Li Dong†
ab,
Min Shi†a,
Sijun Xu*a,
Qilong Suna,
Gangwei Pana,
Lirong Yao*a and
Chunhong Zhub
aSchool of Textile and Clothing, Nantong University, Nantong 226019, P. R. China. E-mail: xusijunwork@hotmail.com
bFaculty of Textile Science and Technology, Shinshu University, 3-15-1 Tokida, Ueda, Nagano 386-8567, Japan
First published on 12th June 2020
Poor ultraviolet (UV) resistance and good hydrophilicity lead to light aging of aramid fabrics and cause heat damage to the human body. This scenario occurs when the absorbed water by the fabric evaporates and forms high-temperature water vapor in a high-temperature fire environment, which may scald the human body. Herein, a superhydrophobic hollow TNT network structure was built on surfaces of aramid fibers by surface coating fluorinated TiO2 nanotubes (TNTs) to develop an air-permeable, UV-protective, and superhydrophobic coating. The as-prepared superhydrophobic aramid fabric exhibited highly superhydrophobic properties against various solutions of sauce, coffee, methylene blue, active red, Au nanoparticles, Ag nanoparticles, HCl, and NaOH with liquid contact angles up to 152–160°. In addition, the superhydrophobic fabric exhibited excellent UV aging resistance (UV protection factor was 100+; 74.58% of strength retention for 24 h of UV radiation compared with 55.15% of untreated fabric), a self-cleaning function against solid soil, and original wearing characteristics, including good breaking strength and air permeability. The developed superhydrophobic coating technology may promote practical application in high-temperature environments for aramid fabrics due to its good UV resistance, chemical resistance, poromericity, superhydrophobicity, anti-fouling, and self-cleaning properties.
Aramid fabrics are important wearable fire/thermal-protective materials due to their good flexibility, high temperature resistance, excellent chemical resistance, and inherent flame resistance.13,14 However, their light aging and hydrophilicity can cause functional decline and heat damage to wearers once liquid water absorbed by the fabric evaporates and forms high-temperature water vapor, which may diffuse into the garment and scald the skin.15,16 Researchers have mainly focused on the improvement of the uvioresistant performance of aramid fabric. For example, Patterson et al. reported a simple zinc oxide (ZnO) nanoparticle coating, which can improve the interfacial reinforcement and UV absorption of fiber-reinforced composites.17 Sun et al. developed UV uvioresistant aramid fibers by synthesizing titanium dioxide (TiO2) nanoparticles both on the aramid III fiber surface and in the interfacial space between the fibrils and microfibrils in supercritical carbon dioxide medium.18 For waterproofness, aramid fabrics are coated with an airtight waterproof coating but suffer from a significant increase in gram weight, reduction in flexibility, and poor thermal-wet comfort. Combined functions of ultraviolet (UV) resistance, waterproofness, and good air permeability are rarely reported for aramid fabric, although such features have been widely reported in natural fabrics such as cotton.19 By contrast, superhydrophobic coating technology offers fabrics with advanced multiple functions including poromericity, self-cleaning ability, and chemical resistance while maintaining their intrinsic advantages.20 The overall performance of a superhydrophobic coating is governed by its physicochemical structure including surface texture, binding forces, and surface chemistry.5 Given that an aramid fabric is usually exposed to high temperature, photoradiation, strong acid or base corrosion, and high oxidation conditions, its superhydrophobic coating should possess good UV, high-temperature, and chemical resistance.4,15 One of the most suitable methods is coating aramid fabrics with the superhydrophobic composite coating of TiO2 and organic hydrophobic materials. However, this method usually involves TiO2 nanoparticles to build a lotus leaf bionic concave–convex structure. Herein, we explore the possibility of the construction of a superhydrophobic bionic network structure by using TiO2 nanotubes (TNTs).
