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 176
13 ) Cas - Campagnes 11 1 / 2 \ N Since the dominant frequency is usually that of
an outer orbital electronic transition , a better approximation results by taking Na
to be the number of electrons in the outer orbital only . Since Na enters to the ...
13 ) Cas - Campagnes 11 1 / 2 \ N Since the dominant frequency is usually that of
an outer orbital electronic transition , a better approximation results by taking Na
to be the number of electrons in the outer orbital only . Since Na enters to the ...
Page 191
6 The Deryaguin approximation When dealing with interactions between
macrobodies , it is often the case that the range of ... Under these circumstances ,
a very useful approximate expression for the interaction energy of the bodies can
be ...
6 The Deryaguin approximation When dealing with interactions between
macrobodies , it is often the case that the range of ... Under these circumstances ,
a very useful approximate expression for the interaction energy of the bodies can
be ...
Page 192
If E ( D ) is the energy per unit area of half - space 1 interacting with the half -
space 2 , then , in this approximation , dV = E ( D ) ds , ( 4 . 6 . 1 ) is the interaction
energy of the area element dS , of body 1 with body 2 . The distance D increases
as ...
If E ( D ) is the energy per unit area of half - space 1 interacting with the half -
space 2 , then , in this approximation , dV = E ( D ) ds , ( 4 . 6 . 1 ) is the interaction
energy of the area element dS , of body 1 with body 2 . The distance D increases
as ...
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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