The Science of Heterogeneous Polymers: Structure and Thermophysical PropertiesThe Science of Heterogeneous Polymers Structure and Thermophysical Properties V. P. Privalko Academy of Sciences of the Ukraine, Kiev, Ukraine and V. V. Novikov Odessa Polytechnical Institute, Odessa, Ukraine The impact of structural heterogeneity on the materials science of polymers cannot be understated, and has provided the stimulus for the production of this comprehensive treatise on the subject. Presented in two parts, the first reviews evidence of heterogeneity of filled polymers, polymer blends and co-polymers on different structural scales. The second section is devoted to the analysis of composition, dependence of heat conductivity and thermoelastic parameters of different polymeric materials, and also develops the Step-by-Step Averaging approach. Providing both a critical evaluation of characterization methods and a quantitative description of composition-dependent properties, The Science of Heterogeneous Polymers will have broad appeal within academic and industrial sectors, being of particular interest to researchers and postgraduate students of materials and polymer science, as well as engineers and technicians developing polymers for advanced technologies. |
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Page 188
... tensors defined as klmn klmn = = S ( 1 ) - klmn ( 5.6a ) ( 5.6b ) < o > = Buimn < mn > ( 5.7a ) ( 5.7b ) < ε ) ) = Amn ' kl klmn < & mn > and Ikimn is the fourth - rank unit tensor . Each of coupled eqs . ( 5.5 ) and ( 5.6 ) contain ...
... tensors defined as klmn klmn = = S ( 1 ) - klmn ( 5.6a ) ( 5.6b ) < o > = Buimn < mn > ( 5.7a ) ( 5.7b ) < ε ) ) = Amn ' kl klmn < & mn > and Ikimn is the fourth - rank unit tensor . Each of coupled eqs . ( 5.5 ) and ( 5.6 ) contain ...
Page 197
... tensor of compliance of the prism with L for the height and dx , dx2 for the basal area , ( L1 ( x1 , x2 ) ) = L1 ... tensor B ( x1 , x2 ) is defined as ( 5.56 ) { on ( r ) } L = Bank ( X1 , X2 ) { σki ( P ) } L mn mnkl 1 mnij ...
... tensor of compliance of the prism with L for the height and dx , dx2 for the basal area , ( L1 ( x1 , x2 ) ) = L1 ... tensor B ( x1 , x2 ) is defined as ( 5.56 ) { on ( r ) } L = Bank ( X1 , X2 ) { σki ( P ) } L mn mnkl 1 mnij ...
Page 227
... tensor & do not coincide with the axes of the laboratory system of coordinates , we can use the tensors of rotation by angle , ø , and determine ' in the laboratory system of coordinates . As an example , consider the transforation of ...
... tensor & do not coincide with the axes of the laboratory system of coordinates , we can use the tensors of rotation by angle , ø , and determine ' in the laboratory system of coordinates . As an example , consider the transforation of ...
Common terms and phrases
Acad assuming binary block copolymers broken line chain Chem cm³/g component Composition dependence contribution corresponding crystalline decrease density Dokl effect elastic enthalpy equation estimated experimental data filled polymers filled samples filler content filler particles filler surface free energy Gibbs free energy glass transition temperature heat capacity heat conductivity Heterogeneous nucleation highly filled increase interactions interface isotactic Kiev kinetics klmn latter layers linear Lipatov Yu liquid Macromolecules microphase modulus molecular morphology nucleation observed obtained oligomers P₁ parameters percolation phase separation PMMA poly(ethylene poly(methyl methacrylate polymer blends polymer melt Polymer Phys Polymer Sci polymer systems polymeric polypropylene polystyrene polyurethane predictions pressure Privalko V. P. properties pure polymer random relaxation respectively segments single-phase specific volume spherulite spinodal decomposition structure substrates T₂ temperature interval theoretical thermal expansion thermodynamic thickness v₁ values viscosity Vysokomol Young's modulus Zhurn ΔΗ