Interfacial Properties of Polymer Nanocomposites: Role of Chain Rigidity and Dynamic Heterogeneity Length Scale

被引:131
作者
Cheng, Shiwang [1 ]
Carroll, Bobby [4 ]
Lu, Wei [5 ]
Fan, Fei [5 ]
Carrillo, Jan-Michael Y. [2 ,3 ]
Martin, Halie [5 ]
Holt, Adam P. [4 ]
Kang, Nam-Goo [1 ,5 ]
Bocharova, Vera [1 ]
Mays, Jimmy W. [1 ,5 ]
Sumpter, Bobby G. [2 ,3 ]
Dadmun, Mark [1 ,5 ]
Sokolov, Alexei P. [1 ,4 ,5 ]
机构
[1] Oak Ridge Natl Lab, Div Chem Sci, Oak Ridge, TN 37831 USA
[2] Oak Ridge Natl Lab, Ctr Nanophase Mat Sci, Oak Ridge, TN 37831 USA
[3] Oak Ridge Natl Lab, Computat Sci & Engn Div, Oak Ridge, TN 37831 USA
[4] Univ Tennessee, Dept Phys & Astron, Knoxville, TN 37996 USA
[5] Univ Tennessee, Dept Chem, Knoxville, TN 37996 USA
关键词
SEGMENTAL DYNAMICS; GLASS-TRANSITION; SUPERCOOLED LIQUIDS; MOLECULAR-DYNAMICS; RELAXATION; REINFORCEMENT; NANOPARTICLES; TEMPERATURE; BEHAVIOR; WEIGHT;
D O I
10.1021/acs.macromol.6b02816
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
While it is known that the properties of polymer nanocomposites are largely dominated by the interfacial layer around nanoparticles, the molecular parameters controlling the interfacial layer structure and dynamics remain unknown. In this work we combine small-angle X-ray scattering, differential scanning calorimetry, and broadband dielectric spectroscopy to analyze the dependence of the interfacial layer thickness, l(int), on polymer rigidity defined through the characteristic ratio, C-infinity. This analysis revealed a value of C-infinity similar to 5-7, beyond which l(int) increases substantially with C-infinity. Moreover, l(int), grows upon approaching the glass transition temperature from above, and the rate of this growth seems to correlate with polymer fragility. Most important, our analysis revealed that lint is comparable to the characteristic length scale of dynamic heterogeneities in the studied materials. These results provide new understandings of molecular parameters controlling the interfacial layer and are important not only for the field of polymer nanocomposites but also for the fields of thin polymer films and dynamics of soft matter in general.
引用
收藏
页码:2397 / 2406
页数:10
相关论文
共 60 条
[1]   ON TEMPERATURE DEPENDENCE OF COOPERATIVE RELAXATION PROPERTIES IN GLASS-FORMING LIQUIDS [J].
ADAM, G ;
GIBBS, JH .
JOURNAL OF CHEMICAL PHYSICS, 1965, 43 (01) :139-&
[2]   ON ENTANGLEMENTS OF FLEXIBLE AND RODLIKE POLYMERS [J].
AHARONI, SM .
MACROMOLECULES, 1983, 16 (11) :1722-1728
[3]  
Akcora P, 2009, NAT MATER, V8, P354, DOI [10.1038/NMAT2404, 10.1038/nmat2404]
[4]   Fifth-order susceptibility unveils growth of thermodynamic amorphous order in glass-formers [J].
Albert, S. ;
Bauer, Th. ;
Michl, M. ;
Biroli, G. ;
Bouchaud, J. -P. ;
Loidl, A. ;
Lunkenheimer, P. ;
Tourbot, R. ;
Wiertel-Gasquet, C. ;
Ladieu, F. .
SCIENCE, 2016, 352 (6291) :1308-1311
[5]   Theories and simulations of polymer-based nanocomposites: From chain statistics to reinforcement [J].
Allegra, Giuseppe ;
Raos, Guido ;
Vacatello, Michele .
PROGRESS IN POLYMER SCIENCE, 2008, 33 (07) :683-731
[6]   FORMATION OF GLASSES FROM LIQUIDS AND BIOPOLYMERS [J].
ANGELL, CA .
SCIENCE, 1995, 267 (5206) :1924-1935
[7]   Network dynamics in nanofilled polymers [J].
Baeza, Guilhem P. ;
Dessi, Claudia ;
Costanzo, Salvatore ;
Zhao, Dan ;
Gong, Shushan ;
Alegria, Angel ;
Colby, Ralph H. ;
Rubinstein, Michael ;
Vlassopoulos, Dimitris ;
Kumar, Sanat K. .
NATURE COMMUNICATIONS, 2016, 7
[8]   Nanoparticle polymer composites: Where two small worlds meet [J].
Balazs, Anna C. ;
Emrick, Todd ;
Russell, Thomas P. .
SCIENCE, 2006, 314 (5802) :1107-1110
[9]   Interface between end-functionalized PEO oligomers and a silica nanoparticle studied by molecular dynamics simulations [J].
Barbier, D ;
Brown, D ;
Grillet, AC ;
Neyertz, S .
MACROMOLECULES, 2004, 37 (12) :4695-4710
[10]   Cooperativity and the Freezing of Molecular Motion at the Glass Transition [J].
Bauer, Th. ;
Lunkenheimer, P. ;
Loidl, A. .
PHYSICAL REVIEW LETTERS, 2013, 111 (22)