Foundations of Colloid Science, Volume 1Liquid suspension systems are the basic ingredients of paints, detergents, biological cells, and countless other systems of scientific and technological importance. This book presents the fundamental physical and chemical concepts necessary to the understanding of these systems and of colloid science in general. New ideas are introduced carefully and formulae are developed in full, with exercises to help the reader throughout. The frequent references to the many applications of colloid science will be especially helpful to beginning research scientists and people in industry, medicine and agriculture who often find their training in this area inadequate. Integrating developments from the time of colloid science's infancy forty years ago to its present state as a rigorous discipline, this intelligently assembled work elucidates a remarkable range of concepts, techniques, and behaviors. |
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Page 200
The dielectric response function e ( w ) for a single undamped oscillator of
resonance frequency wo . We will discuss the function e ( i ) later , but note how
simple it is in form compared to the behaviour of ε ' in the neighbourhood of an ...
The dielectric response function e ( w ) for a single undamped oscillator of
resonance frequency wo . We will discuss the function e ( i ) later , but note how
simple it is in form compared to the behaviour of ε ' in the neighbourhood of an ...
Page 203
39 ) , that the ε function can take complex values for its argument but the results of
Exercise 2 . 2 . 8 show that this is merely a mathematical manipulation of the
function ε = E ' + ie " of a real variable . For later use we must now formally extend
...
39 ) , that the ε function can take complex values for its argument but the results of
Exercise 2 . 2 . 8 show that this is merely a mathematical manipulation of the
function ε = E ' + ie " of a real variable . For later use we must now formally extend
...
Page 214
positive , elić ) is a monotonic decreasing function of Ę . Thus £li£ ) decreases
steadily from the static dielectric constant e ( 0 ) at & = 0 to E , at & = 0o ( see Figs
4 . 7 . 2 and 4 . 7 . 3 ) . It is this well - behaved nature of e ( i ) that enables its ...
positive , elić ) is a monotonic decreasing function of Ę . Thus £li£ ) decreases
steadily from the static dielectric constant e ( 0 ) at & = 0 to E , at & = 0o ( see Figs
4 . 7 . 2 and 4 . 7 . 3 ) . It is this well - behaved nature of e ( i ) that enables its ...
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Contents
CHARACTERIZATION OF COLLOIDAL | 2 |
BEHAVIOUR OF COLLOIDAL DISPERSIONS | 49 |
PARTICLE SIZE AND SHAPE | 104 |
Copyright | |
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Foundations of Colloid Science, Volume 1 Robert J. Hunter,Lee R. White,Derek Y. C. Chan Snippet view - 1987 |
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adsorbed adsorption applied approach approximation assumed becomes behaviour body bulk calculated called Chapter charge chemical coagulation colloidal compared component concentration Consider constant corresponding curve density depends described determined diffuse dipole discussion dispersion distance distribution double layer effect electric electrolyte electron equal equation equilibrium Establish estimate Exercise experimental expression field flocculation flow fluid follows force free energy frequency function given gives important increase integral interaction interface ions layer light limit liquid material mean measured method micelle molecules motion negative Note obtained occurs particles phase plates polymer positive possible potential presence pressure problem procedure quantity radius range referred region relation relative result scattering separation shape shear shown simple solid solution solvent stabilization steric stress surface surface tension suspension Table temperature tension term theory unit usually volume zero