ACCU DYNE TEST ™ Bibliography
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2288. Gao, L., and T.J. McCarthy, “Wetting 101,” Langmuir, 25, 14105-14115, (2009).
We review our 2006−2009 publications on wetting and superhydrophobicity in a manner designed to serve as a useful primer for those who would like to use the concepts of this field. We demonstrate that the 1D (three-phase, solid/liquid/vapor) contact line perspective is simpler, more intuitive, more useful, and more consistent with facts than the disproved but widely held-to-be-correct 2D view. We give an explanation of what we believe to be the reason that the existing theoretical understanding is wrong and argue that the teaching of surface science over the last century has led generations of students and scientists to a misunderstanding of the wetting of solids by liquids. We review our analyses of the phenomena of contact angle hysteresis, the lotus effect, and perfect hydrophobicity and suggest that needlessly complex theoretical understandings, incorrect models, and ill-defined terminology are not useful and can be destructive.
2287. Gao, L., and T.J. McCarthy, “An attempt to correct the faulty intuition perpetuated by the Wenzel and Cassie 'laws',” Langmuir, 25, 7249-7255, (2009).
We respond to a recent report in this journal that criticizes our experiments, which disproved the Wenzel and Cassie theories. The criticism is that we measured contact angles “with drops that were too small, ignoring the indications of existing theoretical understanding.” We take a step back to give an explanation of what we believe to be the reason that the “existing theoretical understanding” is wrong. We explain that the teaching of surface science has led generations of students and scientists to a misunderstanding of the wetting of solids by liquids. This continues as evidenced by this recent criticism and numerous recent papers. We describe several demonstrations that were designed to help teachers, students, and scientists overcome the widespread learning disability that is rooted in their faulty intuition and to help them regard wetting from the perspective of lines and not areas.
2176. Wolf, R.A., and A.C. Sparavigna, “Measuring surface features II: Electrons for chemical analysis,” Converter: Flessibili, Carta, Cartone, 78, 100-108, (2009).
2175. Wolf, R.A., and A.C. Sparavigna, “Measuring surface features I: Surface tension analysis,” Converter: Flessibili, Carta, Cartone, 77, 60-68, (2009).
2166. Bialopiotrowicz, T., “Influence of erroneous data on the results of calculations from acid-base surface free energy theories, III: Solution of a three-equation set in the case of homoscedastic error,” J. Adhesion Science and Technology, 23, 799-813, (2009).
The van Oss–Chaudhury–Good theory (vOCGT) was checked for a large artificial set of work of adhesion input data calculated for 15 solids and 300 liquids. Numerical values of LW component and acid (A) and base (B) parameters were assigned to 15 solids. These 15 solids were grouped in 5 sets of 3 solids in each. Also numerical values of LW component and A and B parameters were assigned to 300 liquids (three sets of 100 liquids in each). Data for these solids and liquids were especially selected to represent real types of materials encountered in practice. For all 15 solids and 300 liquids the work of adhesion values were calculated and these values were assumed to be error-free. Next, new values of the work of adhesion were obtained by adding a random homoscedastic error (A vector of random variables is homoscedastic if it has the same finite variance.) of the normal distribution (Also called the Gaussian distribution — it is continuous probability distribution defined by two parameters: the mean and variance (standard deviation squared, σ2).), belonging to 8 distributions of a mean value equal to the error-free work of adhesion value and standard deviations of 0.5, 1, 2, 5, 7, 10, 15 and 20 mJ/m2. The LW components and A and B parameters for these solids were back-calculated for each error level. Two different methods for the solution of a 3-equation set were used and they gave practically the same results irrespective of the error level and liquids and solids used. It was found that there existed a linear correlation between the RMSE (root mean square error) of the solution and the standard deviation of the work of adhesion data. This correlation was highly significant (with a correlation coefficient higher than 0.999) and was true separately for LW component, A and B parameters as well as for the total solution vector (i.e., combinedly for the LW component, A and B parameters). The RMSE values of the total solution vector (having as elements values of the LW component, A and B parameters) as well as separately for LW component and A and B parameters were correlated with the condition number of a given 3-equation set. A very good correlation was found only for the total solution, much worse for A or B parameters, and practically there was a lack of correlation for the LW component. Based on the correlation between the RMSE and the standard deviation of the work of adhesion it was possible to determine what should have been the maximal standard deviation of the work of adhesion if the calculated value of a given LW component or A or B parameter did not differ by more than 1 mJ/m2 from an error-free (true) value.
