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518. Lekan, S.F., “Corona treatment as an adhesion promoter for UV/EB curable coatings,” in RadTech 88 Proceedings, RadTech, 1988.

1802. Lelah, M.D., T.G. Grasel, J.A. Pierce, and S.L. Cooper, “The measurement of contact angles on circular tubing surfaces using the captive bubble technique,” J. Biomedical Materials Research, 19, 1011-1015, (1985).

Circular tubings are used extensively in biomedical implants and devices. It is desirable to determine contact angles on the inner or outer surfaces of such tubing in its final fabricated form. In this study, a technique for the measurement of contact angles on tubing surfaces in an aqueous environment is reported. This has particular applications to biomaterials research, where polymer tubings contact the biologic environment. In this technique, air or octane captive bubble dimensions can be measured, and an underwater contact angle calculated from these dimensions. The validity of the technique was experimentally confirmed using Solution Grade Biomer and NIH standard polyethylene surfaces.

709. Leonard, D., P. Bertrand, A. Scheuer, R. Prat, and J.P. Deville, “TOF-SIMS and in situ study of O2-N2 afterglow discharge plasma-modified PMMA, PE and hexatriacontane surfaces,” Presented at First International Congress on Adhesion Science and Technology, Oct 1995.

1872. Leonard, D., P. Bertrand, A. Scheuer, et al, “Time-of-flight SIMS and in-situ XPS study of O2 and O2-N2 post-discharge microwave plasma-modified high-density polyethylene and hexatriacontane surfaces,” J. Adhesion Science and Technology, 10, 1165-1197, (1996).

The O2 and O2-N2 ([N2] < 15%) post-discharge microwave plasma modifications of high-density polyethylene (HDPE) and hexatriacontane (HTC) surfaces have been studied as a function of the distance from the discharge and the gas composition. They are compared in terms of the in-situ XPS O/C ratios and C 1s components, and the ex-situ ToF-SIMS O-/CH- ratios and relative intensities of series of peaks. The results on the effect of the distance from the discharge showed a clear correlation between the in-situ XPS results and the O2 post-discharge modeling, exhibiting the double role of oxygen atoms: functionalization initialization by creating radicals (which react with molecular oxygen) and degradation due to the energy released by the oxygen atom recombination process. Specific in-situ XPS and ex-situ ToF-SIMS signatures of this in-situ degradation related to the oxygen atom recombination process were exhibited. When N2 was introduced in the plasma gas, the in-situ XPS results and the ex-situ ToF-SIMS results were very different. The in-situ functionalization decreased as a function of the N2 addition and the ex-situ functionalization exhibited a high maximum for the 5% N2-95% O2 post-discharge plasma and then decreased. Despite the absence of a complete O2-N2 post-discharge modeling, it can be assumed that there is also a maximum of the oxygen atom content for the 5% N2-95% O2 post-discharge. Thanks to the in-situ XPS and ex-situ ToF-SIMS specific signatures, it was also shown that this maximum corresponds to a low in-situ degradation effect. Nitrogen introduction could influence the role of oxygen atoms in such a way that there is a decrease in oxygen atom recombination processes (thus in degradation) for small N2 addition and even a decrease in oxygen functionalization initialization for further N2 incorporation in the plasma gas. No nitrogen was observed in the in-situ XPS results, whereas some ex-situ ToF-SIMS nitrogen-containing ions were observed for the O2 and O2-N2 post-discharge. However, their relative intensities followed the variation in oxidation and not the variation in N2 concentration in the plasma gas. They could be related to a post-treatment functionalization effect. Differences observed between HDPE and HTC are explained in terms of their structural differences (desorption of low molecular weight oxygen-containing fragments for HTC).

1376. Leroux, F., A. Perwuelz, C. Campagne, and N. Behary, “Atmospheric air-plasma treatments of polyester textile structures,” J. Adhesion Science and Technology, 20, 939-957, (2006).

