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 131
6 ) is indeed equal to o . This is exactly analogous to the demonstration ( using
eqn ( 2 . 1 . 25 ) ) that the r . m . s . displacement of a diffusing particle is equal to
o ( Exercise 2 . 1 . 7 ) . Any of the expressions given for discrete distributions can
...
6 ) is indeed equal to o . This is exactly analogous to the demonstration ( using
eqn ( 2 . 1 . 25 ) ) that the r . m . s . displacement of a diffusing particle is equal to
o ( Exercise 2 . 1 . 7 ) . Any of the expressions given for discrete distributions can
...
Page 236
Now consider the consequences of the fact that the forces on opposite sides of
an infinitesimally small cube must be equal and opposite for mechanical
equilibrium . The net pressure normal to the surface must be constant right
through the ...
Now consider the consequences of the fact that the forces on opposite sides of
an infinitesimally small cube must be equal and opposite for mechanical
equilibrium . The net pressure normal to the surface must be constant right
through the ...
Page 249
This equation shows that fo is not equal to the surface tension , y , except for a
specific choice of the Gibbs dividing surface , namely that where Euili = 0 ; this is
a very easy and natural choice for a one - component system , but highly unusual
...
This equation shows that fo is not equal to the surface tension , y , except for a
specific choice of the Gibbs dividing surface , namely that where Euili = 0 ; this is
a very easy and natural choice for a one - component system , but highly unusual
...
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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