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 253
... clusters which make up these lumps and voids . The other way is to extract the individual clusters at different stages of the growth , and separate them to assess their masses or sizes . Then specific growth modes can be recognized ...
... clusters which make up these lumps and voids . The other way is to extract the individual clusters at different stages of the growth , and separate them to assess their masses or sizes . Then specific growth modes can be recognized ...
Page 254
... clusters with other large ones dominate ( n < 1 ) , but they do not lead to runaway growth ( 2 < 1 ) . Small clusters tend to be left behind , hence the mass distribution contains a large number of unreacted small clusters . The mass ...
... clusters with other large ones dominate ( n < 1 ) , but they do not lead to runaway growth ( 2 < 1 ) . Small clusters tend to be left behind , hence the mass distribution contains a large number of unreacted small clusters . The mass ...
Page 255
... 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 high mass ; for λ = 0 the analytical form is ( 1-1 / m m - 1 . As ...
... 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 high mass ; for λ = 0 the analytical form is ( 1-1 / m m - 1 . As ...
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