2018
DOI: 10.1002/ppap.201800021
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Atomic oxygen and hydrogen loss coefficient on functionalized polyethylene terephthalate, polystyrene, and polytetrafluoroethylene polymers

Abstract: Coefficients for atomic loss of hydrogen and oxygen atoms on polyethylene terephthalate (PET), polystyrene (PS), and polytetrafluoroethylene (PTFE) are determined. Measurements are performed in a flowing afterglow with different atom densities between 6 and 60 × 1020 m−3 and in the pressure range between 8 and 200 Pa. The loss coefficients do not depend significantly on the atom density or pressure. For H atoms they are (2.3 ± 0.4) × 10−3, (1.5 ± 0.4) × 10−3, and (8.0 ± 3.0) × 10−4 for PET, PS, and PTFE, respe… Show more

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Cited by 13 publications
(7 citation statements)
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“…The surface loss coefficient for such materials approaches unity because the atoms become trapped in pores where they experience many collisions with the surface, so they are likely to recombine to parent molecules before they can escape from the surface to the gas phase. The loss coefficient for polymers is typically between 10 −3 and 10 −2 at room temperature (see [30] and references thereafter), but little work has been performed on the evaluation of the loss rate at elevated temperatures. The loss coefficients on surfaces facing an active plasma may also increase by the fluxes of positive ions and UV and/or VUV radiation [23].…”
Section: Specificities Of Low-pressure Plasmasmentioning
confidence: 99%
“…The surface loss coefficient for such materials approaches unity because the atoms become trapped in pores where they experience many collisions with the surface, so they are likely to recombine to parent molecules before they can escape from the surface to the gas phase. The loss coefficient for polymers is typically between 10 −3 and 10 −2 at room temperature (see [30] and references thereafter), but little work has been performed on the evaluation of the loss rate at elevated temperatures. The loss coefficients on surfaces facing an active plasma may also increase by the fluxes of positive ions and UV and/or VUV radiation [23].…”
Section: Specificities Of Low-pressure Plasmasmentioning
confidence: 99%
“…The factor γ in Equation (2) is the coefficient for heterogeneous surface recombination of atoms on the polymer surface, and W D /2 is half of the dissociation energy of the parent molecule. The dissociation energy for oxygen molecules is 5.2 eV, and the probability for heterogeneous surface recombination on a smooth polymer surface is around 10 −3 [ 16 ].…”
Section: Theoretical Limitationsmentioning
confidence: 99%
“…Extensive recombination also appeared on the path between plasma and the RGA-this connection was narrow, thus numerous collisions of gaseous species with the surface of the steel tube appeared. The recombination coefficients for polymeric materials were rather low [23], but for H atoms on stainless steel, the probability of surface recombination was close to 0.1 [24]; thus, very few H atoms created in plasma could enter the RGA. As a result, the H 2 signal prevails in Figure 4.…”
Section: Resultsmentioning
confidence: 95%