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2678. Hejda, F., P. Solar, and J. Kousal, “Surface free energy determination by contact angle measurements - a comparison of various approaches,” in WDS '10 Proceedings, Part III, 25-30, MATFYZ Press, 2010.

One of the parameters characterizing the surfaces of materials is the surface free energy. The most common way to determine its value is to measure the surface tension by the sessile drop method. In this case a contact angle between the surface and the edge of droplets of liquids is measured. There are various approaches to calculate the surface free energy from the contact angle measurements. We made a review and a direct comparison of the most widely used methods and testing liquids in order to re-evaluate their advantages and disadvantages. In the presented work we discuss the limits of applicability of the examined methods. We confirm that methods using a pair of liquids give results dependent on the liquids chosen. Using a pair of non-polar and polar liquid yielded most reliable results. This is even more clear when two-liquid method is transformed into a multiple-liquid method. The algorithms developed during the work will be implemented into liquid contact angle analysis software.

511. Lee, B.-I., “Low temperature plasma surface treatment of polymers and fillers (graduate thesis),” MIT, 1971.

556. Sarabia, A., “Plasma surface treatment of poly(phenyl sulfide) and poly(etheretherketone) prior to adhesive bonding (MS thesis),” MIT, 1987.

1742. Coates, D.M., and S.L. Kaplan, “Modification of polymeric surfaces with plasma,” MRS Bulletin, 21, 43-45, (1996).

As adaptable as polymeric materials are in their many applications to our daily lives, the need exists to tailor the polymer surfaces to provide even more flexibility in regard to their uses. Plasma treatments offer an unprecedented spectrum of possible surface modifications to enhance polymers, ranging from simple topographical changes to creation of surface chemistries and coatings that are radically different from the bulk polymer. Furthermore plasma treatments are environmentally friendly and economical in regard to their use of materials.

Plasma processing can be classified into at least four categories that often overlap. These are the following: (1) surface preparation by breakdown of surface oils and loose contaminates, (2) etching of new topographies, (3) surface activation by creation or grafting of new functional groups or chemically reactive, excited metastable species on the surface, and (4) deposition of monolithic, adherent surface coatings by polymerization of monomeric species on the surface. Key features of these processes will be briefly discussed, with a rudimentary introduction to the chemistries involved, as well as examples. Focus is placed on capacitively coupled radio-frequency (rf) plasmas (see Figure 1 in the article by Lieberman et al. in this issue of MRS Bulletin) since they are most commonly used in polymer treatment.

3109. Poirier, A., G.G. Ross, P. Bertrand, and V. Wiertz, “Modification of wetting property of polycarbonate by means of ion beam implantation and storage in different gas environments,” MRS Online Proceedings Library, 504, 425-430, (1998).

The wetting property of polymers is very important in different applications such as biomaterials, textiles, aerospace (fluid management and materials processing in microgravity), and thin film adhesion. Therefore, there is a strong interest in the development of a new technology for the modification at will of this property. The use of low energy ion beams allows the modification of the first surface atomic layers. Nitrogen ions of 500 eV/at. were used to bombard the surface of polycarbonate (PC) samples to a fluence of 5×1016 at/cm2. Five different environments (oxygen, nitrogen, argon, dry air and vacuum) were used to store the samples for some hours (1 to 24 hours) after the implantation. Aging studies of the contact angle (advancing and receding) have shown that the environment gas influences the long term value of the contact angle and helps to maintain the stability of the treated surfaces with the passage of time. XPS and ToF-SIMS have been used to study the chemical effects of both N2 + ion irradiation and storage gas surrounding the samples. The results show faster aging in the case of the samples stored in vacuum, a harmful effect of nitrogen gas on the treatment and the formation of new chemical species for all treatments.

2469. no author cited, “Bonding low surface energy plastics,” Machine Design, 0, (Jun 2000).

1013. Poncin-Epaillard, F., J.C. Brosse, and T. Falher, “Reactivity of surface groups formed onto a plasma treated poly(propylene) film,” Macromolecular Chemistry & Physics, 200, 989-996, (May 1999).