3034. Bahners, T., G. Hoffmann, J. Nagel, E. Schollmeyer, and A. Voigt, “The effect of plasma pre-treatment on the quality of flock coatings on polymer substrates,” in Contact Angle, Wettability and Adhesion, Vol. 6, K.L. Mittal, ed., 325-340, VSP, 2009.
Flock coating is a widely used process to create a textile-like texture on substrates of various shapes and materials. In the process, flock fibers—short fibers typically 1–3 mm long—are oriented and accelerated towards the substrate by means of an electric field. Impacting fibers are stuck to the substrate surface by an appropriate adhesive. Primary quality criteria are adhesion of the flock fibers to the adhesive, and also the so-called flock density, ie number of fibers per unit area, and evenness. The influential physical and chemical factors refer to interfacial adhesion, but also charging effects by the impacting fibers. The system presently under investigation is based on aliphatic polyamides as material for a molded car component, hot-melt adhesive, and flock fibers. Experiments reported here refer to the application of an air plasma pretreatment of the polyamide (PA) substrate, mainly in order to increase the adhesion of the hot-melt layer. It was found that the plasma treatment affects the polar energy of the PA surface with a related increase in wettability due to a reduction of C–C and C–H bonds and an increase of carboxylic groups. Surface carbonization occurred at higher plasma doses. The effect on hot-melt adhesion was rather small, however two types of failures were observed in these experiments, either due to insufficient adhesion of the hot-melt or due to a break of one of the PA plates with the bond still intact. The characterization of flock coatings on these samples showed no effect on flock fiber adhesion in pull-out as well as on abrasion resistance, but an increased flock density was observed. This is assumed to be due to enhanced dissipation of charges by the conductive water layer adsorbed on the substrate surface.
3033. Chibowski, E., and K. Terpilowski, “Comparison of apparent surface free energy of some solids determined by different approaches,” in Contact Angle, Wettability and Adhesion, Vol. 6, K.L. Mittal, ed., 283-300, VSP, 2009.
Four different approaches to determination of solid surface free energy (van Osset al.’s (LWAB), Owens and Wendt’s (O–W), Chibowski’s contact angle hysteresis (CAH) and Neumann’s equation of state (EQS)) were examined on glass, silicon, mica and poly (methyl methacrylate)(PMMA) surfaces via measurements of advancing and receding contact angles. Sessile drop and tilted plate methods were employed to measure the contact angles of probe liquids water, formamide and diiodomethane. The results obtained show that on a given solid the advancing contact angle is slightly larger and the receding one smaller if measured by tilted plate method. Hence, the resulting hysteresis is larger than that from the contact angles measured by sessile drop. The calculated (apparent) surface free energy is the greatest if determined from O–W equation. Unexpectedly, EQS fails for weakly polar polymer PMMA surface, giving significantly lower value of the calculated energy. In rest of the tested systems LWAB, CAH and EQS approaches give comparable results for the apparent surface free energy of the tested solids. A hypothesis is put forward that using a probe liquid only apparent surface free energy of a solid can be determined because the strength of interactions originating from the solid surface depends on the strength of interactions coming from the probe liquid surface.
3032. Salapare III, H.S., G.Q. Blantocas, .R. Noguera, and H. J. Ramos, “The porosity and wettability properties of hydrogen ion treated poly(tetrafluoroethylene),” in Contact Angle, Wettability and Adhesion, Vol.6, K.L. Mittal, ed., 207-218, VSP, 2009.
