Segmented Copolymers: Morphological, Rheo-optical and Dielectric Studies |
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Page viii
... Dispersed Spheres 199 201 203 2. Equations for Dispersed Cylinders or Rods 206 3. Equations for Dispersed Lamellae 207 VIII . Survey of Ultra - Low Frequency Techniques 209 IX . Design of the ULF System using a Computerized Data Acquisi ...
... Dispersed Spheres 199 201 203 2. Equations for Dispersed Cylinders or Rods 206 3. Equations for Dispersed Lamellae 207 VIII . Survey of Ultra - Low Frequency Techniques 209 IX . Design of the ULF System using a Computerized Data Acquisi ...
Page 203
... dispersed particles are non- spherical , interfacial polarization will be dependent on the geometry and orientation of the occluded phase . Theoretical studies of the dielectric behavior of heterogenous sys- tems have been advanced in ...
... dispersed particles are non- spherical , interfacial polarization will be dependent on the geometry and orientation of the occluded phase . Theoretical studies of the dielectric behavior of heterogenous sys- tems have been advanced in ...
Page 206
... Dispersed Cylinders or Rods For long prolate spheroids A = ( -8 , -8,28 ) , where 8 << 1 . Insert- i ing these values into Eq . VII - 7 one obtains < = < + ( 1/3 ) v1⁄2 ( 2-4 206 Equations for Dispersed Cylinders or Rods.
... Dispersed Cylinders or Rods For long prolate spheroids A = ( -8 , -8,28 ) , where 8 << 1 . Insert- i ing these values into Eq . VII - 7 one obtains < = < + ( 1/3 ) v1⁄2 ( 2-4 206 Equations for Dispersed Cylinders or Rods.
Contents
Literature Review | 9 |
Experimental | 23 |
Results and Discussion | 36 |
Copyright | |
6 other sections not shown
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amorphous angle annealing apparent approximately associated average axis becomes behavior block length bridge cast CHARACTERIZATION circuit component composition Compression Molded concentration conductivity consists containing copolymers crystalline crystallization curves decreases deformation dependent determined dielectric constant direction dispersed domains dynamic mechanical effect elastomers elongation energy exhibit experiments extension frequency function glass hard segment hard segment content heat higher homopolymer increase interfacial light lower materials measurements mechanical properties melting method Model modulus molecular morphology motion observed obtained occurs optical orientation parallel pattern PDMS peak phase plate polarization polycarbonate polyether polymers position prepared properties PTMT R₁ range ratio relatively relaxation respectively sample scattering separation shown in Figure shows signal similar soft segments solvent spherulitic strain stretching structure suggests Table temperature thermal tion transition units weight