Cold plasma treatments of polymers, dry processes, allow either the elaboration of hydrophilic or hydrophobic surfaces. For example, a poly(propylene) film treated in nitrogen plasma shows a surface having a hydrophilic and basic character since amino groups are attached onto the surface during the treatment. The treatment induces an increase of the surface tension of the polymeric material, which may be sometimes destroyed by an aging effect. For the treatment of poly(propylene) in nitrogen plasma, the aging is mostly due to a motion of attached groups from the surface to the bulk of the material and some oxidation of radicals formed during plasma treatment. The surface radicals formed and used for a post-reaction such as grafting are characterized in terms of chemical nature, density and reactivity.

1479. Chehimi, M.M., E. Cabet-Deliry, A. Azioune, and M.L. Abel, “Characterization of acid-base properties of polymers and other materials: Relevance to adhesion science and technology,” Macromolecular Symposia, 178, 169-181, (2002).

This paper reviews the background to the theory of Lewis acid-base (AB) interactions in adhesion, adsorption, wetting and mixing of polymers and other materials (pigments, fillers, fibres, etc.). These specific materials interactions require the revision of old concepts («polar» interactions) and the development of new analytical techniques and methodologies. Four of the most currently used techniques to characterize AB interactions are described: contact angle measurements, inverse gas chromatography. X-ray photoelectron spectroscopy, and atomic force microscopy.

2100. Severini, F., L. Di Landro, L. Galfetti, L. Meda, G. Ricca, and G. Zenere, “Flame surface modification of polyethylene sheets,” Macromolecular Symposia, 181, 225-244, (May 2002).

High density polyethylene sheets 2 mm thick were flame treated to modify the surface properties. Sheets treated using a flame with air to gas (methane) ratio ∼ 10:1 at different distances between the inner cone tip of the flame and the polymer surface were investigated. Grafting of selected monomers as maleic anhydride, acrylamide and glycidyl methacrylate was attempted by flame treatment of sheets covered with a monomer layer. Good grafting results were obtained with acrylamide and maleic anhydride. The surface temperature-time dependence during the flame treatment was measured with a high resolution thermocouple. Scanning Electron Microscopy (SEM) allowed evidencing a modified thickness of about 120 μ. The chemical surface modification was studied by X ray Photoelectron Spectroscopy (XPS) and Diffuse Reflectance Infrared Fourier Transform Spectroscopy (DRIFT). The hydroxyl, carbonyl and carboxyl content was measured after derivatization with reagents containing an elemental tag to facilitate XPS analysis of surface functional groups. In comparison to the untreated polyethylene, wetting tension and contact angle of the flamed materials showed a strong variation. This variation was almost independent of the distance between the flame and the polymer surface. Adhesion between treated polyethylene and a polyurethane adhesive was determined using T-peel test measurements. High adhesion levels were found with flame treated polyethylene at 5 mm distance. XPS results indicate that when adhesion is high, the hydroxyl is in excess compared to the other measured functions, i.e. carbonyl and carboxyl species.

261. Nuzzo, R.G., and G. Smolinsky, “Preparation and characterization of functionalized polyethylene surfaces,” Macromolecules, 17, 1013-1019, (1987).

We describe a procedure to modify the surface of polyethylene (PE) film using a combination of gas discharge and wet chemical techniques. This method generates high densities (1014-1016 cm-2) of a specific functionality, largely unaccompanied by other groups, in a 50-100-Å surface layer. The topography of the polymer surface remains unchanged after treatment and functions as an effective starting material for subsequent derivatization by standard synthetic chemical reactions. A plasma of either oxygen, water, or hydrogen is generated under comparable experimental conditions. In all cases a 1-2-s, 5-W, 0.2-Torr treatment produces about the same degree of surface modification as does longer treatment. High-resolution X-ray photoelectron spectroscopy (XPS) shows that either an oxygen or a water plasma produces a variety of oxidation products ranging from alcohols to carboxylic acids. Chromic acid oxidizes the plasma-oxidized surface further to give high densities of carboxylic acid groups which can be readily converted to acid chlorides and derivatized. Borane/tetrahydrofuran reduces the plasma-oxidized surface to give alcohols which can be esterified readily. Contact-angle measurements show that the water-plasma-treated PE surface has a higher surface free energy (γs ∼ 62 dyn/cm) than the oxygen-plasma-treated surface (γs ∼ 50 dyn/cm). A 5-s, ambient-temperature, 0.2-Torr, 2-W hydrogen plasma generates a significant number of quenchable radical sites. XPS spectra of this treated surface, exposed to either nitric oxide or nitrosotrifluoromethane, show that both compounds bond to the surface.