The effects of atmospheric air-plasma treatments on woven and non-woven polyester (PET) textile structures were studied by surface analysis methods: wettability and capillarity methods, as well as atomic force microscopy/lateral force microscopy (AFM/LFM). The water contact angle on plasma-treated PET decreased from 80° to 50–40°, indicating an increase in the surface energy of PET fibres due to a change in the fiber surface chemical nature, which was confirmed by a higher fiber friction force measured by the LFM. The extent of water contact angle decrease, as well as the wash fastness of the treatment varied with the structure of the textile. Indeed the more porous the textile structure is (such as a non-woven), the fewer are the chain scissions of the PET at the fiber surface, during the plasma treatment. Thus, the level of surface oxidation and the weak boundary layers formation depend not only on plasma treatment parameters but also on the textile structure.

1890. Leroux, F., C. Compagne, A. Perwuelz, and L. Gengembre, “Polypropylene film chemical and physical modifications by dielectric barrier discharge plasma treatment at atmospheric pressure,” J. Colloid and Interface Science, 328, 412-420, (Dec 2008).

Dielectric barrier discharge (DBD) technologies have been used to treat a polypropylene film. Various parameters such as treatment speed or electrical power were changed in order to determine the treatment power impact at the polypropylene surface. Indeed, all the treatments were performed using ambient air as gas to oxidize the polypropylene surface. This oxidation level and the surface modifications during the ageing were studied by a wetting method and by X-ray photoelectron spectroscopy (XPS). Moreover polypropylene film surface topography was analyzed by atomic force microscopy (AFM) in order to observe the surface roughness modifications. These topographic modifications were correlated to the surface oxidation by measuring with a lateral force microscope (LFM) the surface heterogeneity. The low ageing effects and the surface reorganization are discussed.

2045. Levine, M., G. Ilkka, and P. Weiss, “Relation of the critical surface tension of polymers to adhesion,” J. Polymer Science Part B: Polymer Letters, 2, 915-919, (1964).

2236. Lewin, M., A. Mey-Marom, and R. Frank, “Surface free energies of polymeric materials, additives and minerals,” Polymers for Advanced Technologies, 16, 429-441, (2005).

This paper presents a review of the ST and SFE values expressed in dyn/cm for a number of polymers, minerals, oxides and clays. The review also deals with the calculation of ST based on parachor values and other polymer properties obtained from a DIPPR database accompanied and coupled with QSPR software entitled TSAR. Data are also given on the ST of clays. The three components of the ST, the apolar Lifshitz–van der Waals component and the two polar (electron-donor and electron-acceptor) components of the various clays are also presented, as calculated by the van Oss et al. equation. Substitution of the cations in the innerlayer of clays by other inorganic cations is reviewed. Data are given on the effect of introducing organic ammonium cations into the clays and how they affect MMT, laponite, and talc. The effect of temperature on the ST of small molecules and on polymers is discussed, and a formula for this effect is shown. The effect of surface crystallinity on ST is discussed. The effect of chemical composition, structure and molecular weight are discussed as well. Systems for the estimation of ITs are reviewed, in relation to the ST values of the components. Data on the ST of high-energy materials are presented. The changes in these values upon interaction with low-energy surfaces are discussed. Copyright © 2005 John Wiley & Sons, Ltd.

1303. Li, D., C. Ng, and A.W. Neumann, “Contact angles of binary liquids and their interpretation,” J. Adhesion Science and Technology, 6, 601-610, (1992).

Contact angles of binary liquid mixtures on Teflon FEP were measured. It was found that the equation of state for interfacial tensions, γSL = f (γLV, γsv), cannot be used to determine solid surface tensions from these contact angles of binary liquid mixtures. These findings are explained in terms of the thermodynamic phase rule.

221. Li, D., E. Moy, and A.W. Neumann, “The equation of state approach for interfacial tensions: comments to Johnson and Dettre,” Langmuir, 6, 885-888, (1989).

1594. Li, D., P. Cheng, and A.W. Neumann, “Contact angle measurement by axisymmetric drop shape analysis (ADSA),” Advances in Colloid and Interface Science, 39, 347+, (1992).

718. Li, D., and A.W. Neumann, “Thermodynamic status of contact angles,” in Applied Surface Thermodynamics, Neumann, A.W., and J.K. Spelt, eds., 109-168, Marcel Dekker, Jun 1996.

725. Li, D., and A.W. Neumann, “Wettability and surface tension of particles,” in Applied Surface Thermodynamics, Neumann, A.W., and J.K. Spelt, eds., 509-556, Marcel Dekker, Jun 1996.

