Shumin Bi†
a,
Yueru Yang†a,
Guangling Peia,
Tianci Yangb,
Shui Hu*b and
Qingxiu Jia
*a
aSchool of Materials Design and Engineering, Beijing Institute of Fashion Technology, Beijing, China. E-mail: clyjqx@bift.edu.cn
bCollege of Materials Science and Engineering, Beijing University of Chemical Technology, Beijing, China. E-mail: hushui@mail.buct.edu.cn
First published on 14th January 2025
Unidirectional moisture-conducting fabrics were prepared by electrospraying polyvinylidene fluoride (PVDF) and polyvinyl chloride (PVC) onto three green fabric substrates, namely cotton, hemp, and modal. Experiments were conducted to examine the effects of coating thickness, coating material, and substrate material on the moisture conductivity of the fabrics. The electrospraying technique was effective in forming uniform and strongly adhered PVDF and PVC coatings on the fabric substrates, and the coating thickness and material type had a significant effect on the fabric's moisture conductivity. The PVDF and PVC coatings significantly improved the unidirectional moisture conductivity of the fabric substrates, and although the unidirectional moisture conductivity effects differed among the substrates, all fabrics exhibited high directional water transport capacities (R values greater than 300%), high air permeabilities, and high water vapor transmission rates. Cotton and hemp substrates coated with hydrophobic layers showed more efficient unidirectional moisture transfer than modal fabrics. This study demonstrated that appropriate coating design and substrate selection can significantly improve the moisture conductivity of fabrics, providing a valuable reference for the development of high-performance functional textiles.
The process of directional water transfer mainly depends on the asymmetric wettability of the material.5,6 There are two main methods to develop unidirectional moisture-conducting fabrics. One is to rationally design the fabric structure by combining hydrophobic fibers with hydrophilic fibers and constructing a wetting gradient or differential capillary effect by adjusting the thickness.7,8 The other is to construct a wettability gradient by modifying the textile surface through finishing processes, such as single-sided coating,4,9,10 plasma treatment,11,12 laser modification,13 and electrospinning.5,14,15 Most commercially available moisture-conducting fabrics rely on the composite or post-finishing technology of polymer materials, which have poor environmental protection and involve complex processes. Therefore, it is necessary to develop an efficient and simple method for manufacturing moisture-conducting fabrics.
Electrostatic spraying (i.e., electrospraying) is an advanced process widely used in the field of coating. It enables the on-demand deposition of functional materials16 and has the advantages of high efficiency, uniformity, and material savings. Electrospraying provides a uniform coating on the surface of textiles and enhances the bonding force between the coating and the substrate,17 thereby imbuing textiles with additional functionality. Moreover, the charge of the droplets can be controlled by changing the voltage and flow rate, thereby adjusting the coating thickness, which is significant in the construction of functional fabrics, particularly unidirectional moisture-conducting fabrics.18
There are several reports on the preparation of unidirectional moisture-conducting textiles by electrospraying. For example, Chen et al.19 prepared high-performance directional water-conducting textiles using a three-step strategy that involved electrospinning oriented polyacrylonitrile on polylactic acid nonwoven surface, dipping the fabrics in hydrophilic reagents, and electrospraying polyvinylidene fluoride (PVDF) solution on one side of the fabric. The prepared hydrophilic oriented polyacrylonitrile (HOPAN)/hydrophilic polylactic acid @polyvinylidene fluoride (HPLA@PVDF) fiber membrane exhibited high directional water transport performance (accumulative one-way transport capacity (R) = 1117%, overall moisture management capacity (OMMC) = 0.91). Cheng et al.20 combined electrospinning and electrospraying to prepare Janus textiles, which consisted of hydrolyzed polyacrylonitrile (HPAN)/hexagonal boron nitride nanosheets (BNNS) fibrous membrane with small pores and hydrophilicity, conductive Ag nanowire (NW)layer and polyurethane (TPU) nanofibrous membrane with large pores and hydrophobicity. The textiles showed a dual gradient in terms of the pore size and wettability in the thickness direction, achieving directional perspiration performance. These recent studies have mostly used electrostatic spraying technology in combination with other methods. Although previous studies have used one-step electrospraying techniques to prepare unidirectional moisture-conducting fabrics, they focused on the quantitative analysis of the liquid transport performance, such as changing the thickness of the hydrophobic coating and the pore size of the hydrophilic fabric substrate.21,22 Notably, there is a lack of reports that comprehensively investigate the effects of coating type, fabric substrate type, and coating thickness on the performance of unidirectional moisture-conducting fabrics.
In this study, three different types of green hydrophilic fabrics, namely cotton, hemp, and modal, were used as substrate materials. A simple and efficient one-step electrospraying technique was employed to form a hydrophobic coating on one side of these fabrics, creating a significant wetting gradient difference between the two sides. The feasibility of achieving unidirectional moisture-conducting performance in the fabrics via electrospraying was systematically verified, providing new insights for the development of multifunctional green unidirectional moisture-conducting textiles.
