Advanced Search

Journal Navigation

Journal Home

Subscriptions

Archive

Contact Us

Table of Contents

Click here to sign up for SAGE Journal Email Alerts today!

Sign In to gain access to subscriptions and/or personal tools.
High Performance Polymers
This Article
Right arrow Full Text (PDF)
Right arrow References
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Email this article to a friend
Right arrow Similar articles in this journal
Right arrow Alert me to new issues of the journal
Right arrow Add to Saved Citations
Right arrow Download to citation manager
Right arrowRequest Permissions
Right arrow Request Reprints
Right arrow Add to My Marked Citations
Citing Articles
Right arrow Citing Articles via Google Scholar
Right arrow Citing Articles via Scopus
Google Scholar
Right arrow Articles by Kajiyama, T.
Right arrow Articles by Takahara, A.
Right arrow Search for Related Content
Social Bookmarking
 Add to CiteULike   Add to Complore   Add to Connotea   Add to Del.icio.us   Add to Digg   Add to Reddit   Add to Technorati   Add to Twitter  
What's this?

Determination Factors on Surface Glass Transition Temperatures of Polymeric Solids

Tisato Kajiyama

Department of Applied Chemistry, Faculty of Engineering, Kyushu University, Fukuoka 812-8581, Japankajiyama{at}cstf.kyushu-u.ac.jp

Daisuke Kawaguchi

Atsushi Sakai

Noriaki Satomi

Keiji Tanaka

Department of Applied Chemistry, Faculty of Engineering, Kyushu University, Fukuoka 812-8581, Japan

Atsushi Takahara

Institute for Fundamental Research of Organic Chemistry, Kyushu University, Fukuoka 812-8581, Japan

The surface molecular motion of monodisperse proton-terminated polystyrene (PS-H), {alpha}, {omega}-diamino-terminated PS ({alpha}, {omega}-PS(NH2)2) and {alpha}, {omega}-dicarboxy-terminated PS ({alpha}, {omega}-PS(COOH)2) films was studied by scanning viscoelasticity microscopy in conjunction with lateral force microscopy. The glass transition temperature Tg, at the surface, Tgs was found to be markedly lower than bulk Tg, Tgb, and the number-average molecular weight, Mn, dependence of Tgs more remarkable than that of Tgb. Also, the magnitude of Tgs was strongly dependent on the chain end chemistry. Hence, the activation of surface molecular motion was explained in terms of an excess free volume induced by the preferential surface segregation of chain end groups. The chain end segregation at the film surface was confirmed by dynamic secondary ion mass spectroscopic measurement. However, the Tgs for the PS-H with quasi-infinite Mn was lower than the corresponding Tgb, even though the number density of chain ends was almost negligible. In addition, Tgs for PS films with hydrophilic chain ends, which might be depleted at the film surface, were lower than the bulk values. The apparent activation energy for the surface micro-Brownian motion corresponding to the {alpha}a-relaxation process was approximately half of the bulk value. Finally, the depression of Tgs in comparison with Tgs is discussed on the basis of several factors, such as a decreased segment size of molecular motion for the surface {alpha}a-relaxation process due to the existence of the free space on the polymer surface and/or a reduced chain entanglement at the surface, in addition to the chain end effect.

High Performance Polymers, Vol. 12, No. 4, 587-597 (2000)
DOI: 10.1088/0954-0083/12/4/314


Add to CiteULike CiteULike   Add to Complore Complore   Add to Connotea Connotea   Add to Del.icio.us Del.icio.us   Add to Digg Digg   Add to Reddit Reddit   Add to Technorati Technorati   Add to Twitter Twitter    What's this?