The interfacial energetics and wettability of small particles are of technological interest in many areas of applied science. Areas where such phenomena are important include the preparation of stable suspensions of particles (e.g., colour pigments in paints), the adhesion of particles to solid surfaces in various scenarios (e.g., lubrication), the dispersion of particles into a liquid or melt of a polymer, and the modification of particle surface properties through the adsorption of polymeric macromolecules or surfactants. The successful manipulation of the process being considered is largely determined by the physicochemical surface properties of the interacting surface components, and particularly the wettability and the surface (or interfacial) tension of the particles. The complexities of contact angle phenomena and surface tensions were discussed in Chapter 3.

1296. Li, D., and A.W. Neumann, “A reformulation of the equation of state for interfacial tensions,” J. Colloid and Interface Science, 137, 304-307, (1990).

1298. Li, D., and A.W. Neumann, “Thermodynamics of contact angle phenomena in the presence of a thin liquid film,” Advances in Colloid and Interface Science, 36, 125-151, (1991).

The effects of a thin liquid film on contact angles are studied using a simplified thermodynamic model. (in this model, the small transition zone between the liquid-vapour interface and the fiat thin liquid film is neglected). A set of mechanical equilibrium conditions have been derived for contact angle systems with a flat thin liquid film. The equilibrium condition at the three-phase intersection explicitly predicts the effects of the film tension, the disjoining pressure and the film thickness, on contact angles.

The number of degrees of freedom for a two-component solid-liquid-vapour surface system with a flat thin liquid film is shown to be three, implying the existence of an equation-of-state-type relationship among the solid-liquid interfacial tension, γsl, liquid surface tension, γlv, the disjoining pressure, Π, and the film tension, γf. An approximate, explicit form of such an equation of state has been derived. The combination of this equation of state with the equilibrium condition of the the three-phase intersection can be used to estimate the film tension, γf, and the solid-liquid interfacial tension, γsl, from the measured data for the vapour pressure, Pv, the film thickness, h, the curvature of the liquid-vapour meniscus, J, the liquid surface tension, γlv, and the contact angle, θ.

The effect of the thin film on the drop-size dependence of contact angles is also investigated and found to be negligible.

1299. Li, D., and A.W. Neumann, “Equation of state for interfacial tensions of solid-liquid systems,” Advances in Colloid and Interface Science, 39, 299-345, (1992).

1301. Li, D., and A.W. Neumann, “Contact angles on hydrophobic solid surfaces and their interpretation,” J. Colloid and Interface Science, 148, 190-200, (1992).

Contact angles of 17 liquids on 3 hydrophobic solid surfaces, FC721, fluorinated ethylene propylene, and polyethylene terephthalate, were measured by using the Axisymmetric Drop Shape Analysis-Profile (ADSA-P) technique. Details of the surface preparation and the experiments are presented. The accuracy of these contact angle data is better than 0.2° in most cases. These data were used to calibrate an equation of state for interfacial tensions of solid—liquid systems. The end results of the analysis is an equation of state for interfacial tensions with a single parameter β = 0.0001247 (m2/mJ)2, cf., Eqs. [22]–[24]. Within the experimental limitations, there is no evidence for the notion that β might change from system to system.

1302. Li, D., and A.W. Neumann, “Surface heterogeneity and contact angle hysteresis,” Colloid and Polymer Science, 270, 495-504, (1992).

The effect of surface heterogeneity on contact angle hysteresis is studied by using the model of Neumann and Good of a vertical plate with horizontal heterogeneous strips. The results of this study explain well known, but not understood patterns of contact angle behaviour: On the one hand, the advancing contact angle on a carefully prepared solid surface is generally reproducible; on the other hand, even a very small amount of surface heterogeneity may cause the receding contact angle to be less reproducible and to depend on several non-thermodynamic factors.

1308. Li, D., and A.W. Neumann, “Wetting,” in Characterization of Organic Thin Films, Ulman, A., ed., 165-192, Manning Publications, 1995.

1327. Li, D., and A.W. Neumann, “Determination of line tension from the drop size dependence of contact angles,” Colloids and Surfaces, 43, 195-206, (1990).

