Scattering from Polymers: Characterization by X-rays, Neutrons, and LightThis book reflects the recent progress made in the field of scattering in polymers. A wide range of scattering studies on different polymer systems, including block copolymers, semicrystalline polymers, complex fluids, multicomponent systems, polymeric surfaces, and polymer processing are included, as well as new experimental techniques and theoretical treatments. This volume provides a comprehensive reference for those researchers who need to know how scattering techniques can be used to tackle different polymer problems, and is ideal for graduate polymer scientists studying scattering techniques. |
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Page 11
... equation has the same form . Including the time dependent portion , this solution is E ( r , t ) = Eŋexp { i [ k • r - wt ] } for the electric field component of the wave . This is the equation of a plane wave with amplitude | Eo ...
... equation has the same form . Including the time dependent portion , this solution is E ( r , t ) = Eŋexp { i [ k • r - wt ] } for the electric field component of the wave . This is the equation of a plane wave with amplitude | Eo ...
Page 11
... equation 11. The scattering amplitude for one electron , Es , will from now on be taken as unity , and will be understood to apply to all equations dealing with scattered wave amplitude . The integral in equation 11 will be treated ...
... equation 11. The scattering amplitude for one electron , Es , will from now on be taken as unity , and will be understood to apply to all equations dealing with scattered wave amplitude . The integral in equation 11 will be treated ...
Page 19
... equation 1 the scattering length , b , depends on the details of the interaction between the neutron and the nucleus ( 4,26,28 ) . The interaction is controlled by the nuclear and spin density distributions , and in magnetic materials ...
... equation 1 the scattering length , b , depends on the details of the interaction between the neutron and the nucleus ( 4,26,28 ) . The interaction is controlled by the nuclear and spin density distributions , and in magnetic materials ...
Contents
Preface Xi | 11 |
Characteristics of SmallAngle Diffraction Data from Semicrystalline | 24 |
Block Crystallization in Model Triarm Star Block Copolymers | 28 |
Copyright | |
28 other sections not shown
Common terms and phrases
alignment American Chemical Society amorphous analysis annealing average beam behavior blends calculated Chem complexes concentration copolymer correlation function crystallization temperature decrease degree of crystallinity dependence detector differential scanning calorimetry diffraction diffusion distribution domain EMAA endotherm equation experimental experiments heating increase interactions interface isotactic isothermal isothermal crystallization lamellar stacks layer light scattering linear long period lyotropic Macromolecules measurements melting temperature micellar micelles microtubules molecular weight molecules neutron neutron scattering nucleation observed obtained orientation P(MAA/NIPAM parameters PEEK fractions Phys plot Pluronic poly(vinyl alcohol polyelectrolyte probes profiles quench reflections region rotator phase sample SAXS scanning scattering curve scattering intensity scattering patterns scattering peaks semicrystalline shear flow shear rate shown in Figure shows small angle solutions solvent spherulite structure factor surface surfactant synchrotron thermal thermotropic transition triclinic two-arm PEOs viscosity volume fraction WAXD WAXS width x-ray scattering