accuracy: ±2 °C or ±2%; thermal sensitivity/NETD < 0.06 °C/<60 mK; temperature range from −20 °C to 550 °C) and was placed at 30 cm from the analyzed surface. The thermal probes Thermo Scientific™ PT100 External Probe (0–400 °C) were placed on the preform, and two different isolation levels were used to prevent direct contact with the soaked net: (#A) two layers of 80% stretched medical net or (#B) two layers of cotton stockinette plus one layer of 80% stretched medical net. The employed isolation level for each measurement is reported in the text.
Traction tests were performed using a MesdanLab mechanical testing machine at a 10 mm min−1 stroke rate on five single-layer and four double-layer composite strip samples (1 × 20 cm2; gauge length: 140 mm), 12 days after irradiation. Elastic modulus was evaluated as the slope of the linear part of stress-deformation curves (linear fit R2 > 0.99); the Yield Stress was calculated with the 0.2% offset method, and the Ultimate tensile strength (UTS) was evaluated as the maximum stress sustained. The average value and the standard deviation were calculated for each parameter and the group. The properties (P) variation between double-layer (DL) and single-layer (SL) composite was evaluated by eqn (3).
(3) |
Three-point bending tests were performed using a Zwick Z005 TN mechanical testing machine at a stroke rate of 2 mm min−1, with a support span of 100 mm. The tests were performed on different materials two months after the preparation of the cylindrical samples (diameter: 5 cm, length: 25 cm). The tested samples are (i) five double-layer composite samples, (ii) one sample of POP, and (iii) one of FGC. Photocured composite samples were performed with a two-cycle load. The Initial Stiffness was evaluated as the slope of the linear part of force-deformation curves (linear fit R2 > 0.96), and the Yield Force was assessed using a 0.25 mm offset method, as performed by Zmurko et al.6
(4) |
Fig. 1 (a) UV-visible spectra of CE-based formulation with and without additives; (b) picture of a 2.1 T76/2 ITX composite cylindrical sample with a net's stretching of +80%. |
After preliminary testing, the most promising formulations were tested to impregnate the medical net (Table S2†). Noteworthily, different formulations were prepared by changing the components’ amount, aiming at optimizing the polymerization process and evaluating their effect on the composite stiffness. Table 1 reports the formulations tested, curing parameters and the obtained results. The composites based on Iod I/ITX, BTB/ITX, and Solf/ITX were demonstrated to be flexible after curing, indicating that those are not suitable for the application as photocurable casts. Instead, the systems T67/ITX and Solf/C allowed the production of composites with promising rigidity; among the tested combinations, one with 2.1 T67/2 ITX appeared to be the most rigid. It must be noted that the differences between the samples were easily distinguishable just by handling them, therefore this preliminary screening was merely qualitative. Conversely, mechanical testing was performed only on the final formulation, as detailed later. The stretchability of the medical net used determines another important parameter in designing composites for the application of orthopedic casts. This is because the net's stretching modifies the mesh size, which determines a variation in the filled/void ratio of the composite's cross-section; characteristics such as breathability and stiffness are both affected by that parameter, even if there is an opposite relation, and this peculiar behavior can be exploited to customize the rigidity in different cast sections, fitting at best the specific requirements. For this reason, a last screening evaluation was performed and aimed at assessing the more suitable net stretching, as a trade-off between stiffness and breathability. Four different 2.1 T67/2 ITX composite samples were prepared with different stretching of the net (+26%, +46%, +80%, +130%). Self-standing tests indicate that a +130% stretching was too high, with a loss of rigidity. Consequently, 80% was selected as the standard stretching level for the following tests and considerations, since it was the highest that guaranteed promising mechanical performance. A photocured sample with this stretching level is reported in Fig. 1b.
Having fixed the optimum conditions (2.1 T67/2 ITX formulation, stretching level of 80%), the polymerization process was studied and characterized in detail. To this aim, a visible broad band white light source (Hamamatsu lamp) was used, and the conversion degree (CD) was followed by means of FT-IR analyses. Furthermore, in these tests, both single- and double-layer specimens were studied, to evaluate the effect of the soft cast thickness in the photopolymerization process.
Table 2 summarizes the testing parameters and the CD (spectra reported in Fig. S1 and S2†). The obtained CDs range between 66% and 96% on the directly irradiated surface, depending on the curing conditions. As expected, the CDs of the two sides (the directly irradiated and the opposite ones) are consistently different in the samples according to their thickness, with a measured decrease of CD ranging from −8% (single layer) to −24% (double layer). This is obviously due to the light absorption along the composite thickness and this difference is more evident in the double-layer composite (#Double) since the increased thickness limits the light penetration and hinders the polymerization. Moreover, single-layer composites were produced with two energy doses (#Single_LD – low dose- and #Single_HD – high dose), and they resulted in a significant difference in the perceived stiffness. This difference reflects the difference in their CDs (Table 2), which are 88–96% in the latter vs. only 66–77% in the former.