The drop size dependence of the advancing contact angle of dodecane and ethylene glycol on carefully prepared FC-721, Zonyl FSC and DDOA surfaces has been studied by means of axisymmetric drop shape analysis. The contact angles were measured in air and were found to decrease by 3 to 5 degrees as the radius of the three-phase contact line increased from approximately 1 to 5 mm. This phenomenon is interpreted in terms of line tension by the modified Young equation. Our experimental results show that the line tensions are positive and of the order of 1 μJ m−1 for all the three solid-liquid systems in our study; these results are consistent with previous work in our laboratory. The occasionally observed phenomenon that contact angles increase as the radius of the three-phase contact line increased on less carefully prepared surfaces is ascribed to the corrugation of the three phase contact line.

1876. Li, D., and J. Zhao, “Surface biomedical effects of plasma on polyetherurethane,” J. Adhesion Science and Technology, 9, 1249-1261, (1995).

Surface biomedical effects of plasma treatment and plasma polymerization on medical-grade polyetherurethane were studied. N2 and Ar plasma treatments and hexamethyldisiloxane (HMDS) plasma polymerization were performed at a power of 100 W with exposure times ranging from 1 to 15 min. The results showed that the contact angle of water was decreased from 79° to 62° by N2 and Ar plasma treatments, and N2 plasma treatment caused a slight enhancement in anti-coagulability and anti-calcific behavior. HMDS polymerization resulted in a decrease from 79° to 43° in the contact angle and an increase from 30.5 to 37.4 s in the recalcification time. At the same time, the anti-coagulability of polymerized samples for the exposure time of 2-5 min was 2.5 times that of the untreated sample. Results of XPS and ESR analyses showed that HMDS deposited onto the polyetherurethane surface and formed new Si-N bonds, and increased the number of radicals in the sample. XPS analysis also showed that N2 and Ar plasma treatments broke some of the CSingle BondO and CDouble BondO bonds at the surface and resulted in oxidation of the surface.

1930. Li, L.-H., C. Macosko, G.L. Korba, A.V. Pocius, and M. Tirrell, “Interfacial energy and adhesion between acrylic pressure sensitive adhesives and release coatings,” J. Adhesion, 77, 95-123, (Oct 2001).

The interfacial adhesive behavior between acrylic pressure sensitive adhesive-like networks (PSA-LNs) and poly(vinyl N-alkyl carbamate) release coatings was studied using a contact mechanical method and peel tests. Surface energy and interfacial energy were directly measured in JKR tests using a novel sample construction. The surface energy of the poly(vinyl N-alkyl carbamates) was found to be around 20 mJ/m2. Interfacial energies between PSA-LNs and the release coatings were found to be quite high – between 7 and 24 mJ/m2. Changes in adhesion dynamics were governed by acid-base interactions between the carbamate in the release coating and the acid groups in the PSA-LN. The length of the alkyl chain in the release coating moderated this effect. We also found a correlation between fundamental adhesion energy and peel strength. Examination of this phenomenon provides a basis for understanding the poor storage stability of PSA tapes made using alkyl carbamates and acid-containing PSAs.

1932. Li, L.-H., M. Tirrell, G.A. Korba, and A.V. Pocius, “Surface energy and adhesion studies on acrylic pressure sensitive adhesives,” J. Adhesion, 76, 307-334, (Aug 2001).

The surface energy and adhesion dynamics of pressure sensitive adhesives-like networks (PSA-LNs) as mimics for PSAs were studied using JKR-based contact mechanics and peel tests. Acrylic acid (AA) was co-polymerized with 2-ethyl hexyl acrylate (2-EHA) and 1,6-hexane diol diacrylate (HDDA) to create PSA-LNs. The measured surface energy (27 to 31 mJ/m2) was sensible as surmised from their structure. Acrylic acid content increases the surface energy, threshold adhesion energy and adhesion hysteresis of PSA-LNs. Measurements of adhesion dynamics showed a dependence of adhesion energy to the 0.6–0.8 power of crack speed, depending upon the model chosen for analysis of the data. When compared with actual pressure-sensitive adhesive tape peel tests, the adhesion dynamics data predicted the peel strength. This study shows a direct relationship between threshold adhesion energy, crack propagation mechanics and peel strength measurements.