In summary, to endow aramid fabric with good properties of UV resistance, water repellency, and air permeability under an actual high-temperature scenario, superhydrophobic polyporous and hollow TNT networks on the surfaces of aramid fabric were built by impregnation with ethanol solution of TNTs and fluorinated siloxane, followed by water-triggered grafting and cross-linking reaction. The fluorinated TNT coating acted as reinforcement and wear-resistant phase displaying a uniform and porous network structure on the fiber surfaces. The superhydrophobic aramid fabric exhibited highly superhydrophobic properties against solutions of sauce, coffee, methylene blue, active red, Au nanoparticles, Ag nanoparticles, HCl, and NaOH with liquid contact angles up to 152–160° with no obvious negative influence on breaking strength and air permeability. In addition, the superhydrophobic fabric possessed improved UV resistance, UV aging resistance, and good self-cleaning function against solid soil.
TNTs were synthesized according to the revised method reported in the literature.21 The as-prepared TNTs before modification were found to have an average tube diameter of about 8–10 nm and tube length of about 500–1000 nm, suggesting a high length–diameter ratio (as shown in Fig. 2a). Note that TNTs after modification demonstrated obvious aggregation, which could be attributed to hydrophobicity of FTES-modified TNTs (FTES/TNTs; Fig. 2b). The grafting of FTES to TNTs was evidenced by FTIR (Fig. 1c). The two convoluted peaks at around 500 and 690 cm−1 represented two different vibration features of the Ti–O and Ti–O–Ti bonds in the TiO2 lattice.22 A broad absorption band at around 3400 cm−1 and a sharp band at around 1620 cm−1 in all FTIR spectra for TNTs were assigned to the physically adsorbed water molecules and hydroxyl groups on surfaces of TNTs.23 In the FTIR spectra of FTES, the peaks at around 890, 1113, 1143, and 1236 cm−1 were attributed to νC–F2 and νC–F3 bands, respectively.24 By grafting FTES to TNT surfaces, FTES/TNTs inherited the typical characteristic absorption peaks of FTES. The emerging weak bands at around 1113, 1143, 1191, and 1236 cm−1 could be assigned to the C–F adsorption bands of FTES. In addition, two peaks at 1056 and 1210 cm−1 attributed to Si–O–Si indicated that FTES was grafted to TNT surfaces.25,26
Fig. 2 TEM images of (a) TNTs and (b) FTES-modified TNTs and (c) FTIR spectra of TNTs, FTES–TNTs, and FTES. |
Superhydrophobic aramid fabric was prepared as described in Fig. 1. The coating of FTES/TNTs on aramid fabrics was evidenced by the FTIR spectra (Fig. 3). Aramid fabric exhibited typical strong absorption peaks of C–O stretching vibration at around 1640 cm−1, OC–N and N–H deformation couple vibration at 1540 and 1260 cm−1, and plane vibration of N–H at 720 cm−1.27 For the FTES/TNT-coated fabric, the emerged weak absorption peaks of FTES/TNTs of the νC–F2 and νC–F3 bands at 1113, 1143, and 1236 cm−1 and Si–O–Si peak at 1056 and 1210 cm−1 proved that FTES and TNTs were coated to the surface of aramid fabric.
The XPS survey spectra indicated that aramid fabric was composed of the elements carbon, nitrogen, and oxygen (Fig. 4a). For the TNT-coated aramid fabric, Ti LMMa, Ti 2s, Ti 3s, and Ti 3p appeared in the spectra, confirming the attachment of TNTs on the aramid fabric. By contrast, three additional strong XPS peaks of F KLL, F 1s, Si 2s, and Si 2p were detected on the FTES/TNT-coated aramid fabric, and these peaks could be assigned to the C–F and Si–O signals of FTES. Thus, aramid fabric was fully covered by FTES/TNTs. Fig. 4b–d show the fitting curves of the C 1s XPS spectra of aramid fabric, TNT-coated aramid fabric, and FTES/TNT-coated aramid fabric. The C 1s spectra of aramid fabric and TNT-coated fabric could be fitted to four independent XPS peaks of C–C, C–C/C–H, C–N, and OC–N–H bonds with binding energies at around 284.5, 284.7, 285.5, and 287.8 eV, respectively.28–30 For the C 1s spectra of FTES/TNT-coated aramid fabric, besides signals of aramid fabric and TNTs, two additional ultra-strong XPS peaks of the C–F bond for FTES with a binding energy at 291.7 (–CF2) and 293.1 eV (–CF3) were separated,31,32o thereby indicating the high content of FTES/TNTs on the surface of aramid fabric. The presence of FTES/TNTs on the surface of fabric was further confirmed by the study of the F 1s XPS signal in Fig. 5e, where the deconvolution of the fitted XPS peaks showed the molar contribution from C–F3 (688.2 eV) and C–F2 (689 eV).33,34 In the high-resolution Ti 2p spectra in Fig. 4f and g, the fitted XPS peaks of Ti 2p3/2 and Ti 2p1/2 were 458.5 and 464.2 eV, respectively, which were in line with the standard values of anatase TiO2, confirming the anatase crystalline nature of TNTs.