The porosity and wettability properties of hydrogen ion treated poly(tetrafluoroethylene) (PTFE) materials are related using contact angle, scanning electron microscopy (SEM) and ellipsometry techniques. PTFE samples are irradiated using a low-energy hydrogen ion shower (LEHIS) produced by a Gas Discharge Ion Source (GDIS). The plasma discharge current (Id) is varied at intervals of 1 mA. Results show that treatment using lower Id improved the hydrophobic property of the PTFE material with water contact angle increasing from 102◦ to 119◦. It also becomes less porous as indicated by the increase in the index of refraction, decrease in optical transmittance, and increased fissures and striations in the SEM images. Opposite effects are observed for higher Id.
3031. Extrand, C.W., “Work of wetting associated with spreading of sessile drops,” in Contact Angle, Wettability and Adhesion, Vol. 6, K.L. Mittal, ed., 81-94, VSP, 2009.
In this theoretical study, the work done on a sessile drop during spreading was estimated. It was found that the energy required to stretch the contact line is much greater than the energy needed to stretch the air–liquid interfacial area. The model shows that wetting energies are relatively small for large contact angles, but increase dramatically as contact angles tend towards zero. For a given drop volume, more work is needed to spread higher surface tension liquids than lower surface tension ones. Similarly, larger drops require more energy to spread than smaller ones. The work of wetting estimated here for sessile drops is comparable to energies from other wetting geometries, such as capillary bridge and sphere tensiometry. This work provides theoretical support for the experimental observation that interactions at the contact line dominate the wetting behavior of spreading sessile drops.
3075. Ren, C.-S., K. Wang, Q.-Y. Nie, D.-Z. Wang, and S.-H. Guo, “Surface modification of PE film by DBD plasma in air,” Applied Surface Science, 255, 3421-3425, (Dec 2008).
In this paper, surface modification of polyethylene (PE) films is studied by dielectric barrier discharge plasma treatment in air. The treated samples were examined by water contact angle measurement, calculation of surface free energy, Fourier transform infrared attenuated total reflection spectroscopy (FTIR-ATR), X-ray photoelectron spectroscopy (XPS) and scanning electron microscopy (SEM). The water contact angle changes from the original value of 93.2° to the minimum value of 53.3° and surface free energy increases from 27.3 to 51.89 J/m2 after treatment time of 50 s. Both ATR and XPS show some oxidized species are introduced into the sample surface by the plasma treatment and that the change tendencies of the water contact angle and surface free energy with the treatment time are the same as that of the oxygen concentration on the treated sample surface. Cu films were deposited on the treated and untreated PE surfaces. The peel adhesive strength between the Cu film and the treated sample is 1.5 MPa, whereas the value is only 0.8 MPa between the Cu film and the untreated PE. SEM pictures show that the Cu film deposited on the plasma treated PE surface is smooth and the crystal grain is smaller, contrarily the Cu film on the untreated PE surface is rough and the crystal grain is larger.
2829. Alexander, C.S., M.C. Branch, M. Strobel, M. Ulsh, N. Sullivan, and T.Vian, “Application of ribbon burners to the flame treatment of polypropylene films,” Progress in Energy and Combustion Science, 34, 696-713, (Dec 2008).
This article focuses on recent advances in the understanding of industrial gas burners. Ribbon burners have been chosen as the focus of the review because of the advantages presented by the burner arrangement and burner performance. The ribbon burner configuration, because of its ability to provide large flame surface and flame stabilization, has a large range of stability as flow rate, equivalence ratio and reactant gas composition are varied. Discussed in detail is the application of ribbon burners in the surface modification, or flame treatment, of polymer films to increase the wettability of a polymer surface. Optimum treatment requires a spatially homogeneous post-flame reaction zone even with burners up to 3 m in length. For methane/air flames, the optimum equivalence ratio is near 0.93 where the active oxidizing-species concentration near the surface is a maximum. Chemical kinetic models of the impinging flame and surface oxidation chemistry of a polymer film are also discussed. The model predictions are in good qualitative agreement with the available understanding of the flame variables affecting surface treatment and the expected oxidized species on the polymer surface.
