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 301
... satisfactory on a solid surface where unbalanced stresses may be taken up by
the solid ; the derivation of eqn ( 5 . 10 . 21 ) requires only that the solid be rigid .
Exercises . 5 . 10 . 1 The volume of a spherical cap ( such as that shown in Fig .
... satisfactory on a solid surface where unbalanced stresses may be taken up by
the solid ; the derivation of eqn ( 5 . 10 . 21 ) requires only that the solid be rigid .
Exercises . 5 . 10 . 1 The volume of a spherical cap ( such as that shown in Fig .
Page 457
... layers must be sufficiently large . The thermodynamic limit to stability under
these conditions has been shown experimentally to be largely independent of the
chemical nature of the anchor polymer and , commonly , the nature and size of
the ...
... layers must be sufficiently large . The thermodynamic limit to stability under
these conditions has been shown experimentally to be largely independent of the
chemical nature of the anchor polymer and , commonly , the nature and size of
the ...
Page 502
4 Stress and velocity field in a fluid in thermodynamic equilibrium By
thermodynamic arguments it can be shown ( Landau and Lifshitz 1969 , section
12 ) that the stress in a fluid in equilibrium is given simply by S ( x , ñ ) = - p ( x )
ÊN , ( 9 . 4 .
4 Stress and velocity field in a fluid in thermodynamic equilibrium By
thermodynamic arguments it can be shown ( Landau and Lifshitz 1969 , section
12 ) that the stress in a fluid in equilibrium is given simply by S ( x , ñ ) = - p ( x )
ÊN , ( 9 . 4 .
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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