Fig. 5 presents FESEM micrographs of pristine, TNT-coated fabric, and FTES/TNT-coated aramid fabric. In the absence of the coating (Fig. 5a–c), the aramid fibers exhibited relatively smooth and clean surfaces with low roughness. By contrast, upon the introduction of a TNT coating, a large number of TNTs were coated to the surfaces of aramid fabric (Fig. 5d–f). However, such a TNT coating was coarse in the microscale and uneven in the nanoscale because of a lack of strong physicochemical binding force between TNTs and the fabric. For the FTES/TNT-coated aramid fabric, the surface became even and smooth in the microscale (Fig. 5g and h) due to the adhesive effect of FTES. In addition, TNTs were found to uniformly self-assemble to a dense porous network structure, thereby improving the surface roughness of the aramid fibers in the nanoscale (Fig. 5g–i). Given that the increase in surface roughness means less contact area for liquid water, this unique structure endowed the aramid fabric with excellent hydrophobicity.35
Water droplet images of the pristine fabric and FTES/TNT-coated aramid fabric are shown in Fig. 6a and b, respectively. When water (8 μL) was dropped onto the pristine fabric, no contact angle could be observed because the water drop completely spread and permeated into the fabric (Fig. 6a). However, when isopyknic water was placed onto the superhydrophobic fabric, a nearly sphere-like water droplet formed (Fig. 6b). Such a spherical droplet was stable and could stay supported on the fabric with the extended contact time. The water contact angle measurements revealed that the FTES/TNT-coated surface had a water contact angle of 165° and a rolling angle of 6°, indicating high superhydrophobicity. Apart from the water droplet, various aqueous solutions such as sauce, coffee, methylene blue solution, active red (AR) solution, nano Au solution, nano Ag solution, aqueous HCl (pH 1), and aqueous NaOH (pH 14) were dropped on the FTES/TNT-coated aramid fabric. As shown in Fig. 8, droplets of different solutions on the FTES/TNT-coated aramid fabric could still form a round ball, indicating the excellent super-hydrophobicity and stain resistance of the material.
We also tested and calculated the lag angles of aramid fabric. The water droplet permeated into untreated aramid fabric within 5 s, indicating hydrophilicity. By contrast, the water droplet remained quasi-sphere, with a contact angle over 160° for the FTES/TNT-coated aramid fabric. The advancing and receding contact angles were 3.18° and 0.86°. Therefore, the calculated lag angle of fabric for water was 2.32°, indicating its excellent water repellency. Fig. 7b presents the contact angle values calculated using the Wenzel equation, which considers the surface roughness and penetration of liquid into grooves. Compared with sauce and coffee, MB solution, AR solution, nano-Au solution, nano-Ag solution, aqueous HCl, and aqueous NaOH had higher contact angles of 159.5°, 157.4°, 159.4°, 155.1°, 155.9°, and 155.7°, respectively. All liquid contact angles were higher than 150°, suggesting the broad-spectrum lyophobicity property. In addition, the as-prepared superhydrophobic fabrics were impregnated in an acid and alkali solution for 24 h to evaluate resistance to corrosion for the superhydrophobic coating. The contact angles of both acid and alkali solution remained largely unchanged, indicating good resistance to acid and alkaline. We also evaluated the anti-wettability of the superhydrophobic coating by impregnation of aramid fabrics in MB solution for 6 h (Fig. 7c). In line with our predictions, the untreated aramid fabric was stained with blue color with 6 h of treatment. However, the TNT-coated fabric showed a dark blue color. The hydrophilic hollow TNT network may be responsible for the enhanced adsorption of MB because of the abundant hydroxyl groups and strong nanocapillary effect. By contrast, the FTES/TNT-coated aramid fabric retained its original faint yellow hue, suggesting good antifouling property.