Sample name | No. of layer (−) | Light intensity (mW cm−2) | Irradiation time (s) | CDa (%) | |
---|---|---|---|---|---|
DIb | NIc | ||||
a FT-IR measurement performed 1 hour after irradiation. b Directly irradiated side. c Not irradiated (opposite side to the irradiated one). | |||||
#Single_LD | 1 | 40 | 50 | 77 | 66 |
#Single_HD | 1 | 130 | 50 | 96 | 88 |
#Double | 2 | 130 | 180 | 66 | 50 |
Moreover, epoxy resins undergo a well-known phenomenon known as dark curing, which consists of the evolution of polymerization reaction also after irradiation. This is related to the fact that cationic polymerization is a semi-living polymerization, in which final conversion is determined by chain mobility rather than termination mechanisms.18,22,23,41,42 Consequently, the CD was monitored for one month on the already analyzed specimens (Fig. 2a and Table S3,† and spectra in Fig. S1 and S2†). The results indicate that, although in some curing scenarios limited CD was reached 1 hour after the irradiation, all the tested cases showed a CD higher than 80% after 6 hours and higher than 89% in 1 month. Interestingly, the investigations showed that the difference between the two sides of the specimens tends to disappear, meaning that polymeric characteristics tend to be homogeneous with time. On the other hand, differences depending on the energy dose were still evident after 1 month (#Single_LD: 89%, #Single_HD: 97–100%), confirming that an optimization of the curing parameters is crucial to obtain rigid composites to be employed as orthopedic casts. Related to the double-layer sample, observing the CDs evaluated 1 hour after irradiation on both surfaces, their values indicated low polymerization, even lower than the #Single_LD sample. However, after 6 hours, the measured CD overcame those values, becoming more similar to #Single_HD. Consequently, despite the polymerization being hindered by the increased thickness, the curing conditions employed led to a proper reaction. However, in the double-layer composites, the irradiation time is strongly increased compared to single-layer samples, therefore two is the maximum number of evaluated layers in this work, to avoid an extremely long curing process.
Fig. 2 (a) Change in the conversion degree over one month, and (b) maximum temperatures developed on the irradiated side of 2.1 T67/2 ITX composites samples. |
Unfortunately, uncured resins could potentially cause skin irritation. To prevent this, the presence of an insulating layer is suggested, it is useful also to avoid the adhesion of the composite on the skin and to control the temperature perceived by the user. However, this part will be better discussed later in the text.
In addition, it is well-known that epoxy curing is an exothermic process; therefore, the exothermicity of the reaction can give an indication of the photopolymerization process but, for the envisaged application, it can be harmful to the human body. For this reason, the temperatures generated on the irradiated surface during the polymerization were monitored employing a thermal camera (Fig. 2b). Those measures highlight the effect of the light dose on the single-layer composite's polymerization, demonstrating that when the intensity is higher, the polymerization process is faster, as confirmed by the high developed temperature. In the double-layer sample, the effective activation was confirmed by the temperatures developed, which are consistently higher than the ones developed in #Single_LD, and more similar to #Single_HD. These results are consistent with the previously discussed increased CDs, so temperature monitoring was revealed to be a proper test to estimate the ongoing polymerization reaction.
FT-IR analyses and temperature measurements demonstrated that an optimization of the curing parameters is crucial to obtaining rigid composites to be employed as orthopedic casts. This procedure aimed to match the applications’ requests as the orthopedic cast; namely, low curing time and high polymerization efficacy were pursued. For this reason, the curing conditions were selected for broad band visible light sources in order to have a CD of (at least) 85–90%, 6 hours after irradiation (Table S5†). It is important to highlight that, even if low conversion degree may be obtained right after the irradiation, dark curing will ensure complete polymerization in a few hours. The optimized curing parameters are reported in Table S4.† This procedure was also conducted for another light source, solar simulator, due to the necessity of fabricating specimens with dimensions sufficient for following characterization; in fact, the Hamamatsu lamp has a spot size of around 1–2 cm2 at the required intensity, which is unsuitable for the production of homogeneous bigger samples for mechanical testing.