The fabric to be treated was soaked in 500 ml of deionized water until it was completely wetted and then suspended until no liquid droplets fell. Subsequently, the fabric was fixed on the electrospinning receiving roller. A certain amount of spinning solution was injected into a 10 ml syringe, and the distance between the needle and the receiving roller was set to 15 cm for PVC spinning solution and 12 cm for PVDF spinning solution, respectively. The solution was electrosprayed onto the fabric at a propulsion speed of 1 ml h−1 and a voltage of 12 kV, and the electrospraying time was set to 1, 2, and 3 h. Thus, the composite fabrics with asymmetric wettability were obtained. The fabrics were named PVC-C-x, PVC-H-x, PVC-M-x, PVDF-C-x, PVDF-H-x, and PVDF-M-x, where x represents the electrospraying time, and C, H, and M denote cotton, hemp, and modal, respectively.
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Fig. 1 Illustration of the process used for preparing and analyzing unidirectional moisture-conducting composite fabrics. |
To analyze the chemical characteristics of the original fabric and composite fabric surfaces, FTIR analysis was performed (Fig. 2(b)). In the infrared spectra of all three fabrics, characteristic peaks were observed in the 3000–3500 cm−1 region, which were attributed to the –OH stretching vibration in cellulose. However, the shape and intensity of the peaks significantly changed after electrospraying treatment. After electrospraying PVC on the surface of cotton and modal fabrics, –OH may form various hydrogen bonds with PVC molecules and exert van der Waals forces, causing the characteristic peak to broaden. After electrospraying PVDF, the characteristic –OH peak weakened, which may simply occur because the fibers are covered. For hemp fabrics, both treatments lead to the broadening of the characteristic –OH peak and its shift in the lower wave number direction. At the same time, the peak intensity of each composite fabric after treatment was significantly enhanced near 1640 cm−1. The broad and weak absorption peak seen here in untreated fabrics is generally attributed to the effects of water molecules and intramolecular hydrogen bonds in cellulose. When PVDF or PVC is coated on the fabric surface, the formation of intermolecular hydrogen bonds enhances the absorption peak. In addition, the CO bonds present in PVC may shift because of changes in the chemical environment and overlap with the absorption peak at 1640 cm−1, further enhancing the peak. For PVDF composite fabrics, characteristic peaks can be observed at 1401 and 1159 cm−1, corresponding to the –CH2 bending vibration and –CF2 tensile vibration, respectively. The absorption peaks at 876 and 838 cm−1 are caused by the crystalline phase in PVDF, which is consistent with the literature.23 These results indicate that the polymer is successfully attached to the fabric surface.
The elemental composition of the fabric surface was analyzed by EDS, and the results are shown in Fig. 2(c) and (d). According to the molecular structure of cellulose, it mainly contains C and O elements. After PVDF modification, F appeared on the fabric surface, which is unique to PVDF. Similarly, Cl appeared on the surface of the fabric after PVC modification. Furthermore, the results show that the elements are evenly distributed on the composite fabric surfaces.
As shown in Fig. 3(a)–(f), the wettability of the fabric is affected by the thickness of the hydrophobic film. Nonetheless, the water droplets can be completely absorbed on the surface of all samples. Among them, the modal-based composite fabric provided faster absorption than the other two substrate materials. The water droplet disappearance times on PVC-M-1, PVC-M-2, and PVC-M-3 were 0.3, 0.3, and 6 s, and the water droplet disappearance times on PVDF-M-1, PVDF-M-2, and PVDF-M-3 were 0.7, 0.6, and 0.4 s, respectively. This is because the moisture absorption performance of the modal fabric is high, and the water droplets falling on the fabric surface are immediately absorbed and diffused. Notably, it is not possible to use this test to determine the unidirectional conduction efficiency of these fabrics. However, when the water droplets fall on PVC-M-3, water droplet penetration can be observed.
Except for the modal-based composites, the water droplets falling on the hydrophobic side surface of the other composite fabrics remain spherical for some time and then vertically penetrate the fabric. As the electrospray time increases from 1 to 3 h, the disappearance time of the water droplets gradually shortens. Moreover, the thickness of the original cotton, hemp, and modal fabrics are 255.9, 249.2, and 522.0 μm, respectively (Fig. 3(g)–(i)). The thicknesses of the cotton and hemp composite fabrics increase with the extension of the electrospraying time, and the WCA on the spraying side also increases. Although the thickness of the modal composite fabric increases with the increase of the spraying time, the WCA remains at 0° owing to the high absorption rate. Additionally, compared with cotton and hemp fabrics, modal fabrics have more microporous structures inside. These tiny gaps can absorb and accommodate more water molecules, contributing to its hygroscopicity. The synergistic effect of absorption and penetration prevents water droplets from remaining on the fabric surface for even a short time. The introduction of both polymers effectively improves the WCA of the substrate material, and when the coating content increases, the hydrophobicity increases. The longer the spraying time, the more that the pores of the fabric become covered, which may effectively prevent the penetration of water molecules and enhance the hydrophobic performance. According to the Young–Laplace equation, the reduction in pore size leads to an increase in the Laplace force, thereby repelling water droplets, which means that the wettability gradient across the fabric is enhanced. In addition, from the morphology of the fabric, electrospraying results in a rough surface layer, thus forming a roughness difference in the thickness direction of the fabric. This roughness difference and the surface energy gradient both promote the transfer of water droplets along a specific direction.24 Ultimately, the unidirectional moisture conduction behavior is maximized using a longer electrospraying time.
