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 58
Page 85
... average P ( r ) Fourier transform A ( s ) square Polydisperse systems DN ( R ) Densely packed systems 1 ( 3 ) Y ( r ) Fourier transform average about orientation size and form factor average P ( x ) Zernike - Prins Nonparticulate ...
... average P ( r ) Fourier transform A ( s ) square Polydisperse systems DN ( R ) Densely packed systems 1 ( 3 ) Y ( r ) Fourier transform average about orientation size and form factor average P ( x ) Zernike - Prins Nonparticulate ...
Page 255
... average mass versus reaction time . Class III : λ < v < 1. Large clusters react preferentially with much smaller ones ( v < λ ) . Thus small clusters are mopped up , and the mass distribution has a broad maximum with a sharp decay at ...
... average mass versus reaction time . Class III : λ < v < 1. Large clusters react preferentially with much smaller ones ( v < λ ) . Thus small clusters are mopped up , and the mass distribution has a broad maximum with a sharp decay at ...
Page 356
... average number of molecules belonging at a given instant at a given micellar aggregate is the aggregation number ( N ) ... average Mw or number average Mn . Scattering methods always give the mass average Mw : Mw = Σ M2 ni i Σ Mi⚫ni i ...
... average number of molecules belonging at a given instant at a given micellar aggregate is the aggregation number ( N ) ... average Mw or number average Mn . Scattering methods always give the mass average Mw : Mw = Σ M2 ni i Σ Mi⚫ni i ...
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