ACCU DYNE TEST ™ Bibliography
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2226. Gatenby, A., “CSC Scientific blog: Surface tension and interfacial tension,” http://www.cscscientific.com/csc-cientific-blog/bid/25530/, Nov 2008.
2227. Gatenby, A., “CSC Scientific blog: Having trouble performing a DuNouy ring test in thick samples?,” https://www.cscscientific.com/csc-scientific-blog/having-trouble-performing-a-dunouy-ring-test-in-thick-samples, Nov 2010.
2228. Gatenby, A., “CSC Scientific blog: How does surface tension relate to viscosity?,” https://www.cscscientific.com/csc-scientific-blog/how-does-surface-tension-relate-to-viscosity, Jan 2011.
2259. Gatenby, A., “CSC Scientific blog: Why calibrate a CSC DuNouy tensiometer?,” https://www.cscscientific.com/csc-scientific-blog/why-calibrate-a-csc-dunouy-tensiometer, Sep 2011.
2298. Gatenby, A., “CSC Scientific blog: Which type of tensiometer do I need?,” https://www.cscscientific.com/csc-scientific-blog/which-type-of-tensiometer-do-i-need, Dec 2011.
2475. Gatenby, A., “CSC Scientific blog: What are the primary conditions affecting surface tension?,” https://www.cscscientific.com/csc-scientific-blog/what-are-the-primary-conditions-affecting-surface-tension, Sep 2013.
2592. Gatenby, A., “CSC Scientific blog: How are consistency, surface tension, and viscosity different?,” https://www.cscscientific.com/csc-scientific-blog/how-are-consistency-surface-tension-and-viscosity-different, Feb 2014.
2652. Gatenby, A., “CSC Scientific blog: Should you move to 'actual' surface tension?,” https://www.cscscientific.com/csc-scientific-blog/should-you-convert-to-actual-surface-tension, Sep 2016.
2791. Gatenby, A., “CSC Scientific blog: Surface tension - rings, bubbles, drops, and plates,” https://www.cscscientific.com/csc-scientific-blog/surface-tension-rings-bubbles-drops-and-plates, Feb 2019.
2915. Gatenby, A., “CSC Scientific blog: Guide to surface tension, surfactants and micelles,” https://www.cscscientific.com/csc-scientific-blog/topic/surfactants, Oct 2022.
3043. Gatenby, A., “CSC Scientific blog: A classical definition of contact angle,” https://www.cscscientific.com/csc-scientific-blog/initiation-to-contact-angle, Aug 2016.
1889. Gatenholm, P., C. Bonnerup, and E. Wallstrom, “Wetting and adhesion of water-borne printing inks on surface-modified polyolefins,” J. Adhesion Science and Technology, 4, 817-827, (1990).
Polyolefin films were surface-modified by different methods to improve the wetting and adhesion of water-borne printing inks. Polyethylene (PE) films were treated with corona at various energy levels. Surface-modified PE films were characterized by contact angle measurements and electron spectroscopy for chemical analysis (ESCA). Good wetting was already achieved with treatment at a lower energy level. Various degrees of adhesion were obtained at various degrees of treatment. A hydrophilic monomer, 2-hydroxyethylmethacrylate (HEMA), was polymerized onto the surfaces of polypropylene (PP) with radiation-induced grafting, which was carried out at two different radiation doses. In both cases, a thick, visible layer of polyHEMA was formed on the surface of PP, and satisfactory wetting was already achieved at lower radiation doses. Scanning electron microscopy (SEM) showed that different degrees of roughness were achieved at various radiation doses. Like the case of corona-treated PE, different degrees of adhesion were obtained at different degrees of surface treatment. This study shows that improved wetting alone is not satisfactory for good practical adhesion', regardless of the surface modification method used.
1767. Gavrilov, N.V., V.N. Mizgulin, R. Stinnett, and A.V. Kondyurin, “Modification of polymer films of PE, PTFE, PC, PI by pulse ion beams,” Khimicheskaya Fizika i Mesoskopiya, 1, 39-47, (1999).
463. Gaydos, J., E. Moy, and A.W. Neumann, “Reply to 'On the existence of an equation of state for interfacial free energies' (letter),” Langmuir, 6, 888-892, (1990).