Consequently, mechanical properties were evaluated. Tensile tests were performed on single- and double-layer composites cured with the optimized curing conditions, and relevant results are reported in Table 3 and Fig. S4.† As predicted, the double-layer composites show an improvement in their mechanical properties compared to single-layer composited: the elastic modulus reaches an average value of 221 ± 28 MPa vs. 187 ± 51 MPa; thus, an improvement of +18% is obtained. Furthermore, yield stress was measured respectively as 1.78 ± 0.12 vs. 1.4 ± 0.24 MPa, with an improvement of +27%. Interestingly, after increasing the number of layers, the dispersion of the values obtained for elastic modulus and yield stress parameters decreased by 45–50%, meaning that the reliability of the composite improved. Comparing those results to Plaster of Paris and Fiber Glass performance reported in the literature, the elastic modulus of the photocured double-layer composite is considerably lower than POP (6-layer samples: 2590 ± 708 MPa), while it has the same order of magnitude of FGC despite the lower layers’ number (4-layers FGC samples: 316 ± 15 MPa), which revealed to be enough for the orthopedic application.43
Compositesa | Single- vs. double-layer variation | |||
---|---|---|---|---|
Single-layerb | Double-layerc | |||
a Irradiated with a solar simulator (curing parameter in Table S4†) and tested 12 days after irradiation. b 6 samples were tested. c 5 sample tested. | ||||
E [Mpa] | Average | 187 | 221 | +18% |
Stand. dev. | 51 | 28 | −45% | |
UTS [Mpa] | Average | 1.43 | 1.88 | +31% |
Stand. dev. | 0.23 | 0.12 | −48% | |
Yield stress [Mpa] | Average | 1.40 | 1.78 | +27% |
Stand. dev. | 0.24 | 0.12 | −50% |
Beyond tensile, three-point bending tests were also performed. To assess a solicitation scenario that was more similar to the real one, the measurements were performed on cylindrical double-layer samples having a dimension comparable to a real limb cast. Nevertheless, the fabrication of such specimens needed a last modification of the irradiation set-up: the sun simulator was replaced with an ad-hoc designed lamp that can irradiate larger surfaces and be portable, thus making it more suitable in view of orthopedic uses. More details are reported in the ESI,† and the optimized curing conditions with this lamp are reported in Table S9.† The reaction of the samples described in Table S8† was followed by monitoring the external temperatures, as reported in Fig. S6.† The values obtained show a significant difference between each irradiation step (three were required to ensure covering the whole cylinder surface), with a consistent reduction of the maximum temperature reached in the last step. This can be related to the fact that the composite is already partially polymerized in the overlapping areas, especially in the last step of the Double_LED_210s samples.
Once those specimens were produced, whose pictures are reported in Fig. 3a, three-point bending tests were performed in order to compare the properly cured specimens (Double_LED_210s) with the ones obtained with non-optimal parameters (samples Double_LED_90s). Load vs. deformation curves are shown in Fig. 3b and Fig. S7b,† while the mechanical properties are summarized in Table S10.† Samples Double_LED_210s_#1, Double_LED_210s_#2, and Double_LED_210s_#3 show an initial stiffness of 5.21 ± 1.08 N mm−2 and yield stress of 2.52 ± 0.56 N, confirming, as expected, better mechanical properties than those of the composites cured with non-optimal parameters (Double_LED_90s samples: initial stiffness: 1.90 ± 0.55 N mm−2, yield stress: 3.44 ± 0.79 N). Interestingly, three-point bending tests on samples Double_LED_210s_#4 and Double_LED_210s_#5 gave results similar to those on Double_LED_90s samples, initial stiffness: 2.26 ± 0.12 N mm−2 and yield stress: 3.28 ± 0.24 N; to better understand this phenomenon, their external temperatures monitoring results were recalled (Fig. S6†). Noteworthily, those particular specimens did not reach the high temperature developed by the other Double_LED_210s samples, probably due to inhomogeneous resin distribution. This confirms the correlation between the external temperature developed, and consequently the extent of polymerization, and the composites’ mechanical properties. To describe in detail, Double_LED_90s samples show similar and low maximum temperatures to Double_LED_210s_#4 and Double_LED_210s_#5 (1st step: <130 °C, 2nd step: <90 °C, 3rd step: <60 °C), and this result in similar weak behavior in the bending test (initial stiffness: 1.34–2.38 N mm−2). Instead, samples Double_LED_210s_#1 and Double_LED_210s_#2 developed higher temperatures in both the first and the second steps (1st step: <180 °C, 2nd step: <130 °C, 3rd step: <60 °C), resulting in stronger composites (Initial Stiffness: 4.95–6.65 N mm−2). Confirming this trend, samples Double_LED_210s_#3 developed intermediate temperatures (1st step: <130 °C, 2nd step: <130 °C, 3rd step: <60 °C) and resulted in intermediate strength (initial stiffness: 4.04 N mm−2).
