Ting-Yu 
            Xu
          
        
      a, 
      
        
          
            Chun-Chen 
            Hung
          
        
      a, 
      
        
          
            Chieh-Yun 
            Juan
          
        
      a, 
      
        
          
            Pei-Chieh 
            Tseng
          
        
      a and 
      
        
          
            Han-Yu 
            Hsueh
          
        
       *ab
*ab
      
aDepartment of Materials Science and Engineering, National Chung Hsing University, Taichung 40227, Taiwan, Republic of China. E-mail: hyhsueh@nchu.edu.tw;  Fax: +886-4-22857017;   Tel: +886-4-22840500 ext 506
      
bInnovation and Development Center of Sustainable Agriculture, National Chung Hsing University, Taichung 40227, Taiwan, Republic of China
    
First published on 16th September 2025
In this study, we present a novel fog-harvesting surface featuring buckled microstructures with alternating hydrophilic–hydrophobic regions, inspired by the elytra of desert beetles. The surface was fabricated by dispersing hydrophilic SiO2 particles on hydrophobic polytetrafluoroethylene (PTFE) buckled patterns. The hydrophilic protrusions promote droplet condensation and capture, whereas the hydrophobic buckled surfaces, functioning similarly to microchannels, facilitate directional transport to enhance water collection. Compared to flat surfaces, buckled structures can improve water collection efficiency by approximately 30%. This design with alternating wettability was systematically compared with fully hydrophilic and fully hydrophobic surfaces. Various parameters, including the fog flow distance, hydrophilic particle composition, surface wettability distribution, and buckle alignment, were investigated. Furthermore, the geometric funnel-shaped growth pattern of bird's nest fern leaves was incorporated to guide condensed droplets toward the collection zone, forming a dual-biomimetic mechanism that integrates microscale desert beetle-inspired structures with macroscale fern-inspired geometry. Real-world field tests—specifically, overnight fog collection experiments conducted in a forest environment—further confirmed the excellent performance of our device. Notably, the entire fabrication process can be conducted under ambient conditions; high-vacuum techniques and costly equipment are not required. The developed high-efficiency fog-harvesting device offers a scalable, sustainable, and inexpensive solution to atmospheric water collection, contributing to improved water accessibility in water-scarce regions.
The desert beetle was the first organism discovered to exhibit fog-harvesting behavior. To survive in extremely arid desert environments, it has evolved a unique elytral structure. When the ambient humidity increases, the beetle performs a specialized “fog-basking” behavior in which the body is tilted forward.29 Parker et al. reported that the elytra of the desert beetle possess granular protrusions and exhibit a surface pattern of alternating hydrophilic and hydrophobic regions.3 This unique surface architecture, combined with the beetle assuming a wind-facing posture, enables the beetle to intercept fog droplets and rapidly direct the collected water toward its mouth along hydrophobic pathways. Inspired by the desert beetle, a variety of fog-harvesting devices have been developed. Surfaces composed of hydrophilic and hydrophobic regions have been widely utilized to enhance fog collection. For example, Lai et al. wove superhydrophilic and superhydrophobic fibers into a patterned surface with alternating wettability, and discovered that optimizing the hydrophilic-to-hydrophobic ratio maximized fog-harvesting performance.4 Wang et al. sprayed polydimethylsiloxane (PDMS) aerogel onto a substrate to create a hydrophobic layer, and then deposited platinum through a mask to create an alternating hydrophilic–hydrophobic patterned surface. This design had higher fog harvesting efficiency than did purely superhydrophobic or superhydrophilic surfaces.5 In addition to surface wettability, surface roughness is a key factor influencing fog-harvesting capacity.7,30 Kim et al. fabricated devices with three-dimensional (3D) hydrophilic protrusions by using PDMS molding techniques and demonstrated that the fog harvesting efficiency resulting from 3D structures was considerably higher than that achieved using two-dimensional (2D) patterned designs.7