To test the self-cleaning properties of the FTES/TNT-coated aramid fabric against solid matter, soil powder was scattered over the pristine and FTES/TNT-coated aramid fabrics. When untreated aramid fabric was scoured by water drops, the soil powder mostly permeated into the fabric and only a part was removed by water because of the hydrophilicity of aramid fiber. However, water droplets could completely wash off the soil on the FTES/TNT-coated aramid fabric when the fabric was slightly inclined (Fig. 8b), suggesting the fabric's good self-cleaning performance. This characteristic could be attributed to the low surface energy on the superhydrophobic surface. Solid pollutants could be electrostatically adsorbed or dissolved by water and then roll down with water droplets.
The mechanical properties of the aramid fabrics were investigated. A comparison of the tensile strength and elongation at break among the pristine, TNT-coated, and FTES/TNT-coated aramid fabrics is summarized in Table 1. The tensile strength and elongation at break of the TNT-coated and FTES/TNT-coated aramid fabrics remained roughly unchanged, indicating that the coating of TNTs had minimal effects on the mechanical properties. In addition, the air permeability of the FTES/TNT-coated aramid fabric showed a relatively larger decline from 122.63 mm s−1 to 69.04 mm s−1, mainly because TNTs and FETS blocked a part of the inter-yarn interspace. However, the declined permeability still meets the demand of comfort requirement. Finally, no distinguishable white index change was observed for the FTES/TNT-coated aramid fabric; this effect was also beneficial for practical applications.
Wearability | Pristine fabric | TNT-coated fabric | FTES/TNT-coated fabric |
---|---|---|---|
Tensile strength (N cm−1) | 361 (warp) | 368 (warp) | 381 (warp) |
417 (weft) | 450 (weft) | 365 (weft) | |
Elongation at break (%) | 25.88 (warp) | 29.90 (warp) | 27.64 (warp) |
17.14 (weft) | 17.64 (weft) | 15.39 (weft) | |
Air permeability (mm s−1) | 122.63 | 96.76 | 69.04 |
White index (WI) | 50.6 | 52.1 | 51.3 |
Aramid fabric is sensitive to UV light due to its highly reactive amide groups. A UV shielding coating is an effective method to retard UV photoaging. Given the strong UV absorption of TNTs, the as-prepared aramid fabric possessed good UV resistance (Fig. 9a). Compared with pure aramid fabric with UPF of around 50, the UPF of the TNT-coated superhydrophobic aramid fabrics increased up to 100+. Thus, the TNT coating blocked most of the UV radiation. In addition, the UV irradiation time-dependent strength retention tests of pristine and FTES/TNT-coated aramid fabrics indicated that the FTES/TNT-coated fabric exhibited enhanced UV light aging resistance. The strength retention of the FTES/TNT-coated aramid fabrics decreased from 77.47% (for 6 h of UV radiation) to 74.58%, 70.37%, and 68.87% (for 12, 24, and 33 h of UV radiation, respectively) compared with 63.11% (for 6 h of UV radiation) to 55.15%, 43.92%, and 40.99% (for 12, 24, and 33 h of UV radiation, respectively). The TNT-coated aramid fabric showed a similar strength retention cure to the FTES/TNT-coated fabrics, indicating that TNTs were responsible for the improved UV light resistance (Fig. 9b).
Fig. 9 (a) UV transmittance curves of pristine and FTES/TNT-coated aramid fabrics and (b) strength retention curve of pristine and FTES/TNT-coated aramid fabrics under different UV irradiation times. |
Footnote |
† Li Dong and Min Shi contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2020 |