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 395
DOUBLE LAYER INTERACTION AND PARTICLE COAGULATION 7 . 1 Surface
conditions during interaction 7 . 2 Free energy of formation of a double layer 7 . 3
Overlap of two flat double layers 7 . 3 . 1 Approximate relations for overlap of flat ...
DOUBLE LAYER INTERACTION AND PARTICLE COAGULATION 7 . 1 Surface
conditions during interaction 7 . 2 Free energy of formation of a double layer 7 . 3
Overlap of two flat double layers 7 . 3 . 1 Approximate relations for overlap of flat ...
Page 397
In most interaction situations it is only the diffuse layers that interact so that the
boundary electrostatic potential ( section 6 . 3 ) is Ya ... We will begin , therefore ,
with an examination of the free energy of a single ( i . e . isolated ) double layer .
7 .
In most interaction situations it is only the diffuse layers that interact so that the
boundary electrostatic potential ( section 6 . 3 ) is Ya ... We will begin , therefore ,
with an examination of the free energy of a single ( i . e . isolated ) double layer .
7 .
Page 426
For films with a water - layer thickness greater than about 10 nm the dominant
force is , for the case of ionic surfactants , due to double - layer repulsion ; it is
usually balanced by hydrostatic pressure ( see Fig . 7 . 7 . 5 ( a ) ) . A soap film
can ...
For films with a water - layer thickness greater than about 10 nm the dominant
force is , for the case of ionic surfactants , due to double - layer repulsion ; it is
usually balanced by hydrostatic pressure ( see Fig . 7 . 7 . 5 ( a ) ) . A soap film
can ...
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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