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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Page 147
... potential veff ( r ) . This potential is not a pair potential and will depend , in theory , on the temperature and the colloidal and salt concentrations . This approach is interesting only if veff keeps a simple mathematical form . The ...
... potential veff ( r ) . This potential is not a pair potential and will depend , in theory , on the temperature and the colloidal and salt concentrations . This approach is interesting only if veff keeps a simple mathematical form . The ...
Page 148
... potential . The RMSA analytical solution , popularized by Hayter , Penfold and Hansen [ 10,4 ] , has been extensively used for 10 years to fit X - ray , neutron and light scattering data . The effective charge is often considered as an ...
... potential . The RMSA analytical solution , popularized by Hayter , Penfold and Hansen [ 10,4 ] , has been extensively used for 10 years to fit X - ray , neutron and light scattering data . The effective charge is often considered as an ...
Page 151
... potential . Test of the One Component Model The test a posteriori of the OCM consists to compare the polyion - polyion pp the 9pp ( r ) ( or S ( q ) ) curve obtained in the OCM with the DLVO potential and a good black box ( RMSA or HNC ) ...
... potential . Test of the One Component Model The test a posteriori of the OCM consists to compare the polyion - polyion pp the 9pp ( r ) ( or S ( q ) ) curve obtained in the OCM with the DLVO potential and a good black box ( RMSA or HNC ) ...
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
allows angle Appl applications approximation atoms average beam calculated charge Chem clusters colloidal components concentration consider constant contains contrast contribution correlation corresponds crystal curve defined density depends described determined dilute dimension direction discussed distance distribution effective electron elements energy equation example experimental experiments expression factor Figure fluctuations Fourier function given gives Glatter important increasing interactions interface labelled layer leads length light scattering limit mass means measured method molecular molecules neutron observed obtained parameters particles peak phase Phys polymer Porod position possible potential present problem radiation radius range reference reflectivity sample scale scattering intensity scattering length separation shape shear shown shows small-angle solution solvent spheres structure structure factor surface technique term transform variation volume volume fraction X-ray