{"id":181,"date":"2020-12-08T18:05:32","date_gmt":"2020-12-08T23:05:32","guid":{"rendered":"https:\/\/mae.ncsu.edu\/pmmf\/?page_id=181"},"modified":"2023-11-24T16:10:38","modified_gmt":"2023-11-24T21:10:38","slug":"droplet-surface-interaction","status":"publish","type":"page","link":"https:\/\/mae.ncsu.edu\/pmmf\/droplet-surface-interaction\/","title":{"rendered":"Droplet Mobility on Fibrous Surfaces"},"content":{"rendered":"<p>&nbsp;<\/p>\n<table style=\"border-collapse: collapse;width: 100%;height: 3627px\">\n<tbody>\n<tr style=\"height: 189px\">\n<td style=\"width: 100%;height: 189px\"><span style=\"font-size: 12pt\">Coating a surface with hydrophobic fibers can serve as a cost-effective alternative to micro-fabricating a hydrophobic roughened surface, a surface characterized by high apparent droplet contact angles. Fibrous coatings are usually made by depositing layers of randomly orientated fibers on top of one another, and while a droplet can exhibit a high apparent contact angle on such surfaces, its adhesion to the surface may still be quite strong and\/or unpredictable. The reasons behind droplet adhesion to a hydrophobic fibrous surface has not yet been fully understood or formulated. Our research in this area is aimed at quantifying the force of adhesion between a droplet and a hydrophobic surface. In particular with this research, we investigate the force required to detach a droplet from a hydrophobic fibrous surface both experimentally and computationally. Electrospun Polystyrene mats were considered for our study as they exhibit both high contact angles and poor droplet mobility.\u00a0<span style=\"font-family: inherit\">As the earth gravity is not strong enough to detach small droplets from such surfaces, aqueous ferrofluid droplets were used in a controllable magnetic field to enhance the effect of gravity. The detachment process was recorded via a high-speed camera and the images were used to detect the moment of detachment and to analyze droplet shape before and during detachment, as can be seen in the figure below and in Video 1.\u00a0<\/span><\/span><\/td>\n<\/tr>\n<tr style=\"height: 384px\">\n<td style=\"width: 100%;height: 384px\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-632\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-600x411.png\" alt=\"\" width=\"350\" height=\"240\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-600x411.png 600w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-1168x800.png 1168w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-768x526.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment.png 1329w\" sizes=\"auto, (max-width: 350px) 100vw, 350px\" \/><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-637\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-force-1-600x294.png\" alt=\"\" width=\"410\" height=\"201\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-force-1-600x294.png 600w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-force-1-768x376.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-force-1.png 1090w\" sizes=\"auto, (max-width: 410px) 100vw, 410px\" \/><\/p>\n<p><em><span style=\"font-size: 10pt\">Our experimental setup is shown in the figure on the left. Snapshots of the droplet detachment process are shown in the right figures. The net force (per unit mass) acting on the droplet is given under the images for each case in unit of g (gravitational acceleration). Both the Wenzel (wetting) and Cassie (non-wetting) droplets are shown [Jamali et. al., 2018a].<\/span><\/em><\/p>\n<p><a href=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-Detachment.mp4\"><span style=\"font-size: 10pt\">Video 1: Droplet Detachment from An Electrospun PS Surface &#8211; Wenzel Droplet<\/span><\/a><\/td>\n<\/tr>\n<tr style=\"height: 46px\">\n<td style=\"width: 100%;height: 46px\"><span style=\"font-size: 12pt\">A series of experiments similar to those shown above were also conducted for droplet moving over the surface of the electrospun PS coatings. Both the Wenzel and Cassie droplets were produced and used in the experiment as can be seen in figures below and Videos 2 and 3.<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-medium wp-image-646\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-detachment-force-600x137.png\" alt=\"\" width=\"600\" height=\"137\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-detachment-force-600x137.png 600w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-detachment-force-1200x274.png 1200w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-detachment-force-768x175.