1738. Li, Q., P.P. Tsai, S. Nourgostar, Z. Chen, J.R. Roth, et al, “Processing of films and fabrics with the MOD III roll-to-roll one atmosphere uniform glow discharge plasma (OAUGDP) reactor,” in 16th IEEE International Pulsed Power Conference, IEEE, Jun 2007.

Atmospheric pressure plasma treatment has unique advantages over vacuum treatment for such industrial applications as surface energy ehancement of materials, cleaning, decontamination, and sterilization of surfaces, surface etching, plasma chemical vapor deposition (PCVD), and related tasks. The MOD VIII plasma reactor system has been developed to provide roll-to-roll surface treatment of fabrics and films using a One Atmosphere Uniform Glow Discharge Plasma (OAUGDP®) operating in air. Webs can be continuously and uniformly treated by proper control of gas flow; electrode configuration; plasma voltage, current, and frequency; fabric speed; and fabric tension.

711. Li, S., D.Y. Wu, W.S. Gutowski, and H.J. Griesser, “Surface dynamics and adhesive bonding of plasma-treated polyolefins and fluoropolymers,” Presented at First International Congress on Adhesion Science and Technology, Oct 1995.

1801. Li, S.K., R.P. Smith, and A.W. Neumann, “Wilhelmy technique and solidification front technique to study the wettability of fibres,” J. Adhesion, 17, 105-122, (Aug 1984).

The strength of fibre-reinforced materials depends heavily on the adhesion between the fibre and the resin. To predict the bond strength of the adhesion, it is desirable for the surface tension of the fibre to be known. Two independent methods, the Wilhelmy balance method and the solidification front method, were investigated. The fibres used for this investigation included a carbon fibre, Thornel 300®, and an aromatic poiyamide fibre, Kevlar.

In the Wilhelmy experiments three liquids, ethylene glycol, glycerol and distilled water were employed to measure the surface tensions of the test fibres. They were found to be 42.4 mJ/m2 and 43.7 mJ/m2 for the carbon fibre and Kevlar, respectively. These values agreed very well with the results obtained from the solidification front method, from which the carbon fibre was found to have a surface tension value of 41.8 mJ/m2 while that for Kevlar was 46.4 mJ/m2. Furthermore, error analysis has shown that the error limits of the experiments are within 5% of the resulting values. The reproducibility and accuracy of these two techniques indicate that they are viable for determining the surface tension of small diameter fibres.

2714. Li, X., M. Toro, F. Lu, J. On, A. Bailey, and T. Debies, “Vacuum UV photo-oxidation of polystyrene,” J. Adhesion Science and Technology, 30, 2212-2223, (2016).

Polystyrene (PS) was treated with vacuum UV (VUV) (λ = 104.8 and 106.7 nm) photo-oxidation and X-ray photoelectron spectroscopy detected a controlled increase in the atomic percentage of oxygen up to a saturation level of ca. 20 at% O. Initially, C–O and carbonyl groups are observed due to the formation of alcohols, ethers, esters, and ketones. Water contact angle measurements showed ca. 25% increase in hydrophilicity of the surface with oxidation. Atomic Force Microscopy observed little changes in surface roughness with treatment time. The super water absorbent polymer poly(acrylic acid) was thinly grafted to the modified PS surface.

2710. Li, Y., J. Sun, L. Yao, F. Ji, S. Peng, Z. Gao, and Y. Qiu, “Influence of moisture on effectiveness of plasma treatments of polymer surfaces,” J. Adhesion Science and Technology, 26, 1123-1139, (2012).

In atmospheric pressure plasma treatments water molecules in the substrate material may disrupt the molecular arrangement in the substrate and thus greatly influence the outcome of the plasma treatment. This paper summarizes the results of our recent studies on how moisture influences the etching, surface chemical modification, crystallinity and aging of aramid, ultrahigh molecular weight polyethylene (UHMWPE), polyamide fibers, and poly(vinyl alcohol) (PVA) films. Overall, a higher moisture regain often results in a greatly enhanced etch rate, less surface chemical composition change, increased near-surface crystallinity, which could lead to a higher surface wettability, higher interfacial shear strength between the fibers and resin, decreased water solubility for PVA films, and delayed hydrophobic recovery of plasma treated fibers. Therefore, it is important to control the moisture contained in the substrate in atmospheric pressure plasma treatments.