2555. Pykonen, M., H. Sundqvist, J. Jarnstrom, O.-V. Kaukoniemi, and M. Tuominen, “Effects of atmospheric plasma activation on surface properties of pigment-coated and surface-sized papers,” Applied Surface Science, 255, 3217-3229, (Dec 2008).
Pigment-coated, surface-sized, and surface-sized copy papers were treated with conventional corona, experimental pilot-scale plasma and laboratory-scale plasma. All the treatments increased the surface energy and oxidized the surface. The changes in the surface chemistry depended on treatment time and composition of the substrate surface. It seems that plasma especially oxidizes the long polymer chains, such as surfactants and other paper chemicals, on the surface of the paper. The ToF-SIMS distribution maps indicated that the pilot-scale treatment led to an uneven CO+ group distribution, whereas laboratory scale treatment gave a more even distribution of CO+ groups. In addition to chemical changes, topographical changes due to plasma treatment were detected. The RMS roughness increased for pigment-coated paper, whereas plasma treatment induced small nodules between the paper pigment particles with pigmented and surface-sized paper. The increase in roughness was also found to increase the wettability. This serves as a demonstration of roughness-induced increase of surface energy of the samples.
2551. Pappas, D.D., A.A. Bujanda, J.A. Orlicki, and R.E. Jensen, “Chemical and morphological modification of polymers under a helium-oxygen dielectric barrier discharge,” Surface and Coatings Technology, 203, 830-834, (Dec 2008).
In this work, the surface modifications of various polymer films due to helium–oxygen dielectric barrier discharge (DBD) exposure operating under atmospheric pressure are reported. The polymer films studied include ultra high molecular weight polyethylene, polyamide, polytetrafluoroethylene and polyimide. Experimental results reveal increased hydrophilicity and surface energy of the plasma exposed polymers. This is attributed to the presence of oxygen containing groups grafted onto the surface during plasma treatment, as confirmed by X-ray photoelectron spectroscopy (XPS) analysis. Scanning electron microscopy (SEM) data show the appearance of micro depressions, the size of which depends on the chemical structure and the treatment time, suggesting that mild etching occurs in a predicted fashion. Most importantly, this uniform modification occurs within a few seconds of exposure, time comparable to continuous on-line industrial processing.
2172. Bishop, C.A., “Optimising plasma treatment,” http://vacuumcoatingblog.co.uk/2008/12/optimizing-plasma-treatment.html, Dec 2008.
1921. Dillingham, R.G., B.R. Oakley, and D. Gilpin, “Wetting measurements for identification of specific functional groups responsible for adhesion,” J. Adhesion, 84, 1007-1022, (Dec 2008).
The relationship between adhesion and surface energy is well established for systems where specific chemical interactions are unlikely, such as pressure sensitive adhesives. However, the relationship of wetting to adhesion in chemically reactive systems is not well understood. This work used atmospheric pressure plasma treatment in air of high density polyethylene to obtain surfaces with a range of electron donor and acceptor character prior to bonding with an amine cured epoxy. Adhesion correlated strongly with the electron donating character of surface energy, and the likely functional groups responsible for this adhesion were amines created by the plasma treatment process. These results indicate that wetting measurements may be useful in detecting the specific chemical interactions important to adhesion in reactive systems.
1890. Leroux, F., C. Compagne, A. Perwuelz, and L. Gengembre, “Polypropylene film chemical and physical modifications by dielectric barrier discharge plasma treatment at atmospheric pressure,” J. Colloid and Interface Science, 328, 412-420, (Dec 2008).