To observe the water transfer process, 10 μl of water was dropped on both sides of the fabric, and the change in the diffusion diameter of the water droplets over time was recorded, as shown in Fig. 5. When the water droplets fall on the hydrophobic side, the diameter becomes 0 mm within a certain period. However, the water droplets initially remain spherical, and at this time, the diffusion diameter is the diameter of the contact surface between the water droplets and the fabric surface. As the water droplets penetrate to the other side, they no longer contact the hydrophobic side, and the wetting diameter at this time is 0. Meanwhile, the diameter of the droplets on the hydrophilic side gradually increases from 0 mm to a fixed value. When the water droplets fall on the hydrophilic side, they diffuse rapidly; the diffusion diameter gradually increases and finally reaches the maximum value. However, owing to the hydrophobic force on the hydrophobic side, the water droplets cannot penetrate, and the diffusion diameter remains 0 mm on the hydrophobic side. These results confirm that when the water droplets contact the hydrophobic surface, they penetrate the fabric and remain on the hydrophilic surface. Therefore, in practical applications, the skin can be kept dry when the hydrophobic side is facing the skin.
Additionally, the directional moisture transport ability of the composite fabric was evaluated using a moisture management tester (MMT), in which water droplet landed on the hydrophobic side. The cumulative unidirectional transport index (R) is a key indicator for determining the directional water transport behavior of the material and can be calculated using the following formula, where T represents the test time, and Ut and Ub represent the moisture content at the top and bottom, respectively.
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The R values of the prepared composite fabric are shown in Fig. 6(a)–(c). Regardless of which coating material is used, the electrospraying time is directly correlated with the R value, indicating that the unidirectional water transport capacity of the composite fabric is enhanced with the increase in the spraying amount. This is because the difference in wettability and roughness on both sides of the fabric increases with the increase in spraying time. For the electrospraying time of 1 h, the cotton and hemp composite fabrics already show effective unidirectional transport capacity, whereas the R values of the modal composite fabrics are negative, indicating that water transport from the top to the bottom is not encouraged, and water diffusion occurs at the top. This can be attributed to the high hygroscopicity of the modal fabric, the small wettability gradient force, and the thrust generated by the hydrophobic layer is not sufficient to prevent the diffusion of water droplets on the upper surface. When the electrospraying time increases to 3 h, the R values of PVC-M and PVDF-M are 729.7% and 309.7%, respectively.
Fig. 6(d)–(i) shows the relative changes in the moisture content on the hydrophobic and hydrophilic sides of each composite fabric prepared using an electrostatic spraying time of 3 h. When water contacts the upper surface (the hydrophobic side), the moisture content on both sides increases and quickly reaches the maximum value. Finally, the moisture content of the lower surface becomes twice or more than that of the upper surface, indicating that water can be transferred from the upper surface to the lower surface because of a strong driving force. Moreover, the larger the gap between the moisture content curves on both sides of the fabric, the higher the unidirectional moisture conduction performance of the fabric. Notably, the gap between the moisture content curves of the modal composite fabric is smaller than that of other fabrics, so the unidirectional moisture conduction performance is relatively poor. This result is consistent with the R value comparison.
Based on the above results, we proposed a mechanism to explain the unidirectional water conduction phenomenon. As shown in Fig. 7(c), when a water droplet falls on the hydrophobic upper surface, it is subjected to two opposing forces in the vertical direction:25 hydrostatic pressure (FHP) and a hydrophobic force (FHF). FHP is proportional to the height of the water droplet from the material, providing the water droplet with the force to penetrate the hydrophobic layer. The calculation is expressed as follows: FHP = ρgh, where h represents the height of the water droplet from the fabric surface, g represents the acceleration of gravity, and ρ is the density of water. Conversely, FHF prevents water from penetrating. When the water droplet first contacts the upper surface, FHP is weak and the water droplet cannot pass through the hydrophobic layer. As the height of the water droplet increases with the accumulation of water, FHP increases accordingly. When FHP > FHF, the water passes through the hydrophobic layer and contacts the hydrophilic side. Then, because of the capillary force FCF, the water drop quickly penetrates and transfers to the hydrophilic side and diffuses, thus achieving continuous transmission of water droplets from the hydrophobic side to the hydrophilic side. However, when the water droplet falls on the hydrophilic side, the capillary force immediately causes the water droplet to diffuse in the horizontal direction. At this time, FHP also promotes water penetration, but when the water reaches the hydrophobic side, FHF prevents further penetration.
Footnote |
† Contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2025 |