2010
DOI: 10.2320/matertrans.m2010118
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Wetting Transition Characteristics on Microstructured Hydrophobic Surfaces

Abstract: Hydrophobicity and wetting transition behavior of water droplets were investigated on microstructured hydrophobic rough surfaces with pillar arrays, fabricated by self-replication with hydrophobic polydimethylsiloxane(PDMS) together with the use of CNC machine. The surfaces consist of microscale pillars(diameter: 105 mm, height: 150 mm) with varying spacing-to-diameter ratio (s=d) ranging from $1:0 to $3:3. A deionized(DI) water droplet of 4.3 ml was placed on hydrophobic surfaces and contact angles(CA) were m… Show more

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Cited by 38 publications
(28 citation statements)
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“…With this amount of liquid, θ * was found to not depend on the size of the droplet. Bigger droplets should however be avoided, because they alter the measurements of the surface tension , . This phenomenon is likely to result from the interaction of the droplet with the surface roughness.…”
Section: Methodsmentioning
confidence: 99%
“…With this amount of liquid, θ * was found to not depend on the size of the droplet. Bigger droplets should however be avoided, because they alter the measurements of the surface tension , . This phenomenon is likely to result from the interaction of the droplet with the surface roughness.…”
Section: Methodsmentioning
confidence: 99%
“…Stage 1 is the sub-process during which the bending depth of meniscus between four pillars changes from h x2 to h x1 , namely, the TPCL on pillars moves downwards from x=H-h x2 to x=H-h x1 (figures 1 A3 to A4). Stage 2 means the sub- Because the contact angle of the TPCL on posts keeps unchanged advancing contact angle during the two stages, R 1 and h x1 will also keep unchanging according to the equations (8) and (9). But the solid-liquid interface below the droplet increases continuously until the entire substrate below the drop is completely wetted.…”
Section: ) Qualitative Descriptionmentioning
confidence: 97%
“…At velocities greater than v min the pressure exerted by the impact in the shock envelope (Field, 1999) is enough to force liquid to fill and wet the inside of the gaps between the particles completely, forming a Wenzel state (Wenzel, 1936), as depicted in Figure 5(b). It is the transition between Cassie‐Baxter and Wenzel states that occurs at the rebound‐to‐pinning transition velocity (Lee et al ., 2010). In our system, as the diameter of the hydrophobic glass spheres increased, the depth of the gaps between features increased.…”
Section: Resultsmentioning
confidence: 99%