ACCU DYNE TEST ™ Bibliography
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1530. Fowkes, F.M., and M.A. Mostafa, “Acid-base interactions in polymer adsorption,” Industrial & Engineering Chemistry Product Research & Development, 17, 3-7, (1978).
1480. Fowkes, F.M., and R.F. Gould, eds., Contact Angle, Wettability and Adhesion: The Kendall Award Symposium Honoring William A. Zisman (Advances in Chemistry Series 43), American Chemical Society, 1964.
103. Fowkes, F.M., and W.D. Harkins, “The state of monolayers adsorbed at the interface solid-aqueous solution,” J. American Chemical Society, 62, 3377-3386, (1940).
104. Fowkes, F.M., and W.M. Sawyer, “Contact angles and boundary energies of a low energy solid (letter),” J. Chemical Physics, 20, 1652, (1952).
1789. Fox, H.W., P.W. Taylor, and W.A. Zisman, “Polyorganosiloxanes: Surface active properties,” Industrial and Engineering Chemistry, 39, 1401-1409, (1947).
109. Fox, H.W., and W.A. Zisman, “The spreading of liquids on low energy surfaces, I. Polytetrafluoroethylene,” J. Colloid Science, 5, 514-531, (1950).
110. Fox, H.W., and W.A. Zisman, “The spreading of liquids on low energy surfaces, II. Modified tetrafluoroethylene polymers,” J. Colloid Science, 7, 109-121, (1952).
111. Fox, H.W., and W.A. Zisman, “The spreading of liquids on low energy surfaces, III. Hydrocarbon surfaces,” J. Colloid Science, 7, 428-442, (1952).
112. Fox, H.W., and W.A. Zisman, “The spreading of liquids on low energy surfaces, VI. Branched-chain monolayers, aromatic surfaces, and thin liquid films,” J. Colloid Science, 8, 194-203, (1953).
861. Fracassi, F., “Architecture of RF plasma reactors,” in Plasma Processing of Polymers (NATO Science Series E: Applied Sciences, Vol. 346), d'Agostino, R., P. Favia, and F. Fracassi, eds., 47-64, Kluwer Academic, Nov 1997.
459. Frederickson, G.H., “Surface ordering phenomena in block copolymer melts,” Macromolecules, 20, 2335-2342, (1987).
2700. French, J., P. Nugent, F. Laxamana, and A. Adarlo, “Ozone adhesion process for insulating container manufacture,” U.S. Patent 9694521, Jul 2017.
1980. Frerichs, H., J. Stricker, D.A. Wesner, and E.W. Kreutz, “Laser-induced surface modification and metallization of polymers,” Applied Surface Science, 86, 405-410, (Feb 1995).
113. Freud, B.B., and H.Z. Freud, “A theory of the ring method for the determination of surface tension,” J. American Chemical Society, 52, 1772-1782, (1930).
2908. Frickley, J., “Solid, liquid, gas and plasma energy: 3DT's improved PlasmaDyne Pro,” Plastics Decorating, 18, (Apr 2022).
2513. Fridman, A., A. Chirokov, and A. Gutsol, “Non-thermal atmospheric pressure discharges,” J. Physics D: Applied Physics, 38, R1-R24, (2005).
There has been considerable interest in non-thermal atmospheric pressure discharges over the past decade due to the increased number of industrial applications. Diverse applications demand a solid physical and chemical understanding of the operational principals of such discharges. This paper focuses on the four most important and widely used varieties of non-thermal discharges: corona, dielectric barrier, gliding arc and spark discharge. The physics of these discharges is closely related to the breakdown phenomena. The main players in electrical breakdown of gases: avalanches and streamers are also discussed in this paper. Although non-thermal atmospheric pressure discharges have been intensively studied for the past century, a clear physical picture of these discharges is yet to be obtained.
114. Friedman, S., “In for a treat,” Package Printing, 45, 42-44, (Apr 1998).
115. Friedman, S., “Surface Buzz,” Package Printing, 46, 68-74, (Oct 1999).
1029. Friedrich, J., “Plasma treatment of polymers,” Adhasion Kleben & Dichten, 41, 28-33, (1997).
846. Friedrich, J., G. Kuhn, R. Mix, I. Retzko, V. Gerstung, St. Weidner, R.-D. Schul, “Plasma polymer adhesion promoters for metal-polymer systems,” in Polyimides and Other High Temperature Polymers: Synthesis, Characterization and Applications, Vol. 2, Mittal, K.L., ed., 359-388, VSP, Jun 2003.
1583. Friedrich, J., I. Loeschcke, H. Frommelt, et al, “Aging and degradation of poly(ethylene-terephthalate) in an oxygen plasma,” Polymer Degradation and Stability, 31, 97-114, (1991).
1212. Friedrich, J., W. Unger, A. Lippitz, L. Wigant, and H. Wittrich, “Corona, spark and combined UV and ozone modification of polymer films WeBP23,” Surface and Coatings Technology, 98, 879-885, (Jan 1998).
