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1080. Martin-Martinez, J.M., M.D. Romero-Sanchez, C.M. Cepeda-Jiminez, et al, “Surface treatments to improve vulcanised latex adhesion: Current state of the art,” in Polymers in Building and Construction (Rapra Review Report 154), 157-178, Rapra, Feb 2003.

2530. Crutchley, E.B., Innovation Trends in Plastics Decoration and Surface Treatment: Decorative Effects on Moulded Plastics, Rapra Publishing, 2014.

1436. Brewis, D.M., and R.H. Dahm, Adhesion to Fluoropolymers (Rapra Review Report 183), Rapra Technology, Jul 2006.

2337. Zisman, W.A., “Surface properties of plastics,” Record of Chemical Progree, 26, 23+, (1965).

1599. Harkins, W.D., The Physical Chemistry of Surface Films, Reinhold, 1952.

935. Cormia, R.D., “Use plasmas to re-engineer your advanced materials,” Research & Development, (Jul 1990).

2515. Williams, T.S., H. Yu, and R.F. Hicks, “Atmospheric pressure plasma activation of polymers and composites for adhesive bonding: A critical review,” Rev. Adhesion and Adhesives, 1, 46-84, (Feb 2013).

A review is presented on the surface preparation of polymers and composites using atmospheric pressure plasmas. This is a promising technique for replacing traditional methods of surface preparation by abrasion. With sufficient exposure to the plasma afterglow, polymer and composite surfaces are fully activated such that when bonded and cured with epoxy adhesives, they undergo 100% cohesive failure in the adhesive. Depending on the material, the lap shear strength and crack delamination resistance (GIC) can be increased several fold over that achieved by either solvent wiping or abrasion. In some cases, a plasma-responsive layer must be incorporated into the top resin layer of the composite to achieve maximum bond strength to the adhesive. Adhesion does not correlate well with water contact angle or surface roughness. Instead it correlates with the fraction of the polymer surface sites that are oxidized and converted into active functional groups, as determined by x-ray photoelectron spectroscopy and infrared spectroscopy.

74. de Gennes, P.-G., “Wetting: statics and dynamics,” Review of Modern Physics, 57(3), P1, 827-863, (1985).

The wetting of solids by liquids is connected to physical chemistry (wettability), to statistical physics (pinning of the contact line, wetting transitions, etc.), to long-range forces (van der Waals, double layers), and to fluid dynamics. The present review represents an attempt towards a unified picture with special emphasis on certain features of “dry spreading”: (a) the final state of a spreading droplet need not be a monomolecular film; (b) the spreading drop is surrounded by a precursor film, where most of the available free energy is spent; and (c) polymer melts may slip on the solid and belong to a separate dynamical class, conceptually related to the spreading of superfluids.

12. Badran, A.A., and E. Marschall, “Oscillating pendant drop: A method for the measurement of dynamic surface and interfacial tension,” Review of Scientific Instrumentation, 57, 259-263, (Feb 1986).

A method is described for measuring dynamic surface and interface tension. The technique is essentially a variation of the pendant drop method in which the drop is allowed to oscillate after sudden formation at the tip of a syringe. Immediately after the oscillation stops but before the drop detaches, there is an instant of rest. At this moment, the profile of the drop is obtained using high‐speed photography. The boundary tension is then calculated from the profile using established methods. The technique is demonstrated on systems consisting of aqueous solutions of sodium stearate or oleate on one hand and mineral oil or air on the other hand. Surface or interface tensions may be obtained within 0.25 to 5 s after surface formation.

268. Ohsawa, T., and T. Ozaki, “New method for determination of surface tension of liquids,” Review of Scientific Instrumentation, 52, 590-593, (1981).

