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 71
Page 29
... term can be neglected ( see the discussion concerning the compressibility term in reference [ 9 ] ) ; this can be written : ST ( q ) = n + n2g ( q ) = = KT XT where v = VH = VD and XT is the isothermal compressibility . ( A3 ) From ...
... term can be neglected ( see the discussion concerning the compressibility term in reference [ 9 ] ) ; this can be written : ST ( q ) = n + n2g ( q ) = = KT XT where v = VH = VD and XT is the isothermal compressibility . ( A3 ) From ...
Page 125
... term is usually dominated by the scattering from the stripped complex ( term 1 ) , but also the other interference terms can become important . In order to reduce the influence of statistical errors by avoi- ding differences of large ...
... term is usually dominated by the scattering from the stripped complex ( term 1 ) , but also the other interference terms can become important . In order to reduce the influence of statistical errors by avoi- ding differences of large ...
Page 202
... term and a background term which has not been subtracted . The slope of the straight line yields the background contribution , the intercept at the origin is the coefficient of the Porod's term . 15 5 qʻx ig ( q ) ( 104 cm ) X1 = 1 q ...
... term and a background term which has not been subtracted . The slope of the straight line yields the background contribution , the intercept at the origin is the coefficient of the Porod's term . 15 5 qʻx ig ( q ) ( 104 cm ) X1 = 1 q ...
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