1163. Friedrich, J., and G. Kuhn, “Contribution of chemical interactions to the adhesion between evaporated metals and functional groups of differeent types at polymer surfaces,” in Adhesion: Current Research and Applications, Possart, W., ed., 265-288, Wiley-VCH, Dec 2005.
2575. Friedrich, J.F., The Plasma Chemistry of Polymer Surfaces: Advanced Techniques for Surface Design, Wiley-VCH, 2012.
1891. Friedrich, J.F., L. Wigant, W. Unger, et al, “Barrier properties of plasma-modified polypropylene and polyethylene terephthalate,” J. Adhesion Science and Technology, 9, 1165-1180, (1995) (also in Polymer Surface Modification: Relevance to Adhesion, K.L. Mittal, ed., p. 121-136, VSP, May 1996).
2539. Friedrich, J.F., R. Mix, and G. Kuhn, “Adhesion of metals to plasma-induced functional groups at polymer surfaces,” Surface and Coatings Technology, 200, 565-568, (Oct 2005).
The peel strength of aluminium to polypropylene and poly(tetrafluoroethylene) was determined in dependence on the type and the concentration of functional groups on the polymer surface. For this purpose the polymer surface was equipped with monotype functional groups. The first method to produce monotype functionalized surfaces was an introduction of O functional groups using an oxygen plasma treatment and converting these groups to OH groups applying a wet chemical reduction. In result of this two-step treatment the hydroxyl group concentration at the polymer surface could be increased from 3–4 to 10–14 OH groups/100 C atoms. The second method consists in the deposition of a 150 nm adhesion-promoting layer of plasmapolymers or copolymers onto the polymer surface using the pulsed plasma technique. For that purpose functional groups carrying monomers as allyl alcohol, allylamine and acrylic acid were used. Applying the plasma-initiated copolymerization and using neutral “monomers” like ethylene or butadiene the concentration of the functional groups was varied.
A correlation of peel strength with the ability of forming chemical interactions between Al atoms and functional groups was found: COOH > OH >> NH2 > H(CH2–CH2).
2514. Friedrich, J.F., R. Mix, and S. Wettmarshausen, “A new concept for adhesion promotion in metal-polymer systems by introduction of covalently bonded spacers at the interface,” J. Adhesion Science and Technology, 22, 1123-1143, (2008).
A new concept for molecular interface design in metal–polymer systems is presented. The main features of this concept are the replacement of weak physical interactions by strong covalent bonds, the flexibilization of the interface for compensating different thermal expansions of materials by using long-chain flexible and covalently bonded spacers between the metal and the polymer as well as its design as a moisture-repellent structure for hindering diffusion of water molecules into the interface and hydrolysis of chemical bonds. For this purpose, the main task was to develop plasmachemical and chemical techniques for equipping polymer surfaces with monotype functional groups of adjustable concentration. The establishing of monotype functional groups allows grafting the functional groups by spacer molecules by applying usual wet-chemical reactions. Four processes were favoured for production of monotype functional groups by highly selective reactions: the plasma bromination, the plasma deposition of plasma polymers, the post-plasma chemical reduction of O-functionalities to OH-groups, and the chemical replacement of bromine groups by NH2-groups. The grafting of flexible organic molecules as spacers between the metal layer and polymer improved the peel strength of the metal. To obtain maximal peel strength of aluminium coatings to polypropylene films and occurrence of cohesive failure in the polypropylene substrate, about 27 OH groups per 100 C-atoms or 6 COOH groups per 100 C-atoms were needed. Introducing C6–11-aliphatic spacers 1 OH or COOH group per 100 C-atoms contributed about 60% of the maximal peel strength of the Al–PP system, i.e. 2 or 3 spacer molecules per 100 C-atoms were sufficient for maximal peel strength.
712. Friedrich, J.F., W. Unger, A. Lippitz, L. Wigant, et al, “Differences in surface oxidation of PP by corona, spark, and low-pressure oxygen discharge treatments and the relevance to adhesion,” Presented at First International Congress on Adhesion Science and Technology, Oct 1995.
1892. Friedrich, J.F., W. Unger, A. Lippitz, et al, “The improvement in adhesion of polyurethane-polypropylene composites by short-time exposure of polypropylene to low and atmospheric pressure plasmas,” J. Adhesion Science and Technology, 9, 575-598, (1995) (also in Polymer Surface Modification: Relevance to Adhesion, K.L. Mittal, ed., p. 49-72, VSP, May 1996).
1582. Friedrich, J.F., W.E.S. Unger, A. Lippitz, et al, “Chemical reactions at polymer surfaces interacting with a gas plasma or with metal atoms - their relevance to adhesion,” Surface and Coatings Technology, 119, 772-782, (Sep 1999).
1946. Fritz, J.L., and M.J. Owen, “Hydrophobic recovery of plasma-treated polydimethylsiloxane,” J. Adhesion, 54, 33-45, (Dec 1995).