A new method of quickly and precisely measuring the surface tension of liquids and solutions is described. Utilizing the fact that the size of the bubbles formed from a gas flowing out of a nozzle is dependent on the nozzle diameter and the surface tension of the liquid used, the surface tension of a liquid can be determined by simply counting the number of bubbles formed from a gas flowing out at a constant flow rate or by measuring the period of bubble formation. The expected accuracy of the method is below 0.1% of variance. An evident correlation between the period of bubble formation and the surface tension was shown with several kinds of liquids which differ in surface tension. Changes in surface tension with varied degree of neutralization were determined in an aqueous solution of polyacrylic acid (PAA), 20-30 points of measurement with an accuracy of about 0.1% could be easily obtained within one hour.

837. Etzler, F.M., “Determination of the surface free energy of solids,” Reviews of Adhesion and Adhesives, 43, 3-45, (Feb 2013).

Knowledge of the surface free energy of solids is important to understanding a number of processes involving wetting and adhesion to solid surfaces. The measurement of surface free energy has been a subject of active interest for at least 50 years. Despite the importance of the problem to a variety of industries a universally accepted method or set of methods for determination of solid surface free energies has not been agreed upon. In this review article various methods that have been used for the calculation of surface free energies are discussed. The limitations and concerns for employment of each of these methods are furthermore highlighted. Of principal concern is the use of contact angles that meet the requirements to be Young’s contact angles and the mixing of quantities obtained by contact angle measurements with those obtained by IGC, as surface free energies obtained by IGC tend to be larger than those obtained from contact angle measurements. Calculated values from IGC data are presumably larger than those from contact angle data as IGC data are often collected at very low surface coverages.

963. no author cited, “Polarised flame treatment,” Revista de Plasticos Modernos, 79, 252-254, (Mar 2000).

853. Bergbreiter, D.E., “New synthetic methodology for grafting at polymer surfaces,” in Chemically Modified Surfaces, Pesek, J.J. and I.E. Leigh, eds., 24-40, Royal Society of Chemistry, 1994.

2767. Sherman, P.B., and M.P. Garrard, “Surface treatments for plastic films and containers,” in Plastics: Surface and Finish, 2nd Ed., Simpson, W.G., ed., 221-236, Royal Society of Chemistry, 1995.

944. Jensen, W.B., “Lewis acid-base interactions and adhesion theory,” Rubber Chemistry and Technology, 55, 881-901, (1982).

The above results are intended to be suggestive rather than definitive. Nevertheless, they strongly support the premise that a cross-fertilization of both concepts and experimental data from the apparently unrelated fields of Lewis acid-base chemistry and adhesion theory can lead to potentially valuable results for both fields, emphasizing again the value of using a generalized acid-base vocabulary in describing the phenomena of chemistry, whatever one's area of specialization.

1749. Crocker, G.J., “Elastomers and their adhesion,” Rubber Chemistry and Technology, 42, 30+, (Feb 1969).

633. Ellul, M.D., and D.R. Hazleton, “Chemical surface treatments of natural rubber and EDPM thermoplastic elastomers: effects on friction and adhesion,” Rubber and Chemical Technology, 67, 582-601, (Sep 1994).

Natural rubber thermoplastic elastomers (NRTPEs) made by dynamic vulcanization of natural rubber during its mixing with polypropylene were subjected to various halogenation surface treatments. Marked reduction in the coefficient of friction is possible depending on the chemical treatment employed, TPE composition and the presence of a lubricant. As a result of halogenation there is an increase in the microroughness and hardness of the NRTPE surface. These effects in part explain the large decrease in the friction coefficients since the contact area is decreased. Thus NRTPE can be employed in applications requiring low friction, such as certain types of seals. Another consequence of halogenation of NRTPE is the increase in its surface energy which in turn promotes adhesion to various polar substrates. Indeed it was determined that halogenation of NETPE is an effective way of priming the surface of these materials for adhesion to acrylic and other substrates. Ethylene Propylene Diene Monomer rubber-Polypropylene thermoplastic elastomers (EPTPEs) were used as a control in this study to assess how a low unsaturation EPDM-based TPE compares with the high unsaturation NRTPEs in different halogenation surface treatments.

2161. Glogauer, S., “Plasma and adhesion to rubber, plastics substrates,” Rubber and Plastics News, 38, 16-19, (Jun 2009).