313. Schmidt, J.J., J.A. Gardella, Jr., and L. Salvati Jr., “Surface studies of polymer blends, II. An ESCA and IR study of poly(methylmethacrylate)/poly(vinyl chloride) homopolymer blends,” Macromolecules, 22, 4489-4495, (1989).

Angle-dependent ESCA and ATR-FTIR results are presented for homopolymer blends of poly(Methyl methacrylate) and poly(vinyl chloride}. Blends over the entire composition range were cut from tetrahydrofuran (THF) and methyl ethyl ketone (MEK). Surfacee enrichment of PMMA was present at all compositions of blends cast from THF, while blends cast from MEK exhibited surface compositions that were within error limits equivalent to the bulk compositions in the blends.

321. Schonhorn, H., “Heterogeneous nucleation of polymer melts on high-energy substrates, II. Effect of substrate on morphology and wettability,” Macromolecules, 1, 145-151, (1968).

Heterogeneous nucleation and crystallization of polymer melts against high-energy surfaces (eg, metals, metal oxides, and alkali halide crystals) have been found to result in markedchanges in both thesurface region morphology and wettability of these polymers even though the chemical constitution of the polymer is un-changed. The critical surface tensions (7c) of a variety of polymers nucleated against gold are considerably in excess of the commonly accepted values. Employing a modified Fowkes-Young equation can account for these sizable differences if the surface layer of these crystallizable polymers generated against high-energy surfaces is essentially crystalline.

342. Siow, K.S., and D. Patterson, “The prediction of surface tensions of liquid polymers,” Macromolecules, 4, 26-30, (1971).

361. Suzuki, M., A. Kishida, H. Iwata, and Y. Ikada, “Graft copolymerization of acrylamide onto a polyethylene surface pretreated with a glow discharge,” Macromolecules, 19, 1804-1808, (1986).

364. Thomas, H.R., and J.J. O'Malley, “Surface studies on multicomponent polymer systems by x-ray photoelectron spectroscopy.Polystyrene/poly(ethylene oxide) diblock copolymers,” Macromolecules, 12, 323-329, (1979).

459. Frederickson, G.H., “Surface ordering phenomena in block copolymer melts,” Macromolecules, 20, 2535-2542, (Oct 1987).

A mean field theory is presented to describe surface ordering phenomena in diblock copolymers near the microphase separation transition (MST). We consider a near-symmetric diblock melt in the vicinity of a solid wall or free surface, such as a film-air interface. The surface is allowed to modify the Flory interaction parameter and the chemical potential in the adjacent copolymer layer. The composition profile normal to the surface is investigated both above and below the MST. In contrast to the surface critical behavior of binary fluids or polymer blends, we find interesting oscillatory profiles in copolymers that arise from the connectivity of the blocks. These composition profiles might be amenable to study by ellipsometry, by evanascent wave-induced fluorescence, or by scattering techniques. Wetting and other surface phenomena and transitions in block copolymers are briefly discussed.

479. Hobbs, J.P., C.S.P. Sung, K. Krishnann, and S. Hill, “Characterization of surface structure and orientation in polypropylene and poly(ethylene terephthalate) films by modified attenuated total reflection IR dichromism studies,” Macromolecules, 16, 193-199, (1983).

986. Kang, E.T., K.L. Tan, K. Kato, Y. Uyama, and Y. Ikada, “Surface modification and functionalisation of polytetrafluoroethylene films,” Macromolecules, 29, 6872-6879, (Oct 1996).

Argon plasma-pretreated polytetrafluoroethylene (PTFE) films were subjected to further surface modification by near-UV light-induced graft copolymerization with acrylic acid (AAc), sodium salt of styrenesulfonic acid (NaSS), and N,N-dimethylacrylamide (DMAA). The surface compositions and microstructures of the modified films were characterized by angle-resolved X-ray photoelectron spectroscopy (XPS). A stratified surface microstructure with a significantly higher substrate-to-graft chain ratio in the top surface layer than in the subsurface layer was always obtained for PTFE surface with a substantial amount of the hydrophilic graft. The stratified surface microstructure was consistent with the observed hysteresis in advancing and receding water contact angles. The graft yield increased with Ar plasma pretreatment time and monomer concentration. Covalent immobilization of trypsin on the AAc polymer-grafted PTFE films was facilitated by water-soluble carbodiimide (WSC). The effective enzyme activities increased initially with increasing surface concentration of the grafted AAc polymer but became saturated at a moderate AAc polymer concentration. The immobilized enzyme could still retain close to 30% of its original activity. Solution-coating of the polymeric acid-modified PTFE films with the emeraldine (EM) base of polyaniline readily resulted in an interfacial charge transfer interaction and a semiconductive PTFE surface.