Dielectric barrier discharge (DBD) technologies have been used to treat a polypropylene film. Various parameters such as treatment speed or electrical power were changed in order to determine the treatment power impact at the polypropylene surface. Indeed, all the treatments were performed using ambient air as gas to oxidize the polypropylene surface. This oxidation level and the surface modifications during the ageing were studied by a wetting method and by X-ray photoelectron spectroscopy (XPS). Moreover polypropylene film surface topography was analyzed by atomic force microscopy (AFM) in order to observe the surface roughness modifications. These topographic modifications were correlated to the surface oxidation by measuring with a lateral force microscope (LFM) the surface heterogeneity. The low ageing effects and the surface reorganization are discussed.
2531. Vesel, A., I. Junkar, U. Cvelbar, J. Kovac, and M. Mozetic, “Surface modification of polyester by oxygen- and nitrogen-plasma treatment,” Surface and Interface Analysis, 40, 1444-1453, (Nov 2008).
In this paper, we present a study on the surface modification of polyethyleneterephthalate (PET) polymer by plasma treatment. The samples were treated by nitrogen and oxygen plasma for different time periods between 3 and 90 s. The plasma was created by a radio frequency (RF) generator. The gas pressure was fixed at 75 Pa and the discharge power was set to 200 W. The samples were treated in the glow region, where the electrons temperature was about 4 eV, the positive ions density was about 2 × 1015 m−3, and the neutral atom density was about 4 × 1021 m−3 for oxygen and 1 × 1021 m−3 for nitrogen. The changes in surface morphology were observed by using atomic force microscopy (AFM). Surface wettability was determined by water contact angle measurements while the chemical composition of the surface was analyzed using XPS. The stability of functional groups on the polymer surface treated with plasma was monitored by XPS and wettability measurements in different time intervals. The oxygen-plasma-treated samples showed much more pronounced changes in the surface topography compared to those treated by nitrogen plasma. The contact angle of a water drop decreased from 75° for the untreated sample to 20° for oxygen and 25° for nitrogen-plasma-treated samples for 3 s. It kept decreasing with treatment time for both plasmas and reached about 10° for nitrogen plasma after 1 min of plasma treatment. For oxygen plasma, however, the contact angle kept decreasing even after a minute of plasma treatment and eventually fell below a few degrees. We found that the water contact angle increased linearly with the O/C ratio or N/C ratio in the case of oxygen or nitrogen plasma, respectively. Ageing effects of the plasma-treated surface were more pronounced in the first 3 days; however, the surface hydrophilicity was rather stable later. Copyright © 2008 John Wiley & Sons, Ltd.
2226. Gatenby, A., “CSC Scientific blog: Surface tension and interfacial tension,” http://www.cscscientific.com/csc-cientific-blog/bid/25530/, Nov 2008.
2163. Muller, M., and C. Oehr, “Surface tensions of polymers,” http://www.igb.fraunhofer.de/www/gf/grenzflmem/gf-physik/en/GFphys-PolymOberfl, Nov 2008.
1730. Klein, K., “Efficient corona treating saves time and energy,” Flexible Packaging, 10, 26, (Nov 2008).
2503. Bismarck, A., W. Brostow, R. Chiu, H.E.H. Lobland, and K.K.C. Ho, “Effects of surface plasma treatment on tribology of thermoplastic polymers,” Polymer Engineering & Science, 48, 1971-1976, (Oct 2008).