1770. Fu, R.K.Y., I.T.L. Cheung, Y.F. Mei, et al, “Surface modification of polymeric materials by plasma immersion ion implantation,” Nuclear Instruments and Methods in Physics Research, B237, 417-421, (2005).
Polymer surfaces typically have low surface tension and high chemical inertness and so they usually have poor wet-ting and adhesion properties. The surface properties can be altered by modifying the molecular structure using plasma immersion ion implantation (PIII). In this work, Nylon-6 was treated using oxygen/nitrogen PIII. The observed improvement in the wettability is due to the oxygenated and nitrogen (amine) functional groups created on the polymer surface by the plasma treatment. X-ray photoelectron spectroscopy (XPS) results show that nitrogen and oxygen plasma implantation result in C–C bond breaking to form the imine and amine groups as well as alcohol and/or car-bonyl groups on the surface. The water contact angle results reveal that the surface wetting properties depend on the functional groups, which can be adjusted by the ratio of oxygen–nitrogen mixtures.
460. Fulcher, M.R., “An evaluation of the measurement of wettability (MS thesis),” Univ. of Notre Dame, 1985.
972. Gabriele, M.C., “Corona systems keep pace with end-use demands,” Modern Plastics Intl., 29, 28-29, (Feb 1999).
1046. Gabriele, M.C., “'Cold-plasma' system takes on polyolefin parts,” Modern Plastics Intl., 28, 46, (Feb 1998).
461. Gagnon, D.R., and T.J. McCarthy, “Polymer surface reconstruction by diffusion of organic functional groups from and to the surface,” J. Applied Polymer Science, 29, 4335-4340, (1984).
1562. Gao, L., and T.J. McCarthy, “Ionic liquids for surface analysis,” PMSE Preprints, 97, 534-535, (Apr 2007).
2286. Gao, L., and T.J. McCarthy, “Teflon is hydrophilic: Comments on definitons of hydrophobic, shear versus tensile hydrophobicity, and wettability characterization,” Langmuir, 24, 9183-9188, (2008).
Comments are made concerning the recent use of adjectives to describe solid surfaces that exhibit anomalously high water contact angle values. We suggest that the meaning of the word hydrophobic be resolved before it is modified, for example, to superhydrophobic and further modified, for example, to sticky superhydrophobic and before the definitions of these new words become issues of contention. The case is made that the first statement in the title is appropriate with experiments that demonstrate significant attractive interaction between liquid water and the surface of solid Teflon. Four types of experiments are described: the interaction of a silicon-supported covalently attached perfluoroalkyl monolayer (a model Teflon surface) with a sessile water drop (1) and with a thin film of water on a clean silicon wafer surface (2), the interaction of 1 and 12 microm diameter solid Teflon particles with a water droplet surface (3), and the interaction of a thin (<5 microm) Teflon film with a water droplet (4). The concepts of shear and tensile hydrophobicity are introduced, and the recommendation that two numbers, advancing and receding contact angle values, should be considered necessary data to characterize the wettability of a surface. That the words hydrophobic, hydrophilic, and their derivatives can and should only be considered qualitative or relative terms is emphasized.
2287. Gao, L., and T.J. McCarthy, “An attempt to correct the faulty intuition perpetuated by the Wenzel and Cassie 'laws',” Langmuir, 25, 7249-7255, (2009).
We respond to a recent report in this journal that criticizes our experiments, which disproved the Wenzel and Cassie theories. The criticism is that we measured contact angles “with drops that were too small, ignoring the indications of existing theoretical understanding.” We take a step back to give an explanation of what we believe to be the reason that the “existing theoretical understanding” is wrong. We explain that the teaching of surface science has led generations of students and scientists to a misunderstanding of the wetting of solids by liquids. This continues as evidenced by this recent criticism and numerous recent papers. We describe several demonstrations that were designed to help teachers, students, and scientists overcome the widespread learning disability that is rooted in their faulty intuition and to help them regard wetting from the perspective of lines and not areas.
2288. Gao, L., and T.J. McCarthy, “Wetting 101,” Langmuir, 25, 14105-14115, (2009).
We review our 2006−2009 publications on wetting and superhydrophobicity in a manner designed to serve as a useful primer for those who would like to use the concepts of this field. We demonstrate that the 1D (three-phase, solid/liquid/vapor) contact line perspective is simpler, more intuitive, more useful, and more consistent with facts than the disproved but widely held-to-be-correct 2D view. We give an explanation of what we believe to be the reason that the existing theoretical understanding is wrong and argue that the teaching of surface science over the last century has led generations of students and scientists to a misunderstanding of the wetting of solids by liquids. We review our analyses of the phenomena of contact angle hysteresis, the lotus effect, and perfect hydrophobicity and suggest that needlessly complex theoretical understandings, incorrect models, and ill-defined terminology are not useful and can be destructive.
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