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2401. Strobel, M.A., M.C. Branch, R.S. Kapaun, and C.S. Lyons, “Flame-treating process,” U.S. Patent 5753754, May 1998.

The present invention provides a method of modifying the surface of a polymeric substrate, e.g., to improve the wettability of the polymer film surface and/or alter the reactivity of the surface of the substrate by further oxidation or affixation of nitrogen, comprising exposing the substrate to a flame. The flame is supported by a fuel and oxidizer mixture that includes an effective amount, for modifying the polymeric substrate, of at least one compound that functions as a fuel or oxidizer substitute and is selected from an oxygen-containing compound, in which the oxygen comprises between about 10 and 50 atomic percent of the compound, a nitrogen-containing compound or an oxygen-nitrogen-containing compound. In a preferred embodiment, which affixes nitrogen or nitrogen-containing chemical groups onto the surface of the film, the flame is supported by a fuel and oxidizer mixture that includes ammonia, nitrous oxide, nitric oxide or a mixture thereof in an effective amount. Large increases in the ASTM wetting test, e.g., greater than 13 mJ/m2 over that reported with conventional flame-treating processes, have been observed in films treated according to this invention. In addition, significant increases in polymer film surface oxidation levels, e.g., as much as 55 percent, have been observed, as have significant amounts of nitrogen and nitrogen-containing chemical groups affixed to film surfaces.

228. Mackey, C.D., “Good adhesive bonding starts with surface preparation,” Adhesives Age, 41, 30-32, (Jun 1998).

762. Chen, P., D.Y. Kwok, R.M. Prokop, O.I. del Rio, S.S. Susnar, and A.W. Neumann, “Axisymmetric drop shape analysis(ADSA) and its applications,” in Drops and Bubbles in Interfacial Research, Mobius, D., and R. Miller, eds., 61-138, Elsevier, Jun 1998.

This chapter discusses axisymmetric drop shape analysis (ADSA) and its application. It provides an account of these ADSA methodologies. It contains a description of the numerical algorithms and their implementation. The applicability of ADSA is illustrated extensively for the investigation of surface tension measurements with pendant and sessile drops and contact angle experiments with sessile drops using both axisymmetric drop shape analysis - profile (ADSA-P) and axisymmetric drop shape analysis - diameter (ADSA-D). The advantages of pendant and sessile drop methods are numerous. In comparison with a method such as the Wilhelmy plate technique, only small amounts of the liquid are required. Drop shape methods easily facilitate the study of both liquid-vapor and liquid-liquid interfacial tensions. Also, the methods have been applied to materials ranging from organic liquids to molten metals and from pure solvents to concentrated solutions. There is no limitation to the magnitude of surface or interracial tension that can be measured: The methodology presented in this chapter works as well at 103 mJ/m 2 as at 10 -3 mJ/m 2.

763. Miller, R., and V.B. Fainerman, “The drop volume technique,” in Drops and Bubbles in Interfacial Research, Mobius, D., and R. Miller, eds., 139-186, Elsevier, Jun 1998.

This chapter focuses on the drop volume technique. The stalagmometer is the most primitive version of the drop volume method. It allows only a very rough estimate of the surface tension of a liquid. With the drop volume technique an accurate determination of the volume of a drop formed at the tip of a given capillary is obtained. The measuring procedure is realized by means of a precise dosing system, which forms drops continuously at the capillary. The method has restrictions for example with respect to the drop formation time. If drops are formed too fast the measured drop volumes are no longer a measure of the surface tension alone but are in addition governed by chaotic effects leading to so-called drop volume bifurcations. A drop volume experiment is described is this chapter.

764. Seifert, A.M., “The spinning drop tensiometry,” in Drops and Bubbles in Interfacial Research, Mobius, D., and R. Miller, eds, 187-238, Elsevier, Jun 1998.