We have subjected polycarbonate (PC), low density polyethylene (LDPE), polystyrene (PS), polypropylene (PP), and Hytrel® (HY, a thermoplastic elastomer) to atmospheric pressure oxygen plasma treatment for varying amounts of time. Effects of the treatment have been evaluated in terms of the water wetting angle, dynamic friction, scratch resistance, and sliding wear. Although PS, PP, and HY do not undergo significant tribological changes as a result of the interaction with plasma, PC and LDPE show more pronounced and useful effects, such as a lowering of dynamic friction in PC and wear reduction in LDPE. These results can be explained in terms of the changes in chemical structures and increase of hydrophilicity. Based on the effects of oxygen plasma treatment on PC and LDPE, these two polymers have been subjected to longer oxygen plasma treatments and to argon, nitrogen, and air plasmas. Resulting effects on friction and scratch resistance are compared to determine the mechanisms responsible for the various surface behaviors. Chemical surface modification—as represented by changing contact angles—contributes to the tribological responses. POLYM. ENG. SCI., 2008. © 2008 Society of Plastics Engineers
2171. Bishop, C.A., “A problem of poor adhesion,” http://www.vacuumcoatingblog.co.uk/blog/2008/10/a-problem-of-po, Oct 2008.
1740. Varella, R., “Business strategies: Surface treatments,” Plastics Decorating, 30-32, (Oct 2008).
1720. Bodine, J., “Overtreatment of PET: Fact or fiction,” in AIMCAL 2008 Fall Technical Conference, AIMCAL, Oct 2008.
2569. Bodine, J., “Over-treatment of PET - fact or fiction (part 1): A study of the following variables: watt density, corona dwell time, film selection, dyne level and water soak bond strength,” in 2008 PLACE Conference Proceedings, 794-801, TAPPI Press, Sep 2008.
2568. Lahti, J., M. Tuominen, and J. Kuusipalo, “The influence of atmospheric plasma treatment on digital print quality of extrusion coated paper,” in 2008 PLACE Conference Proceedings, 767-778, TAPPI Press, Sep 2008.
2567. Mandolini, P., “Polarized flame treatment for BOPP and CPP films and comparison with other treatment methods,” in 2008 PLACE Conference Proceedings, 710-714, TAPPI Press, Sep 2008.
2566. Cushing, G., “Balancing adhesion and slip properties in aqueous heat seal coatings,” in 2008 PLACE Conference Proceedings, 53-60, TAPPI Press, Sep 2008.
2273. Joshi, R., R.-D. Schulze, A. Meyer-Plath, and J.F. Friedrich, “Selective surface modification of poly(propylene) with OH and COOH groups using liquid-plasma systems,” Plasma Processes and Polymers, 5, 695-707, (Sep 2008).
Underwater plasma and glow discharge electrolysis are interesting new methods for polymer surface functionalization. The achievable content of O-containing functional groups exceeds that of oxygen glow discharge gas plasmas by a factor of two (up to ca. 56 O/100 C). The percentage of OH groups among all O-containing groups can reach 25 to 40%, whereas it is about 10% in the gas plasmas. Addition of hydrogen peroxide increases the fraction of OH groups to at most 70% (27 OH/100 C). The liquid plasma systems are also able to polymerize acrylic acid and deposit the polymer as very thin film on substrate surfaces or membranes, thereby retaining about 80% of all COOH functional groups (27 COOH/100 C).
2571. Schubert, G., “Adhesion to foil: More than just a one-sided story,” in 2008 PLACE Conference Proceedings, 1123-1152, TAPPI Press, Sep 2008.
2557. Quere, D., “Wetting and roughness,” Annual Review of Materials Research, 38, 71-99, (Aug 2008).
We discuss in this review how the roughness of a solid impacts its wettability. We see in particular that both the apparent contact angle and the contact angle hysteresis can be dramatically affected by the presence of roughness. Owing to the development of refined methods for setting very well-controlled micro- or nanotextures on a solid, these effects are being exploited to induce novel wetting properties, such as spontaneous filmification, superhydrophobicity, superoleophobicity, and interfacial slip, that could not be achieved without roughness.
2988. Pascual, M., R. Balart, L. Sanchez, O. Fenollar, and O. Calvo, “Study of the aging process of corona discharge plasma effects on low density polyethylene film surface,” J. Materials Science, 43, 4901-4908, (Jul 2008).