1597. Gaydos, J., and A.W. Neumann, “The dependence of contact angles on drop size and line tension,” J. Colloid and Interface Science, 76, 120+, (1987).
We report contact angle measurements of five n-alkanes, dodecane through hexadecane, on Teflon (FEP) as a function of drop size. In all cases the contact angles decreased by approximately 5° when the drop size was increased from approximately 1 to 4 mm contact radius. A complete solution to the problem of mechanical equilibrium of a sessile drop on a solid surface indicates that the dependence of the contact angle on drop size may be explained by including the effect of line tension in the Young equation. The observed drop size dependence of the contact angle yields a line tension of (2.5 ± 0.5) × 10−6 J/m. Over the range of n-alkanes studied it was not possible to discern any dependence of the line tension on liquid surface tension.
2411. Geibart, D., “Method of surface preparation using plasma in air,” U.S. Patent 6476342, Nov 2002.
In accordance with the present invention, a directed plasma beam is employed in air to selectively remove coatings from paper products at high production rates. The shape and intensity of the beam is controlled to obtain a controlled rate of removal of the coating. The method does not require vacuum to be established and allows for the plasma to be generated from high pressure air.
122. Geitner, W., “Flame treatment effect on OPP,” AIMCAL News, 14, (Aug 2001).
2722. Geng, X., Q. Qiang, J. Zhao, J. Yang, and Z. Wang, “The effect of TiO2 morphology on the surface modification of poly(ethylene terephthalate) for electroless plating,” J. Adhesion Science and Technology, 29, 705-715, (2015).
In this study, a surface modification of the poly (ethylene terephthalate) (PET) film using TiO2 photocatalytic treatment was investigated. In order to enhance the adhesion strength between the PET film and the electroless copper film, the effects of TiO2 crystal forms, TiO2 particle sizes, and TiO2 content, as well as treatment condition, upon the surface contact angle, surface characterization, and adhesion strength were investigated. Anatase TiO2 with a particle size of 5 nm had a high catalytic activity and dispersibility in aqueous solution. After the optimal photocatalytic treatment, the surface contact angle of the PET film decreased from 84.4° to 19.8°, and the surface roughness of the PET film increased from 36 to 117 nm. The adhesion strength between the PET film and the electroless copper film reached 0.89 KN m−1. X-ray photoelectron spectroscopy analyses indicated the carbonyl group was formed on the PET surface after photocatalytic treatment, and the surface hydrophilicity was improved. Consequently, TiO2 photocatalytic treatment is an environmentally friendly and effective method for the surface modification of the PET film.
1447. Gengenbach, T.R., X. Xie, R.C. Chatelier, and H.J. Griesser, “Evolution of the surface composition and topography of perfluorinated polymers following ammonia-plasma treatment,” J. Adhesion Science and Technology, 8, 305-328, (1994) (also in Plasma Surface Modification of Polymers: Relevance to Adhesion, M. Strobel, C.S. Lyons, and K.L. Mittal, eds., p. 123-146, VSP, Oct 1994).
Treatment of fluorinated ethylene propylene (FEP) and polytetrafluoroethylene (PTFE) in ammonia plasmas produced surfaces with very high wettability by water, but on storage in air at ambient temperature, the air/water contact angles increased markedly. The evolution of the surface composition and topography was studied by angle-dependent X-ray photoelectron spectroscopy (XPS), derivatization of amine groups with fluorescein isothiocyanate, scanning tunelling microscopy (STM), and atomic force microscopy (AFM). XPS demonstrated a continuous increase in the oxygen content over periods of weeks; this was assigned to oxidation of trapped radicals and subsequent secondary reactions. In addition, the fluorine content also changed markedly on storage; the XPS fluorine signal suggested that there was a substantial amount of fluoride in the freshly treated surfaces, and this component disappeared rapidly on storage. STM and AFM showed no changes in topography with aging but suggested surface hardening on plasma treatment. The events following treatment of FEP and PTFE in ammonia plasmas are not adequately described by a model involving plasma-induced, instantaneous chemical modification followed by surface restructuring; the surface and sub-surface compositions evolve over a period of several weeks due to the occurrence of oxidative reactions, and these chemical changes interact with the physical process of surface restructuring.