The spinning drop technique (SDT) has been developed to measure extremely low interfacial tensions (from 10 -6 mNm -1 to 10 mNm -1). It uses profile analysis of deformed droplets similar to the pendent drop method. Unlike in pendent drop experiments, where the droplets are deformed by the gravitational force, SDT is based on the balance of centrifugal and interracial forces in rapidly rotating systems. Apart from purely tensiometric applications SDT has been found to be a versatile tool for surface and interface science. It allows the study of adsorption phenomena and even permits the “simulation” of spontaneous structure formation processes, e.g., the break-up of liquid threads and the coalescence of droplets. This chapter reviews both standard and non-standard SDT applications. After a brief description of basic principles and properties, the equilibrium properties of a rotating drop, i.e., its shape and its stability, are considered in detail. Experimental aspects of SDT: Both commercial and laboratory SDT set-ups are introduced. Problems arising from sample preparation (particularly in the case of highly viscous polymers) and the determination of the droplet dimensions are discussed.

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.

766. Fainerman, V.B., and R. Miller, “The maximum bubble pressure tensiometry,” in Drops and Bubbles in Interfacial Research, Mobius, D., and R. Miller, eds., 279-326, Elsevier, Jun 1998.

This chapter focuses on the maximum bubble pressure method (MBPM) and deals with the physico-chemical and hydrodynamic processes taking place at various stages of the growth of a bubble and its separation from a capillary. Particular emphasis is made on theoretical problems like surface tension calculation from the measured excess pressure, surface tension calculation from the measured excess pressure, splitting of time interval between consecutive bubbles into lifetime and deadtime, and calculation of these characteristic times involving inertial and viscous properties of liquid and gas, non-stationarity of flows, etc. Emphasis is also made on experimental details like measurements of pressure and bubble formation frequency and optimisation of the geometry of capillary and measuring system related to the application of the MBPM. The results presented in this chapter contribute both to an improvement of the commercially available devices, and to a better understanding of the method by the users, helping them in the application of the MBPM and in a correct interpretation of the results.

767. Wantke, K.D., and H. Fruhner, “The oscillating bubbles method,” in Drops and Bubbles in Interfacial Research, Mobius, D., and R. Miller, eds., 327-366, Elsevier, Jun 1998.

768. Dukhin, S.S., R. Miller, and G. Loglio, “Physico-chemical hydrodynamics of rising bubble,” in Drops and Bubbles in Interfacial Research, Mobius, D., and R. Miller, eds., 367-432, Elsevier, Jun 1998.

This chapter discusses the physico-chemical hydrodynamics of rising bubble. At small Reynolds numbers effective approximate analytical methods allow to characterize different states of dynamic adsorption layers quantitatively: weak retardation of the motion of bubble surfaces, almost complete retardation of bubble surface motion, transient state at a bubble surface between an almost completely retarded and an almost completely free bubble surface. The measurement of bubble terminal velocity in water cannot be used for the experimental verification of these theories because uncontrolled impurities in water immobilize a small bubble surface almost completely without any addition of surfactant. The rising bubble velocity relaxation caused by the dynamic adsorption layer (DAL) formation can be measured. The DAL study is more realistic for large bubbles and large Reynolds numbers (Re) because trace concentrations of surface active impurities cannot retard the bubble surface movement completely.

769. Passerone, A., and R. Ricci, “High temperature tensiometry,” in Drops and Bubbles in Interfacial Research, Mobius, D., and R. Miller, eds., 475-524, Elsevier, Jun 1998.

This chapter presents after a short reminder of thermodynamic definitions, the most commonly used techniques for surface tension measurements with some details of the most interesting of them for high temperature applications. Some recent results on the evaluation of the influence of external factors, like the surrounding atmosphere, on the determination of the surface tension of molten systems are also presented. ASTRA is an experimental methodology and an integrated software to get and process data of drop shape profiles to determine surface and interfacial tension and contact-angle values. Due to its high performances in terms of time of acquisition and reliability, it is particularly suitable for both static and dynamic measurements. Indeed, by using ASTRA it is possible to reach up to two interfacial tension measurements per second, having access to dynamic measurements over very large time scale. ASTRA is currently used both for liquid metals and for liquid systems at room temperature.

919. Podhajny, R.M., “Evaluating the cure of UV flexographic inks,” Paper Film & Foil Converter, 72, 30, (Jun 1998).

978. Zhang, D., Q. Sun, and L.C. Wadsworth, “Mechanism of corona treatment on polyolefin films,” Polymer Engineering and Science, 38, 965-970, (Jun 1998).