Fig. 3 (a) Picture of 2.1 T67/2 ITX double-layer composites; (b) load vs. deformation of the cured cylindrical double-layer composites irradiated with LED lamp, including multiple testing. |
Overall, well-cured double-layer cylindrical samples show an initial stiffness of 5.21 ± 1.08 N mm−2 and a Yield stress of 2.52 ± 0.56 N, and those values were compared to POP and FGC samples prepared by a registered orthopedic technician with the proper amount of layer required for the materials (>6 for POP and >4 for FGC) and tested under the same conditions. Their initial stiffness resulted in 333 N mm−2 and 72 N mm−2 respectively for POP and FGC, while the Yield stress is 23 N and 40 N; those values are quite consistent with literature data, with a reasonable variation related to the operator.6 Despite the lower mechanical properties shown by the photocured composite presented here, its application as a rapid orthopedic cast is still appealing because it shows similar bending behaviors to a Soft Cast applied in a higher number of layers (4–10 layers Initial Stiffness: <10 N mm−2, 4–6 layers Yield stress <10 N).6 Moreover, the presented photocured composites showed an additional advantage compared to the conventional casting technique, since they recover their initial shape after the load removal, while POP and FGC cast are irreversibly deformed. For this reason, the analyzed specimens were tested with a second cycle of load application in the same three-point bending test condition right after the first load cycle. Interestingly, they preserve 76 ± 13% of their initial stiffness despite the failure in the test's first cycle, meaning that the cast will still provide support to the injured part in the case of traumatic events.
However, as already mentioned in this study, the curing of the epoxy resins is an exothermic process, and the developed temperature can be harmful for the application on human skin.
External temperature monitoring has been previously discussed, but it is reasonable to assume that the perceived temperature will be that of the side of the soft cast closer to the skin, which is not the side previously analyzed. For this reason, the internal temperatures developed were monitored through thermal probes directly applied on the preform during the polymerization of single-layer cylindrical composites. These measures were conducted in two different thermal insulating conditions: the first scenario consists of 2 layers of clean medical nets having a stretching of +80%, not impregnated with resins (#A). This option should give a minimum insulating level, simply preventing skin irritation and adhesion with the composite. The second scenario was instead designed with 2 layers of cotton stockinette and a layer of clean medical net (stretching level of 80%) to keep the stockinette in the right position and facilitate the application of the soak layer and hopefully provide a partial thermal insulation (#B). The results of those scenarios are reported in Fig. 4a and b.
In scenario #A, the peak temperatures developed are under 85 °C, which are considerably lower than the temperatures reached externally (180–200 °C). However, despite this drop in temperatures, those values are still too high for applications on the human skin. For this reason, the second insulation scenario was analyzed, and the maximum temperature measured by the thermal probes was 53–59 °C. In summary, in the second configuration (i) the reached maximum temperature decreases by 12–30% (60–85 °C vs. 53–59 °C), (ii) the time needed to reach the maximum temperature increases by 45–67% (55–60s vs. 80–100s), (iii) the period in which the preform stay at temperatures higher than 40 °C slightly increases (220 s vs. 240 s). The second configuration was also tested with double-layer composites (Fig. 4c). Also in this case, the maximum temperatures developed are around 53–58 °C as for the single-layer composite, but the period in which the preform stays at temperatures higher than 40 °C is more than 6 minutes. Analyzing those results, it clearly emerges that a more efficient insulation must be designed in view of the application of this study.
Finally, a last preliminary investigation was conducted to assess the composite's response to harsh conditions, such as direct sun exposure, cold or hot humid environments, and soaking in water, because those conditions can frequently occur if the composite is applied as an orthopedic cast. Cylindrical double-layer samples were exposed to such conditions for two hours and then the mass variation was monitored for 24 hours, as well as the samples’ perceived stiffness. No rigidity changes were registered, and the mass variation, summarized in Table S11† indicates that only water immersion caused a significant weight increase; still, most of the absorbed water can be eliminated in one hour and completely removed in less than one day.
One limitation identified in this study is the elevated temperature developed during the photocuring process, which may be potentially harmful to the user. Temperatures of up to 200 °C are reached on the irradiated surface, however, they decrease significantly across the device thickness, down to under 85 °C on the skin side. Clearly, this temperature is still not acceptable for patients, and the use of an insulating layer was suggested. The presence of this layer allows to reduce the maximum internal temperature by a further 12–30%; however, to ensure the composite's suitability for real applications, a more efficient thermal insulation system must be designed. Additionally, this insulating layer also prevents contact between the skin and the uncured resin, avoiding undesired effects on the skin.
To conclude, the approach proposed simplifies the application process compared to conventional techniques, resulting in casts that are light, breathable, and easy and fast to apply.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4lp00248b |
This journal is © The Royal Society of Chemistry 2025 |