In general, surface roughness and the combination of hydrophilic with hydrophobic domains are both crucial to fog collection performance. However, some researchers have argued that surface roughness is the primary factor influencing fog collection, to the point where the effect of intrinsic wettability may be secondary or negligible. They claim that surfaces comprising hydrophobic granular protrusions can achieve high fog collection efficiency, even higher than those with alternating hydrophilic–hydrophobic patterns. For example, Guo et al. developed fog-harvesting surfaces by embossing hemispherical bumps onto copper sheets, and demonstrated that this granular-protrusion-based design outperformed a design featuring hydrophilic–hydrophobic protrusions.6 Although the desert-beetle-inspired water collection mechanism serves as a foundational model for fog-harvesting devices, certain aspects of the model remain under debate. In addition, researchers of this topic have employed differing experimental setups, measurement methods, and environmental conditions, rendering direct comparisons between studies difficult. Moreover, fog-harvesting devices are often fabricated using expensive equipment and high-vacuum processes such as chemical vapor deposition (CVD) and physical vapor deposition (PVD), which hinders large-scale production and industrial applicability. Therefore, elucidating the mechanisms underlying fog harvesting and developing inexpensive, high-performance and large-area devices remain major challenges in this field.
In this study, we present a novel fog-harvesting surface featuring a buckled microstructure with alternating hydrophilic and hydrophobic regions, inspired by the elytra of desert beetles. The surface was fabricated by dispersing hydrophilic particles on a hydrophobic buckled pattern. The hydrophilic protrusions promote droplet condensation and capture, whereas the hydrophobic buckled surfaces, which function as microchannels, facilitate directional transport to enhance water collection. We systematically compared the alternating wettability design with fully hydrophilic and fully hydrophobic designs. To ensure a meaningful comparison, fog-harvesting parameters such as the flow distance, velocity, and rate were selected in accordance with those reported in other studies. Furthermore, by incorporating the funnel-shaped geometry of bird's nest fern leaves, a dual-biomimetic design was achieved that synergistically enhances fog interception and large-scale directional water transport. Real-world field tests confirmed the excellent performance of our device. Importantly, the entire process of fabricating the device can be conducted under ambient conditions; high-vacuum techniques such as CVD or PVD are not required. To the best of our knowledge, this is the first study to integrate buckled microchannel structures with alternating wettability, together with a fern-inspired macroscopic geometry, to enable high-efficiency fog harvesting over a large area.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 50, 1
50, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 100, 1
100, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 200, 1
200, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 300, 1
300, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 400, and 1
400, and 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 500; the solid content was adjusted to 10, 20, and 30 wt%; and the SiO2 particle sizes employed were 1, 5, and 10 μm. The heat-shrinkable PS sheets were cleaned with ethanol and deionized water, followed by drying under a high-purity nitrogen stream. To further remove organic contaminants and render the surface slightly hydrophilic, the PS sheets were treated with UV ozone for 10 minutes prior to coating. The Tg of the PS sheet was approximately 110 °C, and the melting temperature (Tm) was around 230 °C. To relieve internal stress in the PS sheets and to induce shrinkage, the PS sheets coated with SiO2/PTFE dispersions were thermally treated in an oven at 140 °C for 10 minutes. The original size of each sample was 8 cm × 8 cm; after thermal treatment, the sample size shrank to approximately 3.2 cm × 3.2 cm due to the shrinkage effect. As a result, desert beetle-inspired surfaces with hierarchical micro-scale buckles and alternating hydrophilic SiO2 and hydrophobic PTFE regions were successfully fabricated.
500; the solid content was adjusted to 10, 20, and 30 wt%; and the SiO2 particle sizes employed were 1, 5, and 10 μm. The heat-shrinkable PS sheets were cleaned with ethanol and deionized water, followed by drying under a high-purity nitrogen stream. To further remove organic contaminants and render the surface slightly hydrophilic, the PS sheets were treated with UV ozone for 10 minutes prior to coating. The Tg of the PS sheet was approximately 110 °C, and the melting temperature (Tm) was around 230 °C. To relieve internal stress in the PS sheets and to induce shrinkage, the PS sheets coated with SiO2/PTFE dispersions were thermally treated in an oven at 140 °C for 10 minutes. The original size of each sample was 8 cm × 8 cm; after thermal treatment, the sample size shrank to approximately 3.2 cm × 3.2 cm due to the shrinkage effect. As a result, desert beetle-inspired surfaces with hierarchical micro-scale buckles and alternating hydrophilic SiO2 and hydrophobic PTFE regions were successfully fabricated.
      