519. Liao, W.-C., and J.L. Zatz, “Surfactant solutions as test liquids for measurements of critical surface tension,” J. Pharmaceutical Science, 68, 486-488, (1979).

Contact angles of various liquids and surfactant solutions on polytef and paraffin were measured. Critical surface tension values were obtained by extrapolation of plots of cosine of the contact angles versus corresponding surface tension values. Contact angles measured using polyoxyethylene octylphenols produced linear Zisman plots and yielded critical surface tensions that agreed with accepted values. This liquid series provides a reasonable approach to the measurement of critical surface tension for solid drugs that are soluble in organic liquids but relatively insoluble in water.

952. Liebel, G., “Plasma activation: Industrial technology for large-scale treatment of polypropylene, polyethylene and polypropylene/ethylene-propylene terpolymer (EPDM) parts,” Technics Plasma, 0.

765. Liggieri, L., and F. Ravera, “Capillary pressure tensiometry with applications in microgravity,” in Drops and Bubbles in Interfacial Research, Mobius, D., and R. Miller, eds., 239-278, Elsevier, Jun 1998.

The CPT has consequently been employed with several configurations and with different methodologies to measure the interfacial tension of pure liquids and for studying the dynamics of adsorption on different time scales both on earth and in microgravity. Some of these methodologies are described in detail, discussing the critical aspects and the main experimental results. Capillary Pressure (CP) tensiometry is especially helpful for studying liquid/liquid interfaces. Microgravity represents an ideal tool for studying the dynamic aspects of adsorption of soluble surfactants and the CP tensiometry is the most suitable technique for these kind of studies in this environment, both for liquid-liquid and liquid-vapor interfaces. However, provided that the Bond number is sufficiently small, CP tensiometry can also be used in normal laboratory conditions.

2912. Lightfoot, T., “There's more than one way to treat a film,” PFFC, 27, 26-28, (Jul 2022).

2031. Lim, H., Y. Lee, S. Han, and J. Cho, “Surface treatment and characterization of PMMA, PHEMA, and PHPMA,” J. Vacuum Science and Technology A, 19, 1490-1496, (Jul 2001).

Poly(methylmethacrylate) (PMMA), poly(2-hydroxyethyl methacrylate (PHEMA), and poly(2-hydroxypropyl methacrylate) (PHPMA) were modified to improve the wettability by two techniques: plasma and plasma source ion implantation. The modified surfaces were characterized to investigate the dependence of the modification and hydrophobic recovery on the polymer structure. The differences obtained under optimal experiment conditions among the polymers were interpreted in terms of their polymer structures including the glass transition temperature. The surface free energy, calculated from the contact angle measurements, revealed that its polar component was a dominant factor in improving the wettability. The PSII treatment created more functional groups on the surface and extensively modified the polymer layer than the plasma treatment.

1867. Lin, D.G., “Layer-by-layer modification of thermoplastic coatings to improve adhesion,” J. Adhesion Science and Technology, 11, 1563-1575, (1997).

One of the causes leading to low bond strength between a coating and a substrate (adhesion strength) - if coatings are formed at elevated temperatures in air - is assumed to be a weak boundary layer generated in the region of adhesional contact: the boundary layer consisting mostly of low-molecular-weight products resulting from thermal oxidative degradation of the polymer. It has been verified experimentally that products of oxidation diffuse from the coating surface layer to the contact area. The oxidation process is supposed to be localized within that surface layer. A method has been devised to determine the thickness of the layer, and model experiments have been conducted to show that low-molecular-weight products of oxidation deteriorate the adhesion strength. Ways have been found to increase the adhesion strength of coatings by means of modification of the coating applied in a layer-by-layer manner. The idea is to introduce separately such modifiers as antioxidants, inorganic fillers possessing high adsorption capacities, and crosslinking agents into the coating surface layer. This method of coating modification allows one to eliminate the negative effects of the low-molecular-weight products generated in the surface layers during the formation.

1304. Lin, F.Y.H., D. Li, and A.W. Neumann, “Effect of surface roughness on the dependence of contact angles on drop size,” J. Colloid and Interface Science, 159, 86-95, (1993).