This paper reviews recent studies on the mechanism of corona treatment of polyolefin films, specifically the chemical and physical changes of this process and the self-adhesion mechanism. Corona discharge of polymeric films introduces polar groups into the surfaces, which increases the surface energy and, as a consequence, improves substrate wettability and adhesion. The main chemical mechanism of corona treatment is oxidation. In addition, corona treatment can crosslink surface regions and increase the film cohesive strength.

1794. Deslandes, Y., G. Pleizier, E. Poire, S. Sapieha, M.R. Wertheimer, and E. Sacher, “The surface modification of pure cellulose paper induced by low-pressure nitrogen plasma treatment,” Plasmas and Polymers, 3, 61-76, (Jun 1998).

We have used Time of Flight Secondary Ion Mass Spectroscopy (TOF-SIMS) in combination with X-ray photoelectron spectroscopy (XPS) to study chemical changes taking place at the surface of pure cellulose paper samples treated in N2 plasma for periods of time up to 60 seconds. High resolution TOF-SIMS spectra permit the detection of various functionalities containing nitrogen, even following very brief (∼2s) plasma exposure. Correlations between chemistry and surface properties, such as water wettability, are presented and discussed.

2312. Glocker, D.A., and M.M. Romach, “Near atmospheric pressure treatment of polymers using helium discharges,” U.S. Patent 5767469, Jun 1998.

The present invention is a method and apparatus for treating a polyester support such as polyethylene napthalate or polyethylene terephthalate. The treatment is carried out at near atmospheric pressure in a gas of helium and nitrogen or oxygen. The treatment uses anodized aluminum electrodes and an atmospheric glow discharge results when the electrodes are connected to an RF generator and spaced about 2 mm apart. The process and apparatus improve adhesion of subsequently coated emulsions on the polyester support.

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

849. Park, S.-C., S.-K. Koh, and K.D. Pae, “Effects of surface modification by Ar+ irradiation on wettability of surfaces of poly(ethylene terephthalate) films,” Polymer Engineering and Science, 38, 1185-1192, (Jul 1998).

Surfaces of poly(ethylene terephthalate); PET, films were irradiated with Ar+ at 1 keV using various ion doses (ID) from 1014 to 1017 ions/cm2 (isc) with and without an O2 environment. The wettability of the modified surfaces of PET was determined by measuring the contact angle between water droplets and the modified surfaces. The modified surfaces were also characterized by AFM (atomic force microscopy) and XPS (X-ray photoelectron spectroscopy) for changes in the surface morphology, and the chemical composition and molecular structure, respectively. The contact angle decreased from 70° for unmodified surfaces to 45° for modified surface with ID = 1014 isc without O2 and remained relatively constant with higher ID. The contact angle, however, reached a minimum value of 8° for modified surfaces with ID = 1016 isc with O2. The improved wettability may be due to a combination of the formation of hydrophilic groups, chemical and molecular structural changes, physical structural or morphological changes, and increased roughness of the surface. The wettability of the modified surfaces also depended on the time of exposure to air. The wettability worsened with exposure time to air, but was revived by immersing the films into water. Possible mechanisms for the change of the wettability of the modified surfaces are given.

1017. Moon, S.I., and J. Jang, “Factors affecting the interfacial adhesion of ultrahigh-modulus polyethylene fibre-vinylester composites using gas plasma treatment,” J. Materials Science, 33, 3419-3425, (Jul 1998).