      
        
        As mentioned, the elytra of the desert beetle have granular protrusions and a patterned surface with alternating hydrophilic–hydrophobic areas, giving the beetle the ability to harvest atmospheric water (Fig. 1a). Inspired by the body surface of desert beetles, we created a hierarchically buckled nanoporous PTFE film with superhydrophobic properties, randomly decorated the film with hydrophilic protruding SiO2 particles to enable fog harvesting. Fig. 1b presents field emission scanning electron microscope (FE-SEM) images of SiO2 particles, which constitute the hydrophilic areas of the desert beetle-inspired surfaces. To enable systematic comparison, SiO2 particles of various sizes were employed, including SiO2 particles with a diameter of 1 μm synthesized through the sol–gel method in our laboratory, as well as commercial SiO2 particles (5 μm and 10 μm in diameter). On the other hand, the bioinspired hydrophobic areas were created through aggregation of PTFE@TMN-10 micelles. To investigate the morphology of the micellized PTFE@TMN-10 colloids, samples were examined without staining using transmission electron microscopy (TEM), as depicted in Fig. 1c. Well-dispersed, dark, spherical objects of similar sizes (i.e., PTFE particles, marked with dashed white circles) surrounded by a gray medium (i.e., TMN-10 surfactant, marked with white arrows) were observed, indicating the formation of micellized PTFE@TMN-10 colloids. Compared with the TMN-10 surfactant, which comprises carbon, hydrogen, and oxygen, the micellized PTFE is composed of fluorine and carbon, resulting in the dark appearance of the microdomains in the TEM images due to mass-thickness contrast. PTFE particles with an average diameter of 200 nm were surrounded by a TMN-10 surfactant layer with an average thickness of 25 nm.
Fig. 1d displays FE-SEM images of micellized PTFE@TMN-10 and SiO2 particles closely packed and dispersed on thermally-shrinkable PS sheets before thermal treatment. The PTFE particles were clearly fully covered with TMN-10 surfactant, forming a smooth and dim composite layer (inset of Fig. 1d). Additionally, larger SiO2 particles were randomly dispersed among the micellized PTFE@TMN-10, specifically on the smooth surface. After thermal treatment was applied, which caused the TMN-10 to flow down onto the PS sheet, the PTFE surfaces were exposed, which imparted hydrophobic properties. Meanwhile, micro-level buckles (with a wavelength of ∼25 μm) formed spontaneously and were distributed across the PS sheets due to the sheet's thermal contraction (Fig. 1e). In contrast, due to the flow of TMN-10, the surface exhibited clear nanoporous buckled morphology (i.e., distinct aggregation of PTFE particles) rather than a dim morphology (see the inset of Fig. 1e). The resulting surface displayed hierarchical geometric characteristics: micro-level buckles were homogeneously covered with submicron-level wavelength buckles (∼2 μm), which comprised closely packed PTFE particles. These structures are interconnected in three dimensions, forming nanoporous buckled surfaces. Buckled structures, due to their large surface area and groove-like features, tend to have localized vortices that facilitate the adsorption and capture of surface materials.32,34 The surfaces composed of SiO2 and PTFE particles exhibited nanoporous structural features (pore size: around 50–150 nm), which helped trap air and enhanced the efficiency of water collection. Energy-dispersive X-ray spectroscopy (EDS) mapping images were obtained and are shown in Fig. 1f. Clearly, the multi-scale buckled regions comprising PTFE particles contained carbon and fluorine, while silicon and oxygen were clearly distributed on the larger particles' surfaces, indirectly confirming that they were silica particles. We thus concluded that hierarchical buckled surfaces with randomly distributed hydrophilic SiO2 and hydrophobic PTFE particles—BEETLES surfaces, resembling the surface of a desert beetle—had been successfully fabricated.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 50, 1
50, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 100, 1
100, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 200, 1
200, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 300, 1
300, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 400, and 1
400, and 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 500. Despite the varying mixing ratios, the samples had similar hierarchical buckled surfaces, as shown in Fig. 2a. Before the samples' fog-harvesting performance was tested, their surface wetting properties were assessed. In the measurement of water contact angle, hierarchical buckled surfaces composed solely of PTFE particles (without SiO2) were used for comparison, as shown in Fig. S1. Obviously, surfaces composed of higher hydrophilic particle ratios exhibited lower water contact angles and higher sliding angles, indicating increased hydrophilicity. Nevertheless, these surfaces had noticeable hydrophobic properties due to the predominant distribution of hydrophobic PTFE particles as the base material. Since fog-harvesting performance is determined by the synergistic interaction between hydrophilic and hydrophobic regions, both excessive and insufficient hydrophilic coverage can negatively affect the efficiency of water collection. Although a 1