World-class, fully automated manufacturing processes rely more and more on advanced, environmentally friendly surface treatment technologies. An innovative atmospheric pressure plasma technique allows inline rubber and plastic manufacturing processes to become fully automated with total process control. A thorough pretreatment must produce surfaces with reliable and repeatable characteristics to achieve optimal adhesive bonding, coating and printing results. In addition, pretreatment must be delivered in a cost-effective and safe manner. The new process uses the high effectiveness of plasma for microfine cleaning, high-surface activation and nanocoating. In most cases the plasma application takes the place of environmentally unfriendly and costly solvent cleaning or chemical adhesion promoters and primers.

2079. Kucherenko, O.B., C. Kohlert, E.A. Sosnov, and A.A. Malygin, “Synthesis and properties of polyvinyl chloride films with modified surface,” Russian J. Applied Chemistry, 79, 1316-1320, (Aug 2006).

Atomic-force microscopy was used to study structural chemical transformations on the surface of polyvinyl chloride films subjected to modification with compounds based on acrylic acid derivatives, with preliminary activation of the polymer surface with a corona discharge.

945. Gray, V.R., “Contact angles, their significance and measurement,” in S.C.I. Monograph #25 : Wetting, 99-119, S.C.I., 1966.

2570. Wolf, R.A., “Advances in adhesion with CO2-based atmospheric pressure plasma surface modification,” in ANTEC Conference Proceedings, SPE, 2007 (also in 2008 PLACE Conference Proceedings, TAPPI Press, p. 834-838, Sep 2008).

The use of gas and/or liquid-phase carbon dioxide (CO2) with atmospheric plasma discharge surface pretreatment technology can remove micron and submicron particulates and hydrocarbon-based contaminations on plastics and metals. The cleaning process is based upon the expansion of either liquid or gaseous carbon dioxide through an orifice. The paper provides an understanding of the basic removal mechanism and provides experimental evidence of remarkable adhesion improvements relative to a broad range of applications in electrical, medical, and automotive manufacturing communities.

1023. Ayres, R.L., and D.L. Shofner, “Preparing polyolefin surfaces for inks and adhesives,” SPE Journal, 28, 51-55, (Dec 1972).

508. Koo, M.-N., “The effect of drop size on contact angle (MS thesis),” SUNY Buffalo, 1979.

576. Shu, L.-K., “Contact angles and determination of the components of surface energy of polymer surfaces (PhD dissertation),” SUNY Buffalo, 1991.

55. Chaudhury, M.K., and G.M. Whitesides, “Correlation between surface free energy and surface constitution,” Science, 255, 1230-1232, (Mar 1992).

Self-assembled monolayers (SAMs) of alkylsiloxanes on elastomeric PDMS (polydimethylsiloxane) were used as model systems to study interactions between surfaces. Surface free energies (γsv) of these chemically modified surfaces were estimated by measuring the deformations that resulted from the contact between small semispherical lenses and flat sheets of the elastomer under controlled loads. The measured surface free energies correlated with the surface chemical compositions of the SAMs and were commensurate with the values estimated from the measurements of contact angles. This study provides direct experimental evidence for the validity of estimates of the surface free energies of low-energy solids obtained from contact angles.

209. Langmuir, I., “Overturning and anchoring of monolayers,” Science, 87, 493-500, (1938).

238. Miller, S.A., H. Luo, S.J. Pachuta, and R.G. Cooks, “Soft-landing of polyatomic ions at fluorinated self-assembled monolayer surfaces,” Science, 275, 1447-1449, (Mar 1997).

A method of preparing modified surfaces, referred to as soft-landing, is described in which intact polyatomic ions are deposited from the gas phase into a monolayer fluorocarbon surface at room temperature. The ions are trapped in the fluorocarbon matrix for many hours. They are released, intact, upon sputtering at low or high energy or by thermal desorption, and their molecular compositions are confirmed by isotopic labeling and high-resolution mass measurements. The method is demonstrated for various silyl and pyridinium cations. Capture at the surface is favored when the ions bear bulky substituents that facilitate steric trapping in the matrix.