The interfacial adhesion of ultrahigh-modulus polyethylene (UHMPE) fibre–vinylester composites was improved by the oxygen plasma treatment of the UHMPE fibre. The chemical functional group formations on the UHMPE fibre surface by oxygen plasma treatment were analysed using diffuse reflectance Fourier transform infrared spectroscopy and the morphological changes of the UHMPE fibre surface by plasma etching were observed by scanning electron microscopy. The wettability enhancement by the chemical functional group formation and the mechanical interlocking due to the micropits were important factors in improving the interfacial adhesion of the UHMPE fibre–vinylester composites by oxygen plasma treatment. In order to investigate the relative importance of the two factors, wettability enhancement and mechanical interlocking, in the improved interfacial adhesion of the UHMPE fibre–vinylester composites, nitrogen plasma treatment was also performed. Nitrogen plasma treatment of the UHMPE fibre was proved to be effective in the formation of the micropittings and ineffective in the chemical functional group formation in comparison with the oxygen plasma treatment. The interlaminar shear strengths of the nitrogen-plasma-treated UHMPE fibre–vinylester composites showed almost the same value as those of the oxygen-plasma-treated UHMPE fibre–vinylester composites. The wettability enhancement and mechanical interlocking are important in the improvement of interfacial adhesion of UHMPE fibre–vinylester composites by plasma treatment and mechanical interlocking seems to be more important.

58. Chen, B.-L., “Surface properties of corona treated polyethylene films containing N-(2-hydroxyethyl) erucamide as slip agent for enhanced adhesion of aqueous ink,” TAPPI J., 81, 185-189, (Aug 1998).

119. Garbassi, F., and E. Occhiello, “Surface modification,” in Concise Polymeric Materials Encyclopedia, Salamone, J.C., ed., 1542-1543, CRC Press, Aug 1998.

164. Huang, T., and P. LePoutre, “Effect of basestock surface structure and chemistry on coating holdout and coated paper properties,” TAPPI J., 81, 145-152, (Aug 1998).

Water absorption by the basestock during coating affects coating pickup and coating mass distribution and, thus, the properties of the coated paper. This work presents results of experiments that were designed to separate the effects of two important factors that determine sheet absorbency: hydrophobic sizing and porosity. Bleached kraft handsheets with a broad range of pore size, void fraction, and roughness were sized to different levels with a solution of alkyl ketene dimer (AKD) in non-swelling hexane. A lightweight coated (LWC) basestock was treated similarly. Coating was performed at 762 m/min on a cylindrical laboratory coater. The effect of hydrophobic sizing on coating pickup depended greatly on sheet porosity and roughness. On dense-smooth sheets, sizing resulted in lower coating pickup. On rough sheets, including LWC basestock, the effect of sizing on pickup was concealed by the overwhelming effect of roughness on the metering action. Coating uniformity and holdout were very good on the dense-smooth sheets (although sizing gave a slight reduction) and poor on the porous rough sheets and LWC basestock (sizing had little effect). The results suggest that coating holdout and uniformity are determined mainly by sheet surface structure (porosity and roughness) and not by sizing.

359. Sun, Q.C., D. Zhang, and L.C. Wadsworth, “Corona treatment on polyolefin films,” TAPPI J., 81, 177-183, (Aug 1998).

2102. Paynter, R.W., “XPS studies of the modification of polystyrene and polyethyleneterephthalate surfaces by oxygen and nitrogen plasmas,” Surface and Interface Analysis, 26, 674-681, (Aug 1998).

Polystyrene and polyethyleneterephthalate surfaces were exposed to helium, oxygen/helium and nitrogen/hydrogen plasmas singly and in combination. The treated surfaces were evaluated by water contact-angle measurements and by x-ray photoelectron spectroscopy. It was found that the oxygen and nitrogen tend to graft to common carbon atoms, to form amide groups. The water wettability was found to correlate with the fraction of electronegative atoms incorporated into the surface. © 1998 John Wiley & Sons, Ltd.
https://analyticalsciencejournals.onlinelibrary.wiley.com/doi/abs/10.1002/%28SICI%291096-9918%28199808%2926%3A9%3C674%3A%3AAID-SIA414%3E3.0.CO%3B2-5

477. Cocolios, P., F. Coeuret, A. Villermet, E. Prinz, and F. Forster, “A new high performance, stable surface treatment for plastic films, paper and metal foils,” in 1998 Polymers, Laminations, and Coatings Conference Proceedings, TAPPI Press, Sep 1998.

1027. Kramer, B., and G. Jerdee, “A survey of common process and product parameters designed to improve adhesion of polyethylene,” in 1998 Polymers, Laminations and Coatings Conference Proceedings, 119-125, TAPPI Press, Sep 1998.