500. Despite the varying mixing ratios, the samples had similar hierarchical buckled surfaces, as shown in Fig. 2a. Before the samples' fog-harvesting performance was tested, their surface wetting properties were assessed. In the measurement of water contact angle, hierarchical buckled surfaces composed solely of PTFE particles (without SiO2) were used for comparison, as shown in Fig. S1. Obviously, surfaces composed of higher hydrophilic particle ratios exhibited lower water contact angles and higher sliding angles, indicating increased hydrophilicity. Nevertheless, these surfaces had noticeable hydrophobic properties due to the predominant distribution of hydrophobic PTFE particles as the base material. Since fog-harvesting performance is determined by the synergistic interaction between hydrophilic and hydrophobic regions, both excessive and insufficient hydrophilic coverage can negatively affect the efficiency of water collection. Although a 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 50 ratio resulted in more hydrophilic characteristics, the samples with a hydrophilic-to-hydrophobic particle weight ratio of 1
50 ratio resulted in more hydrophilic characteristics, the samples with a hydrophilic-to-hydrophobic particle weight ratio of 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 300 achieved the highest fog harvesting efficiency (Fig. 2a, right bar chart). To further investigate the effects of upper film thickness on fog harvesting efficiency, a weight ratio of 1
300 achieved the highest fog harvesting efficiency (Fig. 2a, right bar chart). To further investigate the effects of upper film thickness on fog harvesting efficiency, a weight ratio of 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 300 for hydrophilic–hydrophobic particles was used in the subsequent experiments.
300 for hydrophilic–hydrophobic particles was used in the subsequent experiments.
        Particle solutions with solid content of 10, 20, and 30 wt% were prepared and used to fabricate fog-harvesting surfaces. Cross-sectional images of the prepared PS surfaces with different solid contents are shown in Fig. S2a. The upper film thickness clearly increased with higher dispersion concentration. The thickness was 374.0, 552.7, and 1002.0 nm for concentrations of increased from 10, 20, and 30 wt%, respectively. As shown in Fig. S2b, hydrophobicity was enhanced as the solid content was increased. Surfaces with good hydrophobicity can accelerate the transport of water droplets, thus increasing fog harvesting efficiency. However, when the dispersion concentration was 10 wt%, parts of the PS substrate surface remained smooth (Fig. 2b). In the enlarged FE-SEM images (see inset), we can observe that some areas of the surface were even exposed, revealing the underlying PS substrates. It indicated poor and incomplete coverage with PTFE particles due to the lower solid content, which was also reflected in the increased sliding angle. As expected, the surfaces created with the 20 and 30 wt% particle solutions exhibited hierarchical buckled patterns. However, an overly thick upper layer (e.g., for the surfaces created with the 30 wt% particle solution) caused aggregation of PTFE particles and peeling of these particles from the PS substrate, resulting in a fragmented surface morphology (indicated by a white arrow). These surface characteristics directly affected fog harvesting efficiency. As shown in Fig. 2b (right bar chart), the surfaces made with the 20 wt% particle solutions showed comparatively better fog-harvesting performance than did those made with the other two particle solutions.
Furthermore, SiO2 particles with diameters ranging from 1 μm to 10 μm were used to investigate their effect on fog-harvesting efficiency. As shown in Fig. S3a, the water contact angle was smaller when the SiO2 particles were larger, which was attributable to the larger hydrophilic surface area. By contrast, the sliding angle increased as the particle size was increased, likely due to the increased surface roughness. Nevertheless, the fog harvesting efficiency increased with particle size, with the 10 μm SiO2 particles demonstrating the highest efficiency as shown in Fig. 2c (right bar chart). Note that the average size of water droplets in fog is approximately 5–15 μm.35 As a result, the 1 μm SiO2 particles were too small to effectively intercept and adsorb water droplets, leading to significantly lower fog harvesting efficiency compared to samples with 5 μm and 10 μm particles. Conversely, particles larger than 15 μm tended to peel from the PTFE substrate because their larger volume prevented them from adequately