1018. Kuzuya, M., S. Kondo, M. Sugito, and T. Yamashiro, “Peroxy radical formation from plasma-induced surface radicals of polyethylene as studied by electron spin resonance,” Macromolecules, 31, 3230-3234, (May 1998).

The nature of peroxy radical formation from plasma-induced surface radicals of polyethylene (PE), both low-density polyethylene (LDPE) and high-density polyethylene (HDPE), was studied by electron spin resonance with the aid of systematic computer simulations. It was found that peroxy radical formation varies with the structure of component radicals of plasma-irradiated PE, both LDPE and HDPE:  Among three plasma-induced radicals of PE, dangling bond sites (DBS) undergo an instant conversion into the corresponding peroxy radicals in contact with oxygen, while the midchain alkyl radical is of very low reactivity with oxygen in both LDPE and HDPE. Computer simulations disclosed that ESR spectra of peroxy radicals are similar to each other in LDPE and HDPE, both being composed of two types of spectra, a partial >em>g-averaging anisotropic spectrum and a nearly isotropic single line spectrum due to different molecular motional freedom at the trapping sites of peroxy radicals.

1019. Kuzuya, M., T. Yamashiro, S. Kondo, M. Sugito, and M. Mouri, “Plasma-induced surface radicals of low-density polyethylene studied by electron spin resonance,” Macromolecules, 31, 3225-3229, (May 1998).

Plasma-induced low-density polyethylene (LDPE) radicals were studied in detail by electron spin resonance (ESR) by its comparison with ESR of high-density polyethylene (HDPE). The observed ESR spectra of plasma-irradiated LDPE are largely different in pattern from those of HDPE. The systematic computer simulation disclosed that such observed spectra consist of three kinds of radicals, midchain alkyl radical (1), allylic radical (2) as discrete radical species, and a large amount of dangling bond sites (DBS) (3) at an intra- and intersegmental cross-linked region. All these component radicals are essentially identical to those of HDPE. One of the most special features unique to plasma-irradiated LDPE, however, is the fact that thermally stable DBS (3) is a major component radical instead of a midchain alkyl radical in HDPE. This can be ascribed to the difference in polymer morphology between LDPE and HDPE:  branched structure with a large amount of amorphous region for LDPE and linear structure with a large amount of crystalline region for HDPE. Since one of the characteristics of plasma irradiation is the fact that it is surface-limited, LDPE would undergo the radical formation preferentially on the surface-branched structural moiety followed by facile cross-link reactions resulting in the formation of DBS. Thus, the nature of radical formation of PE was found to be affected by the polymer morphology in a very sensitive manner.

1034. Boyd, R.D., A.M. Kenwright, J.P.S. Badyal, and D. Briggs, “Atmospheric non-equilibrium plasma treatment of biaxially oriented polypropylene,” Macromolecules, 30, 5429-5436, (Sep 1997).

The chemical and physical effects incurred at the surface of biaxially oriented polypropylene film during silent discharge plasma treatment have been investigated using XPS, NMR, TOF-SIMS, and AFM techniques. It is found that chain scission accompanied by oxidative attack leads to the formation of low molecular weight oxidized material which agglomerates into globules at the surface due to a large difference in interfacial free energy between the underlying hydrophobic substrate and the oxygenated overlayer.

1786. Carey, D.H., and G.H. Ferguson, “Synthesis and characterization of surface-functional 1,2-polybutadiene bearing hydroxyl or carboxylic acid groups,” Macromolecules, 27, 7254-7266, (1994).

1787. Chapman, T.M., et al, “Determination of low critical surface tensions of novel fluorinated poly(amide urethane) block copolymers I: Fluorinated side chains,” Macromolecules, 28, 331-335, (1995).

1805. Iyengar, D.R., S.M. Perutz, C.-A. Dai, C.K. Ober, and E.J. Kramer, “Surface segregation studies of fluorine-containing diblock copolymers,” Macromolecules, 29, 1229-1234, (1996).