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-detachment-force-1536x351.png 1536w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-detachment-force.png 1966w\" sizes=\"auto, (max-width: 600px) 100vw, 600px\" \/><\/p>\n<p><em><span style=\"font-size: 10pt\">Example snapshots of droplet deformation and sliding are also shown for Wenzel and Cassie droplets with a volume of 4 \u03bcL. The force applied on the droplet is shown above each figure in unit of gravitational acceleration [Jamali et. al., 2018b].<\/span><\/em><\/p>\n<p><em><span style=\"font-size: 10pt\">\u00a0<\/span><\/em><span style=\"font-size: 10pt\"><a href=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Rolling-Cassie.avi\">Video 2: Droplet Mobility on An Electrospun PS Surface &#8211; Cassie Droplet<\/a>\u00a0 <\/span><\/p>\n<p><span style=\"font-size: 10pt\">\u00a0<\/span><span style=\"font-size: 10pt\"><a href=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Rolling-Wenzel.avi\">Video 3: Droplet Mobility on An Electrospun PS Surface &#8211; Wenzel Droplet<\/a><\/span><\/td>\n<\/tr>\n<tr style=\"height: 22px\">\n<td style=\"width: 100%;height: 22px\"><span style=\"font-size: 12pt\">Using a combination of numerical simulation (see the figure below) and experiment, we were able to produce an easy-to-use expression for the body force required to vertically detach a droplet from a electrospun PS surface, or make roll over the surface. The graph shown below compares predictions of our new equations to those obtained experimentally for droplet vertical detachment as a function of fiber-fiber spacing (inversely proportional to electrospinning time).\u00a0<\/span><\/td>\n<\/tr>\n<tr style=\"height: 295px\">\n<td style=\"width: 100%;height: 295px\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-650\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-Sim-545x600.png\" alt=\"\" width=\"318\" height=\"350\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-Sim-545x600.png 545w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-Sim-727x800.png 727w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-Sim-768x845.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Horizontal-Sim.png 1109w\" sizes=\"auto, (max-width: 318px) 100vw, 318px\" \/><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-642\" style=\"font-family: inherit;font-size: inherit\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-2-600x532.png\" alt=\"\" width=\"338\" height=\"300\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-2-600x532.png 600w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-2-902x800.png 902w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-2-768x681.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Vertical-detachment-2.png 1260w\" sizes=\"auto, (max-width: 338px) 100vw, 338px\" \/><br \/>\n<em><span style=\"font-size: 10pt\">Droplet profile and bottom views (droplet footprints) are given in the figures on the left for a droplet on a hydrophobic fibrous surface. The blue droplet is under gravity while the red droplet is pulled to the right. The YLCA for the droplet in the upper and lower rows are 100 and 85 degrees, respectively [Jamali et. al., 2018b]. The plot on the right is comparison between droplet detachment force in the vertical direction versus fiber-to-fiber spacing (inversely proportional to electrospinning time) obtained from our easy-to-use equation and experimental data [Jamali et. al., 2018a].<\/span><\/em><\/td>\n<\/tr>\n<tr style=\"height: 22px\">\n<td style=\"width: 100%;height: 22px\"><span style=\"font-size: 12pt\">We also conducted a similar computational-experiment study for droplets deposited on coated wire screens used for droplet separation (see the figures below and Video 4). The plot shown below compares droplet roll-off angle obtained from our simulations with those measured experimentally.\u00a0<\/span><\/td>\n<\/tr>\n<tr style=\"height: 480px\">\n<td style=\"width: 100%;height: 480px\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-660\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-Roll-off-ngle-1-552x600.png\" alt=\"\" width=\"368\" height=\"400\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-Roll-off-ngle-1-552x600.png 552w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-Roll-off-ngle-1-736x800.png 736w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-Roll-off-ngle-1-768x834.