embedding within aggregated PTFE particles, as shown in Fig. S3b. In summary, the ideal parameters selected in this study were 10-μm SiO2 particles mixed with PTFE particles, a weight ratio of 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 300, and solid content of 20%; this combination resulted in fog harvesting efficiency of 983.55 mg cm−2 h−1. To investigate the impacts of surface wettability and buckled structural characteristics on fog harvesting efficiency, flat and buckled surfaces covered with entirely hydrophilic particles (platinum, Pt), entirely hydrophobic particles (PTFE), and hydrophilic–hydrophobic particles (SiO2/PTFE) were prepared for fog-harvesting testing as shown in Fig. 2d. Regardless of the intrinsic surface wetting tendency of a surface, the fog harvesting efficiency was higher for buckled surfaces than for flat surfaces. This was attributable to the buckled surfaces providing a larger surface area, facilitating easier contact between the surface and fog. Also, as mentioned, the buckled surfaces formed channels that aided in the transport of water droplets, thereby enhancing the fog harvesting efficiency. Compared to flat surfaces, buckled structures can improve water collection efficiency by approximately 30%. Moreover, the surfaces coated with SiO2/PTFE exhibited better fog harvesting efficiency than did the surfaces coated with only Pt or PTFE particles, regardless of whether the surface was flat or buckled. Although the buckled surface composed entirely of PTFE particles was hydrophobic, exhibiting a water contact angle of 155.75° (Fig. S1a), it did not demonstrate effective fog-harvesting behavior, as it was unable to capture water droplets from the air. In contrast, while the hydrophilic Pt surface could readily condense water, it was ineffective in transporting the collected droplets away (a more detailed discussion is provided in Fig. 4). In addition, flat sheets composed of various materials, including copper, aluminum, silicon dioxide, titanium dioxide, PS, and Teflon, were prepared for fog-harvesting tests and were compared with the desert beetle-inspired buckled surfaces. Notably, our desert beetle-inspired buckled surfaces exhibited excellent fog-harvesting capability (Fig. 2e). This result demonstrates that the surfaces alternating hydrophilic–hydrophobic characteristics, similar to the elytra of desert beetles, had high fog-harvesting capability.
300, and solid content of 20%; this combination resulted in fog harvesting efficiency of 983.55 mg cm−2 h−1. To investigate the impacts of surface wettability and buckled structural characteristics on fog harvesting efficiency, flat and buckled surfaces covered with entirely hydrophilic particles (platinum, Pt), entirely hydrophobic particles (PTFE), and hydrophilic–hydrophobic particles (SiO2/PTFE) were prepared for fog-harvesting testing as shown in Fig. 2d. Regardless of the intrinsic surface wetting tendency of a surface, the fog harvesting efficiency was higher for buckled surfaces than for flat surfaces. This was attributable to the buckled surfaces providing a larger surface area, facilitating easier contact between the surface and fog. Also, as mentioned, the buckled surfaces formed channels that aided in the transport of water droplets, thereby enhancing the fog harvesting efficiency. Compared to flat surfaces, buckled structures can improve water collection efficiency by approximately 30%. Moreover, the surfaces coated with SiO2/PTFE exhibited better fog harvesting efficiency than did the surfaces coated with only Pt or PTFE particles, regardless of whether the surface was flat or buckled. Although the buckled surface composed entirely of PTFE particles was hydrophobic, exhibiting a water contact angle of 155.75° (Fig. S1a), it did not demonstrate effective fog-harvesting behavior, as it was unable to capture water droplets from the air. In contrast, while the hydrophilic Pt surface could readily condense water, it was ineffective in transporting the collected droplets away (a more detailed discussion is provided in Fig. 4). In addition, flat sheets composed of various materials, including copper, aluminum, silicon dioxide, titanium dioxide, PS, and Teflon, were prepared for fog-harvesting tests and were compared with the desert beetle-inspired buckled surfaces. Notably, our desert beetle-inspired buckled surfaces exhibited excellent fog-harvesting capability (Fig. 2e). This result demonstrates that the surfaces alternating hydrophilic–hydrophobic characteristics, similar to the elytra of desert beetles, had high fog-harvesting capability.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 300 and total solid content of 20 wt%. The generated BEETLES surfaces obtained using diatomaceous earth, CaCO3, and multibranched flower-like ZnO particles are shown in Fig. 3d–f, respectively. Overall, the hydrophilic particles were embedded in the buckled surface formed by the hydrophobic PTFE particles.