1102. Tamm, R.R., “Effect of film additives on printing,” in 1998 Polymers, Laminations and Coatings Conference Proceedings, 1067-1071, TAPPI Press, Sep 1998.

1810. Nickerson, R., “Plasma surface modification for cleaning and adhesion,” in 1998 Polymers, Laminations and Coatings Conference Proceedings, TAPPI Press, Sep 1998.

2755. Jadon, N., and M.D. Nolan, “Exploring the benefits of newly developed adhesion promotion methods,” in 1998 Polymers, Laminations and Coatings Conference Proceedings, 1109-1118, TAPPI Press, Sep 1998.

2760. Campbell, R.N., and D. Wolters, “Improved barrier properties with metallized films from corona process improvements and from copolymer characteristics,” in 1998 Polymers, Coatings and Laminations Conference Proceedings, 385-396, TAPPI Press, Sep 1998 (also in J. Plastic Film and Sheeting, V. 16, p. 108-123, Apr 2000).

Vastly improved film surface tension values were achieved using elevated corona treater roll temperatures in the production of BOPP film with a coextruded skin layer designed for subsequent metallization. These film surface tension values did not significantly decrease with time. A new propylene/butene-1 copolymer was coextruded as the metallizing layer in the BOPP film construction. When metallized, this film provided improved barrier to water vapor transmission by a factor of 5:1 when compared to a similar film produced with a propylene/ethylene copolymer as the metallizing layer. Stringent analysis of the surface of the propylene/butene copolymer revealed that the unique smoothness of its surface enhanced the barrier properties of the film after metallizing. The surface of the ethylene/propylene copolymer was much rougher.

3037. Cheney, G., and R.T.E. Sylvester, “Factors affecting adhesion in the extrusion coating process,” in 1998 Polymers, Laminations and Coatings Conference Proceedings, 1095-1100, TAPPI Press, Sep 1998.

1030. Yamaguchi, M., “Effect of molecular structure in branched polyethylene on adhesion properties with polypropylene,” J. Applied Polymer Science, 70, 457-463, (Oct 1998).

Adhesion properties between branched polyethylene (PE) and isotactic polypropylene (PP) were studied by a peel test and scanning electron microscopy. In this study, two types of branched PEs were used; one is a linear low density polyethylene (LLDPE) and the other is a high pressure low density polyethylene (LDPE). The adhesive strength of the LLDPE/PP is much higher than that of LDPE/PP. Furthermore, the formation of PE influxes between PP spherulites has a small effect on the adhesion. The dynamic viscoelastic measurements for the binary blends composed of branched PE and PP were also carried out to estimate the interfacial tension by using a rheological emulsion model proposed by Palierne. The interfacial tension is 1.0 mN for LLDPE/PP and 2.1 mN for LDPE/PP, suggesting that the interfacial thickness of LLDPE/PP is about twice that of LDPE/PP. The adhesive strength between branched PE and PP will be determined by the interfacial thickness, which represents the entanglements between two polymers. © 1998 John Wiley & Sons, Inc. J. Appl. Polym. Sci. 70: 457–463, 1998
https://onlinelibrary.wiley.com/doi/abs/10.1002/%28SICI%291097-4628%2819981017%2970%3A3%3C457%3A%3AAID-APP5%3E3.0.CO%3B2-M

2482. Wetterman, R.P., “Surface tension measurement and coatings development,” Paint and Coatings Industry, 202-206, (Oct 1998).

191. Kenny, J., “Corona treating,” Label & Narrow Web Industry, 3, 30-35, (Nov 1998).

973. Novak, I., and I. Chodak, “Adhesion of poly(propylene) modified by corona discharge,” Angewandte Makromolekulare Chemie, 260, 47-51, (Nov 1998).