123. Gengler, P., “The role of dielectrics in corona treating,” Converting, 8, 62-66, (Jun 1990).
124. Gengler, P., “Corona treating equipment for the flexographic printer,” Flexo, 18, 36-38, (Mar 1993).
2331. Gent, A.N., and J. Schultz, “Effect of wetting liquids on the strength of adhesion of visoelastic materials,” J. Adhesion, 3, 281-294, (1973) (also in Recent Advances in Adhesion, L.-H. Lee, ed., Gordon and Breach, p. 253-268, 1973).
The effect of a variety of wetting liquids on the resistance to peeling separation for a lightly crosslinked rubbery adhesive in contact with a Mylar substrate has been studied over a wide range of peeling rates and at two temperatures. Although the magnitude of the peel strength is much greater than the thermodynamic work of detachment, it is reduced by alcohols and alcohol/water mixtures in good agreement with calculated reduction factors. It is concluded that the measured strength is a product of two terms: the thermodynamic work, and a numerical factor, generally large, denoting inefficiency. The latter term is strongly dependent on peel rate and temperature for viscoelastic adhesives. Two anomalies are pointed out: particularly low adhesion is observed at low rates of peel for certain liquids, attributed to swelling of the adhesive, and smaller effects are found for some other liquids than predicted.
894. Genuario, L., “Corona treatment,” Label & Narrow Web Industry, 7, 58-64, (Oct 2002).
1109. Genuario, L., “Surface treatment,” Label and Narrow Web, 10, 50-56, (Jan 2005).
125. George, G.A., “Surface modification and analysis of ultra-high modulus polyethylene fibres for composites,” in Polymer Surfaces and Interfaces II, Feast, W.J., H.S. Munro, and R.W. Richards, eds., 161-202, John Wiley & Sons, Apr 1993.
826. Gerenser, L.J., “XPS studies of in situ plasma-modified polymer surfaces,” J. Adhesion Science and Technology, 7, 1019-1040, (1993) (also in Plasma Surface Modification of Polymers: Relevance to Adhesion, M. Strobel, C.S. Lyons, and K.L. Mittal, eds., p. 43-64, VSP, Oct 1994).
X-ray photoelectron spectroscopy (XPS) has been used to study the chemical effects of both inert (argon) and reactive (oxygen, nitrogen, and mixed gas) plasma treatments done in situ on a variety of polymer surfaces. Inert gas plasma treatments introduce no new detectable chemical species onto the polymer surface but can induce degradation and rearrangement of the polymer surface. However, plasma treatments with reactive gases create new chemical species which drastically alter the chemical reactivity of the polymer surface. These studies have also shown that the surface population of chemical species formed after plasma treatment is dependent on both the chemical structure of the polymer and the plasma gas. The effects of direct and radiative energy-transfer processes in a plasma have also been studied. Polymers containing certain functional groups were found to be more susceptible to damage via radiative energy transfer. Ageing studies of plasma-modified polymer surfaces exposed to the atmosphere have shown that the ageing process consists of two distinct phases. The initial phase, which occurs rapidly, involves adsorption of atmospheric contaminants and, in some cases, specific chemical reactions. The second phase, which occurs slowly, is due to surface reorganization.
1744. Gerenser, L.J., “X-Ray photoemission study of plasma modified polyethylene surfaces,” J. Adhesion Science and Technology, 1, 303-318, (1987).
X-Ray photoelectron spectroscopy (XPS) was used to determine plasma induced chemical species on the surface of polyethylene (PE). Argon plasmas were found to have no detectable chemical effect on the PE surface, whereas oxygen and nitrogen plasmas created new chemical species which altered the chemical reactivity of the PE surface. Oxygen plasmas were found to react more rapidly with the PE surface than nitrogen plasmas. The degree of incorporation of new chemical species in the near surface region is approximately 20 at. % at the saturation level for both oxygen and nitrogen plasmas. Core level spectra for oxygen and nitrogen plasma treated PE suggest the formation of primarily C-O-C species in the former and C-N species in the latter. Angle-resolved XPS measurements indicate that the depth of incorporation of new chemical species is confined to the top 25 A.