300 and total solid content of 20 wt%. The generated BEETLES surfaces obtained using diatomaceous earth, CaCO3, and multibranched flower-like ZnO particles are shown in Fig. 3d–f, respectively. Overall, the hydrophilic particles were embedded in the buckled surface formed by the hydrophobic PTFE particles.
        Fig. 3g demonstrates the fog harvesting efficiency of devices fabricated using SiO2 particles, diatomaceous earth, CaCO3, and multibranched flower-like ZnO particles. Although all of these hydrophilic additives resulted in remarkable water collection capabilities, the BEETLES surface incorporating artificial SiO2 particles exhibited the highest performance (983.55 mg cm−2 h−1). This superior efficiency was attributable to the particles' uniform shape, size, and distribution. The significant enhancement of water vapor capture by SiO2 particles is attributed to the Laplace effect and the particles' spherical structure. The Laplace pressure, caused by the curvature of a droplet's surface, generates a pressure difference between the interior and exterior of the droplet. This pressure difference influences the condensation process by affecting the stability and growth of newly formed droplets on the surface. As shown in Fig. 3h(I), water droplets of various sizes initially condensed on the surface of the SiO2 spheres. Smaller droplets, which have greater curvature, experience greater Laplace pressure, which destabilizes them and renders them more likely to evaporate. By contrast, larger droplets have smaller curvature, resulting in lower Laplace pressure, higher stability, and the promotion of further condensation. In other words, water vapor is driven by the pressure gradient, migrating from high-pressure regions (i.e., the surface of small droplets) to low-pressure regions (i.e., the surface of larger droplets), where it recondenses. This pressure-driven mass transfer leads to water being concentrated in low-curvature areas and facilitates stable droplet growth. From a macroscopic perspective, the smaller droplets gradually disappear as they feed the growth of the larger droplets on the SiO2 spheres—this is the classic Ostwald ripening process (Fig. 3h(II)). Subsequently, due to the curved geometry of the spheres, the growing droplets become spindle-shaped under the influence of gravity (Fig. 3h(III)). Once the gravitational force acting on the droplet exceeds the interfacial friction (i.e., when θ1 ≫ θ2), the droplet begins to slide off due to the geometric shape effect (the curved triangular region indicated by the red line in Fig. 3h(IV), resembling a slide-like structure). Finally, the sliding droplets are directed into the hydrophobic buckled channels formed by PTFE particles, which completes the water-harvesting process.
Compared with the SiO2 particles, which had spherical morphology and inherent hydrophilicity, the cubic CaCO3 and polygonal diatomaceous earth were associated with lower fog-harvesting performance. The fog harvesting efficiencies of devices fabricated using diatomaceous earth, CaCO3, and flower-like ZnO particles were 953.93, 928.72, and 894.54 mg cm−2 h−1, respectively. Nonetheless, the devices incorporating these alternative hydrophilic materials exhibited commendable water collection performance. Notably, both diatomaceous earth and CaCO3 derived from waste oyster shells have significant potential for future industrial applications, particularly those in alignment with environmental sustainability and circular economy principles. To further enhance fog harvesting efficiency, unidirectionally aligned buckled patterns were fabricated that could function similarly to microchannels. Unlike randomly distributed buckles formed via uncontrolled shrinkage, directional alignment during the thermal process of PS sheet shrinkage restricted the release of stress along one axis, resulting in uniformly oriented buckled patterns (see inset of Fig. 3i and S4). These aligned structures are expected to improve water droplet transport efficiency, thereby enhancing fog-harvesting performance. Fig. 3i presents a comparison of the fog harvesting efficiencies of devices with randomly oriented buckles and those with single-orientation buckles aligned either parallel or perpendicular to the direction of droplet movement. When the buckles were aligned with the direction of droplet flow, they acted as microchannels, generating capillary forces that facilitated linear transport and significantly improved fog harvesting efficiency (1069.02 mg cm−2 h−1). By contrast, when the buckles were perpendicular to the droplet movement, they acted as barriers to transport, resulting in a substantial decrease in fog harvesting efficiency (475.54 mg cm−2 h−1). The device with randomly oriented buckles exhibited performance that fell between those of these two configurations.