A study of the durability of corona discharge plasma effects on a polymer surface was investigated in this work. We used the corona discharge plasma technique to modify the wettability properties of low density polyethylene (LDPE) film and evaluated the influence of relative humidity and temperature on the aging process with three different storage conditions. The effects of the aging process on the plasma-treated surface of LDPE film were quantified by contact angle measurements, Fourier-transformed infrared spectroscopy, and X-ray photoelectron spectroscopy. The results obtained with these techniques have allowed us to determine how the aging process promotes changes in the plasma-treated surface by decreasing its wettability and taking place a remarkable hydrophobic recovery process.
2901. Xiu, Y., L. Zhu, D.W. Hess, and C.P. Wong, “Relationship between work of adhesion and contact angle hysteresis on superhydrophobic surfaces,” J. Physical Chemistry, 112, 11403-11407, (Jul 2008).
Low contact angle hysteresis is an important characteristic of superhydrophobic surfaces for nonstick applications involving the exposure of these surfaces to water or dust particles. In this article, a relationship is derived between the surface work of adhesion and the dynamic contact angle hysteresis, and the resulting predictions are compared with experimental data. Superhydrophobic surfaces with different contact angles and contact angle hysteresis were prepared by generating silicon pillars with varying pillar size and pitch. Surfaces were subsequently treated with fluoroalkyl silanes to modify further the hydrophobicity. The three-phase contact line established for such systems was related to the Laplace pressure needed to maintain a stable superhydrophobic state.
2675. Argent, D., “Dyne levels part 2,” http://www.pffc-online.com/surface-prep/corona-flame-plasma/6338-dyne-..., Jul 2008.
2537. Dubreuil, M.F., and E.M. Bongaers, “Use of atmospheric pressure plasma technology for durable hydrophilicity enhancement of polymeric substrates,” Surface and Coatings Technology, 202, 5036-5042, (Jul 2008).
Parallel plates dielectric barrier discharge (DBD) at atmospheric pressure has been investigated to modify and functionalize the surface of different polymer substrates, e.g. polyolefins, poly(ethylene terephtalate), polyamide, in order to enhance their hydrophilic properties. Surface properties have been altered to meet the requirements of specific applications by introducing the appropriate functionalities through the use of either acetic acid or ethyl acetate. The coatings have been characterized through wettability measurements, labeling coupled with X-Ray photoelectron spectroscopy, and IR spectroscopy.
2170. Bishop, C.A., “Lifetime of surface treatment,” http://www.vacuumcoatingblog.co.uk/blog/2008/07/lifetime-of-sur, Jul 2008.
2169. Bishop, C.A., “Question re backsurface treatment & starry film,” http://www.vacuumcoatingblog.co.uk/blog/2008/07/questions-re-ba.html, Jul 2008.
1708. Bishop, C.A., “Question re plasma treatment: Effect of distance of plasma target plates and substrate surface, and possibility of back treatment during plasma treatment,” http://www.vacuumcoatingblog.com, Jul 2008.
2674. Argent, D., “Dyne levels part 1,” http://www.pffc-online.com/process-management/6240-dyne-levels-part-1-0608, Jun 2008.
1922. Guild, F.J., M.D. Green, R. Stewart, and V. Goodship, “Air plasma pre-treatment for polypropylene automotive bumpers,” J. Adhesion, 84, 530-542, (Jun 2008).
The effect of forced air-plasma pre-treatment, Lectro-treat (TM), on polypropylene has been investigated using X-ray photoelectron spectroscopy (XPS), angle-resolved XPS (AR-XPS), and atomic force microscopy (AFM). The pre-treatment process is found to induce both surface chemistry changes and topographical changes. The parameters of the pre-treatment process can be optimised from these observations. The Lectro-treat pre-treatment process has been used for adhesive bonding of a demonstrator component: a bumper assembly. The adhesively bonded bumpers performed successfully in standard automotive tests.
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