Surface molecular aggregation structure and surface molecular motions of high-molecular-weight polystyrene/low-molecular-weight poly(methyl methacrylate) blend films

Keiji Tanaka, Atsushi Takahara, Tisato Kajiyama

研究成果: ジャーナルへの寄稿記事

103 引用 (Scopus)

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Surface molecular aggregation structure and surface molecular motions of high-molecular-weight polystyrene/low-molecular-weight poly(methyl methacrylate) (HMW-PS/LMW-PMMA) blend films were investigated on the basis of X-ray photoelectron spectroscopic measurements and scanning force microscopic observations. Monodisperse PS with Mn = 1450k, where Mn denotes the number-average molecular-weight, and monodisperse PMMAs with Mn 1.2k, 4.2k, 40.5k, 144k, and 387k were used as HMW-PS and LMW-PMMAs, respectively. Static contact angle measurements revealed that the magnitudes of surface free energy, γ, of PMMAs for all Mns studied here were higher than that of PS with Mn = 1450K. In the case of the (HMW-PS/LMW-PMMA) blend films, in which the Mn for each PMMA was less than 144K, PMMA was preferentially segregated at the air-polymer interface, even though PMMA had a main chain with a higher γ compared with that of PS. It was found from scanning viscoelasticity microscopic measurements that the surface molecular motion of the (PS with Mn = 1450k/ PMMA with Mn = 4.2k) blend film was fairly activated in comparison with that of the bulk one due to the surface segregation of LMW-PMMA. The surface enrichment of LMW-PMMA can be explained by enthalpic and entropie terms as follows. (1) Since the magnitudes of γ of both chain end groups of a polymer chain synthesized by an ordinary living anionic polymerization are smaller than that of the main chain part, the chain end groups are preferentially segregated at the surface. Therefore, the chain end effect at the air-polymer interface becomes more remarkable with a decrease of Mn, due to an increases in the number density of chain end groups. (2) Since polymeric chains existing in a surface region are compressed along the direction perpendicular to the film surface, the surface chains take smaller conformational entropy in a confined state compared with that of bulk chains. The difference in conformational entropy between the surface chain and the bulk one, that is, the conformational entropic penalty of the polymeric chain at the surface, decreases with a decrease in Mn. Then, when the enthalpic and entropic effects mentioned above overcome the γ difference of main chain parts between PS and PMMA, PMMA with higher γ is stably enriched at the blend film surface.

元の言語英語
ページ(範囲)863-869
ページ数7
ジャーナルMacromolecules
31
発行部数3
DOI
出版物ステータス出版済み - 2 10 1998

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Polystyrenes
Polymethyl Methacrylate
Polymethyl methacrylates
Agglomeration
Molecular weight
Polymers
Entropy
Scanning
Surface segregation
Living polymerization
Anionic polymerization
Viscoelasticity
Angle measurement
Photoelectrons
Air
Free energy
Contact angle

All Science Journal Classification (ASJC) codes

  • Organic Chemistry
  • Polymers and Plastics
  • Inorganic Chemistry
  • Materials Chemistry

これを引用

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title = "Surface molecular aggregation structure and surface molecular motions of high-molecular-weight polystyrene/low-molecular-weight poly(methyl methacrylate) blend films",
abstract = "Surface molecular aggregation structure and surface molecular motions of high-molecular-weight polystyrene/low-molecular-weight poly(methyl methacrylate) (HMW-PS/LMW-PMMA) blend films were investigated on the basis of X-ray photoelectron spectroscopic measurements and scanning force microscopic observations. Monodisperse PS with Mn = 1450k, where Mn denotes the number-average molecular-weight, and monodisperse PMMAs with Mn 1.2k, 4.2k, 40.5k, 144k, and 387k were used as HMW-PS and LMW-PMMAs, respectively. Static contact angle measurements revealed that the magnitudes of surface free energy, γ, of PMMAs for all Mns studied here were higher than that of PS with Mn = 1450K. In the case of the (HMW-PS/LMW-PMMA) blend films, in which the Mn for each PMMA was less than 144K, PMMA was preferentially segregated at the air-polymer interface, even though PMMA had a main chain with a higher γ compared with that of PS. It was found from scanning viscoelasticity microscopic measurements that the surface molecular motion of the (PS with Mn = 1450k/ PMMA with Mn = 4.2k) blend film was fairly activated in comparison with that of the bulk one due to the surface segregation of LMW-PMMA. The surface enrichment of LMW-PMMA can be explained by enthalpic and entropie terms as follows. (1) Since the magnitudes of γ of both chain end groups of a polymer chain synthesized by an ordinary living anionic polymerization are smaller than that of the main chain part, the chain end groups are preferentially segregated at the surface. Therefore, the chain end effect at the air-polymer interface becomes more remarkable with a decrease of Mn, due to an increases in the number density of chain end groups. (2) Since polymeric chains existing in a surface region are compressed along the direction perpendicular to the film surface, the surface chains take smaller conformational entropy in a confined state compared with that of bulk chains. The difference in conformational entropy between the surface chain and the bulk one, that is, the conformational entropic penalty of the polymeric chain at the surface, decreases with a decrease in Mn. Then, when the enthalpic and entropic effects mentioned above overcome the γ difference of main chain parts between PS and PMMA, PMMA with higher γ is stably enriched at the blend film surface.",
author = "Keiji Tanaka and Atsushi Takahara and Tisato Kajiyama",
year = "1998",
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T1 - Surface molecular aggregation structure and surface molecular motions of high-molecular-weight polystyrene/low-molecular-weight poly(methyl methacrylate) blend films