Obviously, the closer the fog-harvesting device was to the fog outlet, the higher was the fog collection efficiency (Fig. 4b). For the BEETLES surfaces, the harvesting efficiency at distances of 20 and 10 cm was respectively approximately 2.2 times and 5.9 times that for the non-front-facing configuration. The harvesting efficiencies at distances of 10 cm and 20 cm were 5770.77 and 2148.92 mg cm−2 h−1, respectively. The higher efficiency for the front-facing configurations was attributable to the higher droplet density and kinetic energy near the fog outlet, which promoted the collection of droplets. However, conditions such as high droplet concentration and high wind speeds (which are common in controlled laboratory settings) are rarely present during foggy weather. In other words, directly testing samples with their front side facing the fog flow for efficiency measurement does not reflect efficiency in real-world settings. A more accurate approach to measurement would be positioning samples farther from the fog outlet to capture naturally floating water droplets in the air. To observe water droplet condensation on device surfaces, a digital microscope was used to monitor the in situ fog collection process on the BEETLES, hydrophobic buckled, and hydrophilic buckled surfaces, as shown in Fig. 4c. The optical images of water droplets on the surfaces were adjusted to enhance their contrast and brightness, making the condensed droplets could be more easily distinguished (Fig. S7). All surfaces began to capture water droplets within 30 seconds, and over time, all three surfaces accumulated a high number of droplets. On the hydrophilic buckled surfaces, water droplets condensed easily due to their intrinsic hydrophilicity. However, the condensed droplets tended to adhere to the surface rather than slide off. By contrast, on the hydrophobic buckled surfaces, while droplets detached immediately after condensing, but the intrinsic hydrophobicity rendered it less effective at attracting water vapor for condensation, resulting in a lower condensation rate and the formation of smaller droplets. As a result, the hydrophilic and hydrophobic buckled surfaces both exhibited relatively low fog collection efficiency. The fog harvesting efficiency for capturing naturally floating water droplets in the air was 634.67 mg cm−2 h−1 for the hydrophilic buckled surface and 663.52 mg cm−2 h−1 for the hydrophobic buckled surface (Fig. 4b). By contrast, the BEETLES surface demonstrated excellent fog collection efficiency; it induced water droplet condensation through hydrophilic SiO2 zones, and the large-area hydrophobic PTFE buckles promoted the coalescence and rapid detachment of droplets. The BEETLES surface's efficiency in capturing water droplets in the air was 983.55 mg cm−2 h−1. The detachment of water droplets from the surface was clearly observed (Fig. S8). Moreover, to evaluate experimental reliability, we added the results of a 10-day fog-harvesting cycling test on the BEETLES surface. In this experiment, the device was placed for 10 consecutive days, and one fog-harvesting test was performed each day, simulating the natural frequency of fog occurrence. The average fog-harvesting efficiency of the BEETLES surface showed no significant variation throughout the 10-day period (Fig. S9), confirming the reproducibility and durability of the device.
To evaluate fog-harvesting performance under natural conditions, the two fog-harvesting devices were placed overnight in Huisun Forest (Nantou, Taiwan), as shown in Fig. 5d. The device on the left consisted of PS sheets coated with only PTFE micelles (control group), while the device on the right featured BEETLES surfaces. Due to the presence of SiO2 particles, the BEETLES surfaces exhibited a light green appearance. Fig. 5d shows a time-lapse sequence, with images captured at 0, 4, 8, 9, and 11 hours. The entire fog collection process is also presented in Movie S1. Initially, the density of fog in the forest was low, and limited water was observed in the collection bottles. Nevertheless, fog formation became noticeable after approximately 4 hours, and water visibly accumulated in both bottles. The blurriness of the 8-hour photograph was caused by dense fog enveloping the setup. After 11 hours, the BEETLES-based device (right) had collected substantially more water than the control device had (left). Following overnight exposure (approximately 12 hours), the bioinspired BEETLES surfaces shaped like bird's nest fern leaves had harvested approximately 125 grams of water from the ambient air, roughly twice the amount collected by the control sample (see enlarged inset of Fig. 5d after 11 hours). Although fog-harvesting performance is inherently influenced by environmental factors such as temperature, humidity, and wind speed, the BEETLES surfaces were clearly demonstrated superior efficiency under real-world conditions.