126. Gerenser, L.J., J.F. Elman, M.G. Mason, and J.M. Pochan, “ESCA studies of corona-discharge-treated polyethylene surfaces by use of gas-phase derivatization,” Polymer, 26, 1162-1166, (1985).
Chemically specific gas-phase reactions have been used to tag corona-discharge-induced chemical species on the surface of polyethylene. These tag reactions provide distinct moieties that can be detected via e.s.c.a. to provide a surface count of induced species. Hydroxyl, epoxy, hydroperoxy, carboxylic acid and carbonyl populations are discussed as a function of corona energy input, time after treatment and water washings.
127. Gerenser, L.J., J.M. Pochan, J.F. Elman, and M.G. Mason, “Effect of corona discharge treatment of poly(ethylene terephthalate) on the adsorption characteristics of the fluorosurfactant Zonyl FSC as studied via ESCA and surface energy measurements,” Langmuir, 2, 765-770, (1987).
1286. Gerenser, L.S., “XPS studies of in-situ plasma-modified polymer surfaces,” J. Adhesion Science and Technology, 7, 1019-1040, (1993).
X-ray photoelectron spectroscopy (XPS) has been used to study the chemical effects of both inert (argon) and reactive (oxygen, nitrogen, and mixed gas) plasma treatments done in situ on a variety of polymer surfaces. Inert gas plasma treatments introduce no new detectable chemical species onto the polymer surface but can induce degradation and rearrangement of the polymer surface. However, plasma treatments with reactive gases create new chemical species which drastically alter the chemical reactivity of the polymer surface. These studies have also shown that the surface population of chemical species formed after plasma treatment is dependent on both the chemical structure of the polymer and the plasma gas. The effects of direct and radiative energy-transfer processes in a plasma have also been studied. Polymers containing certain functional groups were found to be more susceptible to damage via radiative energy transfer. Ageing studies of plasma-modified polymer surfaces exposed to the atmosphere have shown that the ageing process consists of two distinct phases. The initial phase, which occurs rapidly, involves adsorption of atmospheric contaminants and, in some cases, specific chemical reactions. The second phase, which occurs slowly, is due to surface reorganization.
2844. Gerke, G., “Can plasma surface treatment deliver sustainable solutions and reduce cost?,” https://digitaledition.flexpackmag.com/march-2021/plasma-surface/?oly_enc_id=1127B7669590J0V, Mar 2021.
464. Gerstenberg, K.W., “Corona pretreatment to allow wetting and bonding,” Deutsch Papierwirtsch, 1, 8, (1990).
128. Gervason, G., J. Ducom, and H. Cheradame, “Relationship between surface energy and adhesion strength in polyethylene-paper composites,” British Polymer Journal, 21, 53-59, (1989).
This work reports adhesion behaviour of polyethylene on paper, and deals with the surface energy of the materials involved in the manufacture of these composites, and its influence on the adhesion strength, at constant roughness, for the paper substrates. The surface energy of different papers treated with various sizing agents was determined by measuring contact angles according to the Owens-Wendt method. The peeling energy was shown to follow a linear relationship versus the reversible energy of adhesion. This result is explained by the fact that rupture takes place at the interface and that the size of the defect at the interface depends on the spreading coefficient. Corona treatment, applied to strongly sized papers before making the composites, restored the adhesion strength to its original range of values, again demonstrating the thermodynamic character of adhesion in thermoplastic-paper composites.
1481. Ghali, K., B. Jones, and J. Tracy, “Experimental techniques for measuring parameters describing wetting and wicking in fabrics,” Textile Research J., 64, 106-111, (1994).
Once capillary pressure and permeability are determined for saturations ranging from near zero to 100%, liquid transport related to both wicking and wetting behavior can be described by Darcy's equation. The purpose of the work reported here is to assess and develop experimental techniques that allow capillary pressure and per meability to be measured over a wide range of saturations. Cotton and polypropylene fabrics are the test materials. Capillary pressure head is measured as a function of saturation for cotton and polypropylene fabric samples using the column test, and permeability is measured as a function of saturation using the siphon test. The siphon test works for cotton but not for polypropylene. A new method using a transient measurement technique is developed to determine the permeability of both samples as a function of saturation; it works well for both samples.
