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. |
From inside the book
Results 1-3 of 45
Page 121
... peak at larger r is due to all the distance vectors connecting volume elements of one sphere with volume elements of the other sphere , and the maximum of this peak corres- ponds closely to the distance separating the centres of gravity ...
... peak at larger r is due to all the distance vectors connecting volume elements of one sphere with volume elements of the other sphere , and the maximum of this peak corres- ponds closely to the distance separating the centres of gravity ...
Page 128
... peaks represent the intra - component distances , one peak the inter - com- ponent distances , and residual scattering from imperfect matching can be taken into account for by an additional , usually flat peak . The basic idea was that ...
... peaks represent the intra - component distances , one peak the inter - com- ponent distances , and residual scattering from imperfect matching can be taken into account for by an additional , usually flat peak . The basic idea was that ...
Page 182
... peak position and also the scattering peak shape ; but if this was true , one would have the interfacial area par molecule of about 0-30 Å2 , which is impossible since in the solid state , the smallest possible is 0-60 Å2 . In other ...
... peak position and also the scattering peak shape ; but if this was true , one would have the interfacial area par molecule of about 0-30 Å2 , which is impossible since in the solid state , the smallest possible is 0-60 Å2 . In other ...
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