Beyond SiO2, we also demonstrated the use of alternative hydrophilic fillers such as CaCO3 derived from waste oyster shells, diatomaceous earth, and ZnO, thereby highlighting the material versatility and sustainability of this approach. Furthermore, this study introduced a dual-biomimetic design, in which the desert beetle-inspired micro/nanostructure was integrated with the bird's nest fern-inspired macroscopic geometry, significantly enhancing fog collection efficiency across multiple length scales. Scholars have continued to debate the relative importance of surface chemistry (i.e., hydrophilic–hydrophobic properties) versus physical structure (micro- and nanoscale topographies) in the design of fog-harvesting surfaces, as discussed in the introduction. Moreover, a standardized methodology for measuring fog collection efficiency is still lacking across research groups, making it difficult to perform direct comparisons between different fog-harvesting surfaces. Nevertheless, we attempted to organize and compare a variety of reported biomimetic fog-harvesting surfaces. As shown in Table 1, taking into account differences in fog flow distance, velocity, and flow rate, we can conclude that our BEETLES device exhibits outstanding water collection performance. Its low-cost, scalable fabrication, integration of dual biomimetic strategies, material sustainability, and comprehensive validation imbue it with significant industrial competitiveness, indicating high potential for wide-scale applications. In future work, we aim to engineer gradient buckled structures in the hydrophobic regions, where the buckles will function as microchannels with gradually increasing wavelengths. In addition, our future work will focus on integrating macroscopic, nature-inspired structural designs—such as cactus-like geometries—with the BEETLES framework to further enhance the performance of composite fog-harvesting devices.
| Substrate | Method | Bio-inspired mechanism | Fog flow distance (cm) | Fog flow velocity (m s−1) | Fog flow rate (L h−1) | Fog harvesting efficiency (mg cm−2 h−1) | Publication year | Ref. | 
|---|---|---|---|---|---|---|---|---|
| Copper wire | Surface modification | Cactus/spider silks/Nepenthes/blueberry | 10–20 | 1.39–2.37 | N/A | 30 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 162 | 2024 | 38 | 
| Aluminum sheet | 3D printing | Cactus/spider silk/camphor leaves/desert beetles/lizards | 15 | 1.83–2.24 | N/A | 27 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 720 | 2025 | 39 | 
| Copper sheet | Laser printing | Desert beetle/nephrolepis cordifolia | 10 | 2 | N/A | 19 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 200 | 2024 | 26 | 
| PS sheet | Spin coating | Namib desert beetle | 10 | 1.2 | 2.2 | 5770.77 | This work | |
| PS sheet | Spin coating | Namib desert beetle | 20 | 1.2 | 2.2 | 2148.92 | This work | |
| PP plate | Surface modification | N/A | 10 | 1 | 0.23 | 2130 | 2024 | 40 | 
| APTES/PDMS | Grafting | Porcupinefish | 10 | 0.2 | N/A | 1700 | 2023 | 41 | 
| Zinc sheet | Surface modification/grafting | N/A | 15 | 0.25 | N/A | 1442 | 2023 | 30 | 
| A SHB/SHL fabric | Textile weaving | Namib desert beetle | 20 | N/A | 0.3 | 1432.7 | 2021 | 4 | 
| PS sheet | Spin coating | Namib desert beetle | 20 (non-directly) | 1.2 | 2.2 | 983.55 | This work | |
| Stainless steel sheet | Laser structuring/surface oxidation | Cactus spine/leaf vein/desert beetles | 20 | N/A | 1.5 | 560 | 2024 | 42 | 
| PET film | Surface oxidation | Leaf vein | 10 | 0.5 | 0.35 | 467.3 | 2018 | 43 | 
| Copper sheet | Surface modification | Namib desert beetle | 12 | 0.5 | N/A | 430 | 2018 | 6 | 
All data are included in the manuscript and/or the SI. Supplementary information: water contact and sliding angles of buckled surfaces fabricated with SiO2/PTFE at different weight ratios, and all-PTFE surfaces (Fig. S1); cross-sectional FE-SEM images and water contact angles of buckled surfaces fabricated with mixed particle solutions at different concentrations (Fig. S2); water contact angles of buckled SiO2/PTFE surfaces with various SiO2 particle sizes, and FE-SEM image of buckled structures formed by PTFE after SiO2 particle detachment (Fig. S3); schematic of unidirectional buckled pattern formation via thermal shrinkage, and FE-SEM images of aligned PTFE patterns with embedded SiO2 particles (Fig. S4); photograph of the fog-harvesting setup, including an ultrasonic humidifier, acrylic chamber, and samples mounted on an aluminum tray for water collection (Fig. S5). FE-SEM images of buckled PTFE particle and platinum surfaces, and water contact angles of BEETLES, buckled PTFE particle, and platinum surfaces (Fig. S6); digital microscope images of the BEETLES surface before and after contrast/brightness adjustment to enhance droplet visibility (Fig. S7); handheld digital microscope image of the BEETLES surface during the roll-off process of water droplets (Fig. S8); fog-harvesting efficiency of the BEETLES surface throughout the 10-day period (Fig. S9). FE-SEM images of BEETLES surfaces fabricated by spin-coating, brush-coating, and spray-coating methods, and cross-sectional FE-SEM images of micellized PTFE/TMN-10 and SiO2 thin layers (Fig. S10). See DOI: https://doi.org/10.1039/d5ta05905d.
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