Neutron, X-ray and Light Scattering: Introduction to an Investigative Tool for Colloidal and Polymeric Systems : Proceedings of the European Workshop on Neutron, X-Ray and Light Scattering as an Investigative Tool for Colloidal and Polymeric Systems, Bombannes, France, 27 May-2 June, 1990Peter Lindner, Thomas Zemb This book is devoted to a simple practical approach to neutron, X-ray and light scattering experiments, involving model calculation of the scattering and mathematical transformation. It is intended to attract colloid and polymer scientists using scattering methods in their laboratory or at common research facilities. The primary objective is to explain the current methodology of elastic and quasi-elastic scattering techniques (avoiding both under and over-exploitation of data) rather than a general course on colloids and polymers. Basic information on data interpretation, on the complementarity of the different types of radiation, as well as information on recent applications and developments are presented. |
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Results 1-3 of 24
Page 24
... detector and the solid angle A of the detector . I。( λ ) is given by Lo ( λ ) = ( 2 ) AE ( 2 ) A ΔΩ E ( A ) where ( 2 ) is the flux ( cm - 2s - 1 ) of the incident beam of cross section A ( cm2 ) and E ( X ) the efficiency of the ...
... detector and the solid angle A of the detector . I。( λ ) is given by Lo ( λ ) = ( 2 ) AE ( 2 ) A ΔΩ E ( A ) where ( 2 ) is the flux ( cm - 2s - 1 ) of the incident beam of cross section A ( cm2 ) and E ( X ) the efficiency of the ...
Page 286
... Detector plane Figure 9. Schematic model of a focusing SAXS - camera . Sa : beam defining ; Sa : antiscatter ; S .: guard slits . Note the diffuse scattering around the primary beam in the detector plane due to scattering from the ...
... Detector plane Figure 9. Schematic model of a focusing SAXS - camera . Sa : beam defining ; Sa : antiscatter ; S .: guard slits . Note the diffuse scattering around the primary beam in the detector plane due to scattering from the ...
Page 313
... detector . The number of coherence areas at the detector is important only in dynamic light scattering experiments ( QELS and LDV ) . Fluctuations in the local dielectric constant & are generated by Brownian mo- tion of the particles or ...
... detector . The number of coherence areas at the detector is important only in dynamic light scattering experiments ( QELS and LDV ) . Fluctuations in the local dielectric constant & are generated by Brownian mo- tion of the particles or ...
Contents
Introduction to scattering experiments | 3 |
Initial data treatment | 19 |
Smallangle scattering and light scattering | 33 |
Copyright | |
15 other sections not shown
Common terms and phrases
amplitude angle scattering Appl atoms average beam calculated Chem chord distribution clusters coefficient coil colloidal components concentration contrast variation correlation function corresponds counterions Cryst crystal curvature Debye detector determined deuterated diffusion dilute dimension distance distribution function DLVO dodecanol effective electron electrostatic energy equation experimental extrapolation Figure fluctuations Fourier transform fractal Glatter Guinier homogeneous incoherent scattering interactions interface ionic isotopic Kratky labelled layer light scattering linear Macromolecules measured method micelles molecular molecules monodisperse monomers neutron scattering obtained parameters particles PDDF peak phase Phys polydisperse polymer chain polystyrene Porod potential problem proteins radius of gyration range refractive index sample scattering curve scattering experiments scattering function scattering intensity scattering length scattering vector shear gradient small-angle scattering solvent spheres spherical Stuhrmann subunits surface surfactant suspensions Synchrotron Radiation technique temperature term virial volume fraction wavelength X-ray scattering Zemb zero