2017
DOI: 10.1088/1742-6596/788/1/012003
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The surface tension effect on viscous liquid spreading along a superhydrophobic surface

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Cited by 3 publications
(3 citation statements)
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“…For long rod-shaped E. coli of about 2 μm in length, it is more difficult for flagella to be perpendicular to the interface and generate attractive radial fluid flow that leads to cluster formation, 43−47 giving rise to a more significant improvement which can resist the adhesion of 88% E. coli. For the lasertextured superhydrophobic surface under the stationary state, the driving force of the bacterial cluster cannot break through the air−liquid interface because of the surface tension 48 created by the trapped air layer on the superhydrophobic surface, which lead to hardly any bacterial adhesion is achieved as shown in Figure 7b. While under the oscillation state, the oscillating motion gives the opportunity for exposing the surface area and making bacteria to contact and colonize.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
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“…For long rod-shaped E. coli of about 2 μm in length, it is more difficult for flagella to be perpendicular to the interface and generate attractive radial fluid flow that leads to cluster formation, 43−47 giving rise to a more significant improvement which can resist the adhesion of 88% E. coli. For the lasertextured superhydrophobic surface under the stationary state, the driving force of the bacterial cluster cannot break through the air−liquid interface because of the surface tension 48 created by the trapped air layer on the superhydrophobic surface, which lead to hardly any bacterial adhesion is achieved as shown in Figure 7b. While under the oscillation state, the oscillating motion gives the opportunity for exposing the surface area and making bacteria to contact and colonize.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…coli. For the laser-textured superhydrophobic surface under the stationary state, the driving force of the bacterial cluster cannot break through the air–liquid interface because of the surface tension created by the trapped air layer on the superhydrophobic surface, which lead to hardly any bacterial adhesion is achieved as shown in Figure b. While under the oscillation state, the oscillating motion gives the opportunity for exposing the surface area and making bacteria to contact and colonize.…”
Section: Resultsmentioning
confidence: 99%
“…Example 16. From expressions (47) and (48) it follows that the Guderley equation 17has two solutions of the same type u 1 = ϕy 3/2 +ψ and u 2 = ϕy 3 +ψ, which differ from each other by the exponent y. This circumstance suggests an attempt to construct a more general solution of equation (17), that includes both terms with different exponents at once.…”
Section: Construction Of Compound Solutions (Nonlinear Superposition mentioning
confidence: 99%