AU - Tanaka, Keiji

AU - Takahara, Atsushi

AU - Kajiyama, Tisato

PY - 1998/2/10

Y1 - 1998/2/10

N2 - Surface molecular aggregation structure and surface molecular motions of high-molecular-weight polystyrene/low-molecular-weight poly(methyl methacrylate) (HMW-PS/LMW-PMMA) blend films were investigated on the basis of X-ray photoelectron spectroscopic measurements and scanning force microscopic observations. Monodisperse PS with Mn = 1450k, where Mn denotes the number-average molecular-weight, and monodisperse PMMAs with Mn 1.2k, 4.2k, 40.5k, 144k, and 387k were used as HMW-PS and LMW-PMMAs, respectively. Static contact angle measurements revealed that the magnitudes of surface free energy, γ, of PMMAs for all Mns studied here were higher than that of PS with Mn = 1450K. In the case of the (HMW-PS/LMW-PMMA) blend films, in which the Mn for each PMMA was less than 144K, PMMA was preferentially segregated at the air-polymer interface, even though PMMA had a main chain with a higher γ compared with that of PS. It was found from scanning viscoelasticity microscopic measurements that the surface molecular motion of the (PS with Mn = 1450k/ PMMA with Mn = 4.2k) blend film was fairly activated in comparison with that of the bulk one due to the surface segregation of LMW-PMMA. The surface enrichment of LMW-PMMA can be explained by enthalpic and entropie terms as follows. (1) Since the magnitudes of γ of both chain end groups of a polymer chain synthesized by an ordinary living anionic polymerization are smaller than that of the main chain part, the chain end groups are preferentially segregated at the surface. Therefore, the chain end effect at the air-polymer interface becomes more remarkable with a decrease of Mn, due to an increases in the number density of chain end groups. (2) Since polymeric chains existing in a surface region are compressed along the direction perpendicular to the film surface, the surface chains take smaller conformational entropy in a confined state compared with that of bulk chains. The difference in conformational entropy between the surface chain and the bulk one, that is, the conformational entropic penalty of the polymeric chain at the surface, decreases with a decrease in Mn. Then, when the enthalpic and entropic effects mentioned above overcome the γ difference of main chain parts between PS and PMMA, PMMA with higher γ is stably enriched at the blend film surface.

AB - Surface molecular aggregation structure and surface molecular motions of high-molecular-weight polystyrene/low-molecular-weight poly(methyl methacrylate) (HMW-PS/LMW-PMMA) blend films were investigated on the basis of X-ray photoelectron spectroscopic measurements and scanning force microscopic observations. Monodisperse PS with Mn = 1450k, where Mn denotes the number-average molecular-weight, and monodisperse PMMAs with Mn 1.2k, 4.2k, 40.5k, 144k, and 387k were used as HMW-PS and LMW-PMMAs, respectively. Static contact angle measurements revealed that the magnitudes of surface free energy, γ, of PMMAs for all Mns studied here were higher than that of PS with Mn = 1450K. In the case of the (HMW-PS/LMW-PMMA) blend films, in which the Mn for each PMMA was less than 144K, PMMA was preferentially segregated at the air-polymer interface, even though PMMA had a main chain with a higher γ compared with that of PS. It was found from scanning viscoelasticity microscopic measurements that the surface molecular motion of the (PS with Mn = 1450k/ PMMA with Mn = 4.2k) blend film was fairly activated in comparison with that of the bulk one due to the surface segregation of LMW-PMMA. The surface enrichment of LMW-PMMA can be explained by enthalpic and entropie terms as follows. (1) Since the magnitudes of γ of both chain end groups of a polymer chain synthesized by an ordinary living anionic polymerization are smaller than that of the main chain part, the chain end groups are preferentially segregated at the surface. Therefore, the chain end effect at the air-polymer interface becomes more remarkable with a decrease of Mn, due to an increases in the number density of chain end groups. (2) Since polymeric chains existing in a surface region are compressed along the direction perpendicular to the film surface, the surface chains take smaller conformational entropy in a confined state compared with that of bulk chains. The difference in conformational entropy between the surface chain and the bulk one, that is, the conformational entropic penalty of the polymeric chain at the surface, decreases with a decrease in Mn. Then, when the enthalpic and entropic effects mentioned above overcome the γ difference of main chain parts between PS and PMMA, PMMA with higher γ is stably enriched at the blend film surface.

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