129. Ghannam, M.T., and M.N. Esmail, “The effect of pre-wetting on dynamic contact angle,” Canadian J. Chemical Engineering, 70, 408-412, (1992).
A roll-coating experimental system is used to study the effect of pre-wetting on dynamic contact angles, the interfacial displacement depth, and the associated phenomenon of air entrainment. The system consists of a roll, which is horizontally rotating in a liquid pool. The dynamic contact angle is recorded by a macrophotography system. The test liquids are glycerol solutions with viscosities in the range 104 < μ < 748 mPa · s. The value of (μV/ρg)0.5 is taken as the characteristic length to be used in the dimensionless relationships which correlate experimental measurements. The effect of base layer entry angle into the liquid pool on the dynamic contact angles and other flow parameters is studied. Comparison is made with measurements in dry tape-coating and other pre-wet roll–coating systems.
756. Gheorghiu, M., G. Popa, M. Pascu, and C. Vasile, “Chemical and physical surface modifications of polymers by ion beam treatments,” in Metallized Plastics: Fundamentals and Applications, K.L. Mittal, ed., 269-280, Marcel Dekker, Nov 1997.
Knowing that the oriented positive ion bombardment plays an important role in the plasma treatments of polymers, some investigations using a positive ion beam-plasma system were carried out. Preliminary results concerning the surface modifications of poly (ethylene terephthalate) films induced by the action of oxygen ion beam are presented. Ion energies (50-500 eV) and doses (3.0 x1015 1.5 x1016 ions/cm²) are those used in a reactive ion etching device. Techniques such as: determination of the surface free energy components by the contact angle method, thermal methods (DTA, DSC, etc.), IR spectroscopy, SEM, XPS, were used to characterize the surface modifications. The relation between chemical and physical modifications is discussed.
879. Gheorghiu, M., M.C. Pascu, and G. Popa, “Surface modifications of polyolefins by gas-phase methods,” in Handbook of Polyolefins, 2nd Ed., Vasile, C., ed., 649-688, Marcel Dekker, Jun 2000.
1869. Ghosh, I., J. Konar, and A.K. Bhowmick, “Surface properties of chemically modified polyimide films,” J. Adhesion Science and Technology, 11, 877-893, (1997).
Surface modification of Kapton polyimide film (325 nm thick) by means of chromic acid and perchloric acid at different times and temperatures has been carried out. The contact angle of water decreased from 82 to 55° and the surface energy increased accordingly from 26 to 45 mJ/m2 with times of etching by chromic acid up to 45 min at 33°C. Etching at higher temperatures increased the surface energy. Chromic acid was more effective than perchloric acid. IR and XPS studies indicated multiple bonding and generation of poler groups on the surface. The peak at 1778 cm-1 due to the imide group decreased on acid etching. The O/C ratio increased and the N/C ratio decreased. The peel strength of the joint polyimide film/copper film/epoxy adhesive/aluminium sheet increased about two-fold on modification of the polyimide (PI) film at 33°C for 45 min, although the changes were marginal for the PI film/silicone rubber/PI film joint. The peel strength is a function of the time and temperature of etching.
2021. Giacometti, J.A., S. Fedosov, and M.M. Costa, “Corona charging of polymers: Recent advances on constant current charging,” Brazilian J. Physics, 29, (Jun 1999).
This paper contains a brief overview on the recent developments of corona charging of polymers, with emphasis on the current corona triode. This latter method, which has been successfully applied to several types of polymer, is a legacy from Prof. Bernhard Gross' work in São Carlos, Brazil. Following a short introduction to corona charging, the experimental setups are described, especially with regard to the advantages in the constant current method. A few examples are given of the use of the constant current corona triode in the investigation of electrical properties of nonpolar and ferroeleectric polymers. The application of corona charging to pole nonlinear optic (NLO) polymers is discussed, including the perspectives for the constant current charging method for the NLO field.
1997. Gifford, W.A., “The effect of contact angle on ring tensiometry,” J. Colloid and Interface Science, 64, 588-591, (May 1978).
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