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-Roll-off-ngle-1.png 1205w\" sizes=\"auto, (max-width: 368px) 100vw, 368px\" \/><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-655\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-Mesh-270x600.png\" alt=\"\" width=\"180\" height=\"400\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-Mesh-270x600.png 270w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-Mesh-360x800.png 360w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-Mesh.png 615w\" sizes=\"auto, (max-width: 180px) 100vw, 180px\" \/><\/p>\n<p><span style=\"font-size: 10pt\"><em>Comparison is made between the roll-off angle obtained from our simulations with those measured experimentally for droplets with different volumes [Venkateshan and Tafreshi 2018].<\/em><\/span><\/p>\n<p><a href=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Double-Mesh.mov\"><span style=\"font-size: 10pt\">Video 4: Droplet Penetrates through the 1st Mesh but Not the 2nd Mesh<\/span><\/a><\/td>\n<\/tr>\n<tr style=\"height: 22px\">\n<td style=\"width: 100%;height: 22px\"><span style=\"font-size: 12pt\">We also studied to the force required to make a droplet penetrate into a thin electropun PS mat as can be seen in figure below and in Video 5. We also conducted numerical simulation for the same (see below).\u00a0<\/span><\/td>\n<\/tr>\n<tr style=\"height: 439px\">\n<td style=\"width: 100%;height: 439px\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-669\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-exp-532x600.png\" alt=\"\" width=\"320\" height=\"361\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-exp-532x600.png 532w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-exp-709x800.png 709w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-exp-768x866.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-exp.png 993w\" sizes=\"auto, (max-width: 320px) 100vw, 320px\" \/><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-673\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-sim-1-600x456.png\" alt=\"\" width=\"379\" height=\"288\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-sim-1-600x456.png 600w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-sim-1-1053x800.png 1053w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-sim-1-768x583.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Droplet-penetration-sim-1.png 1103w\" sizes=\"auto, (max-width: 379px) 100vw, 379px\" \/><\/p>\n<p><em><span style=\"font-size: 10pt\">The figure to the left shows snapshots taken from a droplet magnetically forced to penetrate into a thin PS electrospun mat. The plot shows the effects of fibers&#8217; orientation angle relative to one another on the force required to pull the droplet through the mat. The figure to the right shows examples of droplet profiles and footprints under the influence of gravity and at the moment of spontaneous penetration [Jamali et. al. 2019].\u00a0 <\/span><\/em><\/p>\n<p><em><span style=\"font-size: 10pt\">\u00a0<\/span><\/em><a href=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Penetration.mp4\"><span style=\"font-size: 10pt\">Video 5: Droplet Penetration into An Electrospun PS Mat<\/span><\/a><\/td>\n<\/tr>\n<tr style=\"height: 22px\">\n<td style=\"width: 100%;height: 22px\"><span style=\"font-size: 12pt\">We recently developed a new experimental method to measure the force required to detach a water (a polar liquid) droplet from a hydrophobic surface. This was done by partially cloaking the droplet with a high-surface-tension oil-based ferrofluid and using <\/span><span style=\"font-size: 12pt\">a magnet to apply a controllable body force to the resulting compound droplet (see figure below). This method is novel as the solid\u2212droplet contact area is not contaminated by the ferrofluid.<\/span><\/td>\n<\/tr>\n<tr style=\"height: 270px\">\n<td style=\"width: 100%;height: 270px\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-680\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS1-600x265.png\" alt=\"\" width=\"622\" height=\"275\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS1-600x265.png 600w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS1-1200x531.png 1200w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS1-768x340.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS1-1536x679.png 1536w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS1.png 1841w\" sizes=\"auto, (max-width: 622px) 100vw, 622px\" \/><br \/>\n<em><span style=\"font-size: 10pt\">The left figure shows the process of adding an oil-based ferrofluid to a pendent water droplet and detaching the <\/span><\/em><em><span style=\"font-size: 10pt\">resulting compound droplet from an electrospun PS surface. The figure on the right is an example of the force trajectories recorded by a sensitive scale during the detachment experiment [Jamali and Tafreshi 2020].