A diblock copolymer of deuterated styrene and isoprene (dPS−PI) with a small volume fraction of isoprene was chemically modified to incorporate pendant fluorinated side chains (“fingers”). The composition distribution of the diblock copolymers within a high molecular weight polystyrene (PS) homopolymer was determined by forward recoil spectrometry. Surface segregation and interfacial segregation of the modified block copolymers from a polystyrene matrix are observed in as-spun films. Equilibrium segregation was achieved on annealing at 160 °C for several days. The segregation isotherms at the air−polymer interface are shown to be quantitatively described by a self-consistent mean field theory (SCMF), and these permit us to estimate an effective Flory parameter which describes the attraction of the fluorinated segments to the surface and their repulsion from the bulk. The change in the surface tension as a result of the adsorption of the block copolymers at the air−homopolymer interface was evaluated from the predictions of SCMF theory and compared with the changes in the water contact angle observed. Advancing water contact angle data are consistent with the presence of a nonuniform layer of PS, CF2, and CF3 segments on the surface of the segregated samples.

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

609. Dick, F., “Beta Kit Wettability Test Solutions,” Marbetech, 1989.

18. Berg, J.C., ed., Wettability, Marcel Dekker, Apr 1993.

19. Berg, J.C., “Role of acid-base interactions in wetting and related phenomena,” in Wettability, Berg, J.C., ed., 75-148, Marcel Dekker, Apr 1993.

26. Blake, T.D., “Dynamic contact angles and wetting kinetics,” in Wettability, Berg, J.C., ed., 251-310, Marcel Dekker, Apr 1993.

35. Bose, A., “Wetting by solutions,” in Wettability, Berg, J.C., ed., 149-182, Marcel Dekker, Apr 1993.

166. Huntsberger, J.R., “Interfacial energies, contact angles, and adhesion,” in Treatise on Adhesion and Adhesives, Vol. 5, 1-20, Marcel Dekker, 1981.

178. Johnson, R.E. Jr., and R.H. Dettre, “Wetting of low energy surfaces,” in Wettability, Berg, J.C., 1-74, Marcel Dekker, Apr 1993.

Wetting involves the interaction of a liquid with a solid. It can be the spreading of a liquid over a surface, the penetration of a liquid into a porous medium, or the displacement of one liquid by another. It can help to characterize surfaces and to determine solid/liquid interactions. Wettability is most often described by a sessile or resting drop. A schematic diagram is shown in Fig. 1. The contact angle (6) is a measure of wettability. A low contact angle means high wettability and a high contact angle means poor wettability. Zero contact angles are possible but they are always less than 180.(The highest commonly observed angle, mercury on glass, has been reported to be as high as 148 [1].) Systems having more than one stable contact angle are said to show contact-angle hysteresis.

196. Kistler, S.F., “Hydrodynamics of wetting,” in Wettability, Berg, J.C., ed., 311-430, Marcel Dekker, Apr 1993.

637. Good, R.J., “Semantic physics of adhesion,” in Treatise on Adhesion and Adhesives, Vol. 5, Patrick, R., ed., 293-312, Marcel Dekker, 1981.

658. Wu, S., Polymer Interface and Adhesion, Marcel Dekker, 1982.

697. Jarvis, S.P., “Adhesion on the nanoscale,” in Nano-Surface Chemistry, Rosoff, M., ed., 17-58, Marcel Dekker, Oct 2001.

717. Neumann, A.W., and J.K. Spelt, eds., Applied Surface Thermodynamics, Marcel Dekker, Jun 1996.

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.

719. Spelt, J.K., and D. Li, “The equation of state approach to interfacial tensions,” in Applied Surface Thermodynamics, Neumann, A.W., and J.K. Spelt, eds., 239-292, Marcel Dekker, Jun 1996.

720. Spelt, J.K., E. Moy, D.Y. Kwok, and A.W. Neumann, “The theory of surface tension components and the equation of state approach,” in Applied Surface Thermodynamics, Neumann, A.W., and J.K. Spelt, eds., 293-332, Marcel Dekker, Jun 1996.

The determination of solid and solid-liquid surface tensions is of importance in a wide range of problems in pure and applied science. There exist, at present, many indirect approaches for obtaining these values because it is not possible to measure directly surface tensions involving a solid phase. These various methods are often in considerable disagreement, both quantitatively and from a theoretical standpoint. The problem persists since most of these approaches have not been tested objectively through the prediction of physical phenomena which could be independently observed and thus used to validate the various theories.

 

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