332. Sharp, K.A., A. Nichols, R.F. Fine, and B. Honig, “Reconciling the magnitude of the microscopic and macroscopic hydrophobic effects,” Science, 252, 106-109, (Apr 1991).

The magnitude of the hydrophobic effect, as measured from the surface area dependence of the solubilities of hydrocarbons in water, is generally thought to be about 25 calories per mole per square angstrom (cal mol-1 Å-2). However, the surface tension at a hydrocarbon-water interface, which is a "macroscopic" measure of the hydrophobic effect, is ≈72 cal mol-1 Å-2. In an attempt to reconcile these values, alkane solubility data have been reevaluated to account for solute-solvent size differences, leading to a revised "microscopic" hydrophobic effect of 47 cal mol-1 Å-2. This value, when used in a simple geometric model for the curvature dependence of the hydrophobic effect, predicts a macroscopic alkane-water surface tension that is close to the macroscopic value.

454. Dorsey, N.E., “Ring methods for surface tension measurement,” Science, 69, 189+, (1929).

1117. Ryu, D.Y., K. Shin, E. Drockenmuller, C.J. Hawker, and T.P. Russell, “A generalized approach to the modification of solid surfaces,” Science, 308, 236-238, (Apr 2005).

Interfacial interactions underpin phenomena ranging from adhesion to surface wetting. Here, we describe a simple, rapid, and robust approach to modifying solid surfaces, based on an ultrathin cross-linkable film of a random copolymer, which does not rely on specific surface chemistries. Specifically, thin films of benzocyclobutene-functionalized random copolymers of styrene and methyl methacrylate were spin coated or transferred, then thermally cross-linked on a wide variety of metal, metal oxide, semiconductor, and polymeric surfaces, producing a coating with a controlled thickness and well-defined surface energy. The process described can be easily implemented and adapted to other systems.

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.

2997. Riyanto, E., “Surface treatment of polyimide using atmospheric pressure dielectric barrier discharge plasma,” ScienceAsia, 46, 444-449, (2020).

In this study, polyimide was treated by atmospheric pressure dielectric barrier discharge plasma using a helium and/or helium-oxygen mixture gasses. The polyimide was placed between copper electrodes with dielectric material installed on the cathode electrode. To investigate the surface treatment, the plasmas as a function of power, treatment time, and plasma gasses were introduced on the polyimide substrate. The experimental results show that the polyimide treated by dielectric barrier discharge plasma increases the wetting property. This property can be attributed to the surface roughness and the water compatible functional groups. The roughness increases by helium plasma treatment and can be further improved by increasing plasma power or the presence of oxygen in the helium-oxygen mixture plasma. On the other hand, the plasma surface treatment led to formation of oxygen related functional groups of -C=O and -OH.

345. Smith, R.E., “UV inks + plastics = web/treater combo,” Screen Graphics, 4, 56-63, (Jul 1998).

926. Pennance, J.R., “Printing on plastic films: problems with surface tension,” Screen Printing, 73, 108-109, (Jun 1983).

7. Agler, S., “Are your bottles print ready?Understanding treatments for surface tension,” ScreenPrinting, 84, 100, (Jan 1994).

133. Gilleo, K.B., “Rheology and surface chemistry for screen printing,” ScreenPrinting, 79, 128, (Feb 1989).

219. Leech, C.S. Jr., “Surface tension and surface energy: Practical procedures for printing on problem plastics,” ScreenPrinting, 81, 52-62, (Jan 1991).

236. Maxham, D., “Pushing the limits: halftone screen printing on plastic containers,” ScreenPrinting, 83, 106-108, (Feb 1993).

257. Newberry, D., “Glass and ceramic surface dynamics,” ScreenPrinting, 85, 32-36, (Jul 1995).

285. Pennance, J.R., “The role of surface tension in printing on plastic films,” ScreenPrinting, 78, 64-69, (Jul 1988).

 

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