The surface of isotactic poly(propylene) foils was oxidized by corona discharge plasma in order to improve the adhesive characteristics. The dependence of the degree of surface oxidation on either the current density or the time of exposure was determined. Rapid increase of the free surface energy was observed at current densities ranging from 0.4 to 0.6 mA. A reduction of the exposure time of discharge at the foil surface has an effect similar to the reduction of current density. The change of free surface energy of extruded poly(propylene) was rapid, especially during the first 24 h, while for modified biaxially oriented poly(propylene) the decrease of free surface energy was substantially slower.

700. van Oss, C.J., W. Wu, and R.F. Giese, “Lifshitz-van der Waals, Lewis acid-base and electrostatic interactions in adhesion in aqueous media,” in First International Congress on Adhesion Science and Technology: Festschrift in Honor of Dr. K.L. Mittal on the Occasion of his 50th Birthday, W.J. van Ooij and H.R. Anderson Jr., eds., 49-62, VSP, Dec 1998.

Lifshitz-van der Waals (LW) and Lewis acid-base (AB), together with electrostatic (EL) forces are the non-covalent forces acting in adhesion in condensed phase media, such that the work of adhesion, VEadh= WLW+ WAB+ WEL. In the case of serum albumin (SA) and glass surfaces or silica particles, on a macroscopic scale, WEW> 0, WAB< 0 and WEL< 0, so that W'ddh is negative, ie repulsive. Nonetheless, in aqueous media, at neutral pH, SA adheres to glass surfaces, as well as to silica particles. It may be hypothesized that on a microscopic level, negatively charged, electron-donating SA moieties, located on prominent sites with a small radius of curvature, can penetrate the macroscopic repulsion field and bind to electron-accepting cations imbedded in the glass surfaces (Ca ions) or in silica particles (Si ions). The correctness of the hypothesis is supported by the fact that all adhering SA can be desorbed from, say, silica particles with Na2-EDTA. Furthermore, energy vs. distance diagrams demonstrate that the more prominently located SA sites with a small radius of curvature should indeed be able to overcome the macroscopic repulsion field and to adhere locally to microscopic cationic sites in the glass or silica. Thus, energy vs. distance balances of the extended DLVO type (including AB as well as LW and EL forces), combining macroscopic and microscopic interactions, can be used to predict adhesion in complex systems.

701. Dwight, D.W., “Relationships between interfacial acid-base interactions and adhesive bond strength,” in First International Congress on Adhesion Science and Technology: Festschrift in Honor of Dr. K.L. Mittal on the Occasion of his 50th Birthday, W.J. van Ooij and H.R. Anderson, Jr., eds., 63-80, VSP, Dec 1998.

Acid–base interactions across interfaces are shown to have predictable influences on adhesion. The history of this development, and methods to assay the acid–base character of solvents, polymers and a variety of powders and fibers are reviewed briefly. Recent studies are described that demonstrate directly how acid–base interactions influence both ‘fundamental’ and ‘practical’ adhesion.

771. McHale, G., S.M. Rowan, M.I. Newton, and N.A. Kab, “Estimation of contact angles on fibers,” J. Adhesiev Science and Technology, 13, 1457-1469, (1999) (also in Apparent and Microscopic Contact Angles, J. Drelich, J.S. Laskowski, and K.L. Mittal, eds., p. 319-331, VSP, Jun 2000).

403. no author cited, “ASTM D5946: Standard test method for using water contact angle measurements,” ASTM, 1999.

569. McCafferty, E., and J.P. Wightman, “Determination of the acid-base properties of metal oxide films and of polymers by contact angle measurements,” J. Adhesion Science and Technology, 13, 1415-1436, (1999) (also in Apparent and Microscopic Contact Angles, J. Drelich, J.S. Laskowski, and K.L. Mittal, eds., p. 149-170, VSP, Jun 2000).

770. Neimark, A.V., “Thermodynamic equilibrium and stability of liquid films and droplets on fibers,” J. Adhesion Science and Technology, 13, 1137-1154, (1999) (also in Apparent and Microscopic Contact Angles, J. Drelich, J.S. Laskowski, and K.L. Mittal, eds., p. 301-318, VSP, Jun 2000).

967. Zenkiewicz, M., and J. Golebiewski, “Use of photoelectron spectroscopy in studies of the depth profile of polypropylene film,” Polimery, 44, 246-254, (1999).

 

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