<\/span><\/em><\/td>\n<\/tr>\n<tr style=\"height: 22px\">\n<td style=\"width: 100%;height: 22px\"><span style=\"font-size: 12pt\">Our study was accompanied by numerical simulations aimed at unveiling the interplay between the interfacial forces in a two-phase droplet (a complicated four-phase interfacial problem conssiting of water, oil, air, and solid) under the influence of a strong (detaching) body force. Our study showed that the detachment force measured via partial cloaking is independent of the volume of the ferrofluid used for the experiment.<\/span><\/td>\n<\/tr>\n<tr style=\"height: 352px\">\n<td style=\"width: 100%;height: 352px\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-682\" src=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS2-600x278.png\" alt=\"\" width=\"750\" height=\"347\" srcset=\"https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS2-600x278.png 600w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS2-1200x555.png 1200w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS2-768x355.png 768w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS2-1536x711.png 1536w, https:\/\/mae.ncsu.edu\/pmmf\/wp-content\/uploads\/sites\/24\/2020\/12\/Compound-PS2.png 1992w\" sizes=\"auto, (max-width: 750px) 100vw, 750px\" \/><br \/>\n<em><span style=\"font-size: 10pt\">Comparison between simulated detachment forces for pure and partially cloaked water droplets is given in the left figure for different <\/span><\/em><em><span style=\"font-size: 10pt\">water droplet volumes and YLCAs. The figure on the right shows water droplet pressure at the water\u2212solid interface vs water droplet volume. The inset figure shows pressure contours inside a water droplet with a volume of 7 \u03bcL and a YLCA of 110\u00b0 with and <\/span><\/em><em><span style=\"font-size: 10pt\">without a ferrofluid cloak [Jamali and Tafreshi 2020].<\/span><\/em><\/td>\n<\/tr>\n<tr style=\"height: 234px\">\n<td style=\"width: 100%;height: 234px\"><strong>Representative Publications:<\/strong><\/p>\n<ul style=\"list-style-type: square\">\n<li><span style=\"font-size: 10pt\">M. Jamali, A. Moghadam, H.V. Tafreshi, and B. Pourdeyhimi, Droplet Adhesion to Hydrophobic Fibrous Surfaces, <strong><em>Applied Surface Science<\/em><\/strong>, 456, 626 (2018a)<\/span><\/li>\n<li><span style=\"font-size: 10pt\">M. Jamali, H.V. Tafreshi, and B. Pourdeyhimi, Droplet Mobility on Hydrophobic Fibrous Coatings Comprised of Orthogonal Fibers, <strong><em>Langmuir<\/em><\/strong>, 34, 12488 (2018b)<\/span><\/li>\n<li><span style=\"font-size: 10pt\">D.G. Venkateshan and H.V. Tafreshi, Modelling Droplet Sliding Angle on Hydrophobic Wire Screens, <em><strong>Colloids and Surfaces A<\/strong><\/em> 538, 310 (2018)<\/span><\/li>\n<li><span style=\"font-size: 10pt\">M. Jamali, H.V. Tafreshi, and B. Pourdeyhimi, Formulating Droplet Penetration in Thin Hydrophobic Fibrous Materials, <em><strong>Journal of Applied Physics<\/strong><\/em> 125, 145304 (2019)<\/span><\/li>\n<li><span style=\"font-size: 10pt\">M. Jamali and H. V. Tafreshi, Measuring Force of Droplet Detachment from Hydrophobic Surfaces via Partial Cloaking with Ferrofluids, <strong><em>Langmuir<\/em> <\/strong>36, 22. 6116 (2020)<\/span><\/li>\n<\/ul>\n<p><span style=\"font-size: 10pt;color: #ff0000\"><a style=\"color: #ff0000\" href=\"https:\/\/mae.ncsu.edu\/pmmf\/publications\/\">Click here for a more complete list of publications<\/a><\/span><\/td>\n<\/tr>\n<tr style=\"height: 97px\">\n<td style=\"width: 100%;height: 97px\"><strong>Acknowledgement:<\/strong><\/p>\n<ul>\n<li><span style=\"font-size: 10pt\">The Nonwovens Institute.<\/span><\/li>\n<\/ul>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n","protected":false},"excerpt":{"rendered":"<p>&nbsp; Coating a surface with hydrophobic fibers can serve as a cost-effective alternative to micro-fabricating a hydrophobic roughened surface, a surface characterized by high apparent&#8230;<\/p>\n","protected":false},"author":394,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-181","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/mae.ncsu.edu\/pmmf\/wp-json\/wp\/v2\/pages\/181","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/mae.ncsu.edu\/pmmf\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/mae.ncsu.edu\/pmmf\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/mae.ncsu.edu\/pmmf\/wp-json\/wp\/v2\/users\/394"}],"replies":[{"embeddable":true,"href":"https:\/\/mae.ncsu.edu\/pmmf\/wp-json\/wp\/v2\/comments?post=181"}],"version-history":[{"count":10,"href":"https:\/\/mae.ncsu.edu\/pmmf\/wp-json\/wp\/v2\/pages\/181\/revisions"}],"predecessor-version":[{"id":1125,"href":"https:\/\/mae.ncsu.edu\/pmmf\/wp-json\/wp\/v2\/pages\/181\/revisions\/1125"}],"wp:attachment":[{"href":"https:\/\/mae.ncsu.edu\/pmmf\/wp-json\/wp\/v2\/media?parent=181"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}