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 387
Sum of diffuse layer charge ( 0 ) and Stern layer charge ( 00 - , ONa + ) with the
measured surface charge ( 00 ) . ( From Foissy et al . 1982 , with permission . )
disposition of the counter charge . They find ( Fig . 6 . 10 . 6 ) that less than 10 per
...
Sum of diffuse layer charge ( 0 ) and Stern layer charge ( 00 - , ONa + ) with the
measured surface charge ( 00 ) . ( From Foissy et al . 1982 , with permission . )
disposition of the counter charge . They find ( Fig . 6 . 10 . 6 ) that less than 10 per
...
Page 389
The diffuse double layer around a sphere of low potential . ( Note the change of
coordinate system . ) The solution of this equation , for a particle of radius ao ,
with a compact layer of thickness d ( Fig . 6 . 11 . 1 ) is ( Exercise 6 . 11 . 1 ) : W =
4o ...
The diffuse double layer around a sphere of low potential . ( Note the change of
coordinate system . ) The solution of this equation , for a particle of radius ao ,
with a compact layer of thickness d ( Fig . 6 . 11 . 1 ) is ( Exercise 6 . 11 . 1 ) : W =
4o ...
Page 422
... in the equations for the repulsive potential energy . Since the interaction occurs
between the diffuse layers it would seem to be more reasonable to assess the
magnitude of VR from the value of the diffuse layer potential , Wa ( section 6 . 3 ) .
... in the equations for the repulsive potential energy . Since the interaction occurs
between the diffuse layers it would seem to be more reasonable to assess the
magnitude of VR from the value of the diffuse layer potential , Wa ( section 6 . 3 ) .
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Contents
CHARACTERIZATION OF COLLOIDAL | 1 |
BEHAVIOUR OF COLLOIDAL DISPERSIONS | 52 |
PARTICLE SIZE AND SHAPE | 106 |
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 attraction average becomes behaviour bulk calculated called Chapter charge chemical coagulation colloidal compared components concentration constant contribution corresponding curve density depends derived 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 formula free energy function given gives groups important increase integral interaction interface ions liquid material measured method micelle molecules motion negative Note observed obtained occurs particles phase plates polymer positive possible potential presence pressure problem procedure quantity radius range referred region relation relative repulsion result separation shear shown solid solution solvent stabilization steric stress surface surface charge surface tension suspension Table temperature term theory unit usually volume zero