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 6
3 Classification of colloids Freundlich , in his classical text on the subject ( 1926 )
, suggested that colloidal dispersions could be divided into two classes , called
lyophilic ( solvent loving ) and lyophobic ( solvent hating ) respectively ...
3 Classification of colloids Freundlich , in his classical text on the subject ( 1926 )
, suggested that colloidal dispersions could be divided into two classes , called
lyophilic ( solvent loving ) and lyophobic ( solvent hating ) respectively ...
Page 462
Thus the 6 - point represents the transitional point with respect to segment -
solvent interactions : at this point , the polymer segments change from exhibiting
a net mutual repulsion to a net mutual attraction . A fuller description of that
change ...
Thus the 6 - point represents the transitional point with respect to segment -
solvent interactions : at this point , the polymer segments change from exhibiting
a net mutual repulsion to a net mutual attraction . A fuller description of that
change ...
Page 470
The experimental results imply that there is a noncombinatorial entropy change
that opposes the mixing of polymer and solvent and is not accounted for by the
Flory - Huggins theory . Second , X1 is found experimentally to depend upon the
...
The experimental results imply that there is a noncombinatorial entropy change
that opposes the mixing of polymer and solvent and is not accounted for by the
Flory - Huggins theory . Second , X1 is found experimentally to depend upon the
...
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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 |
Common terms and phrases
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