Absence of drop size dependence of contact angles of sessile drop systems is sometimes observed in experiments. The contact angle data sometimes fluctuate periodically about a horizontal line. Moreover, in cases where a drop size dependence of contact angles exists, the contact angle data often scatter significantly. These fluctuations may be caused by surface roughness. In this paper, two idealized rough surface models are developed. The mean contact angle of a sessile drop in each rough solid surface model is calculated. The fluctuations of the drop size dependence of contact angles produced by these models resemble those obtained experimentally and the fluctuations may therefore be a consequence of the roughness on solid surfaces. It is also concluded that the apparent absence of drop size dependence of contact angles does not necessarily imply zero or extremely low line tension.

1033. Lin, G., W. Wenig, and J. Petermann, “Influence of thermal treatment on the adhesion of polypropylene/ethylene-propylene copolymer interfaces,” Angewandte Makromolekulare Chemie, 255, 33-36, (Mar 1998).

The influence of thermal treatment on the adhesion between isotactic poly(propylene) (iPP) and ethylene-propylene copolymer has been studied. The adhesive force between the polymer films was measured by performing peel tests. It was found that an interface layer has been formed. Its structure and thickness are dependent on the thermal history of the sample: the peel strength increases with annealing temperature and time, and the cooling rate, too, influences the peel strength. The method of preparing the iPP films has an effect on the adhesion of the sandwich sample as well.

2793. Lin, K., M. Vuckovac, M. Latikka, T. Huhtamiiki, and R.H.A. Ras, “Improving surface-wetting characterization,” Science, 363, 1147-1148, (Mar 2019).

Highly hydrophobic surfaces have numerous useful properties; for example, they can shed water, be self-cleaning, and prevent fogging (1, 2). Surface hydrophobicity is generally characterized with contact angle (CA) goniometry. With a history of more than 200 years (3), the measurement of CAs was and still is considered the gold standard in wettability characterization, serving to benchmark surfaces across the entire wettability spectrum from superhydrophilic (CA of 0°) to superhydrophobic (CA of 150° to 180°). However, apart from a few reports [e.g., (48)], the inherent measurement inaccuracy of the CA goniometer has been largely overlooked by its users. The development of next-generation liquid-repellent coatings depends on raising awareness of the limitations of CA measurements and adopting more sensitive methods that measure forces.

2521. Lin, T.-K., S.-J. Wu, C.-K. Peng, and C.-H. Yeh, “Surface modification of polytetrafluoroethylene films by plasma pretreatment and graft copolymerization to improve their adhesion to bismaleimide,” Polymer International, 58, 46-53, (Jan 2009).

BACKGROUND: Polytetrafluoroethylene (PTFE) is utilized in many engineering applications, but its poor wettability and adhesion properties with other materials have limited its use. The study reported was aimed at achieving surface modification of PTFE films by radiofrequency NH3 and N2 plasma treatment, followed by graft copolymerization, in order to improve the interfacial adhesion of PTFE and bismaleimide.

RESULTS: X-ray photoelectron spectroscopy results showed that a short-time plasma treatment had a distinct defluorination effect and led to nitrogen functional group formation. The nitrogen chemical bonding form was different for NH3 and N2 plasma treatments. Under the same experimental conditions, the NH3 plasma exhibited a better etching effect than did the N2 plasma. Contact angle measurement showed an improvement in both surface energy and wettabliity by short-time plasma treatment. The concentration of the surface-grafted bismaleimide on PTFE increased after the plasma pretreatment. The lap shear strength between PTFE and bismaleimide increased significantly after surface modification.

CONCLUSION: This study found that plasma treatment caused changes in surface chemistry, thus leading to an increase of the wettability of PTFE surfaces. Hence, the adhesion properties of PTFE with bismaleimide were significantly improved. Copyright © 2008 Society of Chemical Industry

222. Lindholm, G., “Ink transfer in flexo,” Flexo, 23, 40-45, (Feb 1998).

759. Lindland, H.T., “Flame surface treatment,” in Coatings Technology Handbook, Satas, D., ed., 287-294, Marcel Dekker, 1991 (also in Coatings Technology Handbook, 2nd Ed., D. Satas and A.A. Tracton, eds., p. 343-350, Marcel Dekker, Jan 2001, and Coatings Technology: Fundamentals, Testing, and Processing Techniques, A.A. Tracton, ed., p. 39/1-39/7, CRC Press, Oct 2006).

 

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