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 542
Since the problem is linear , we can write S as the sum of a dipole strength due to
the rigid body velocity field , plus a dipole strength due to the portion of the
ambient field rigid body , the sum of ath due to the Žex ; ( 9 . 10 . 11 ) Since there
is no ...
Since the problem is linear , we can write S as the sum of a dipole strength due to
the rigid body velocity field , plus a dipole strength due to the portion of the
ambient field rigid body , the sum of ath due to the Žex ; ( 9 . 10 . 11 ) Since there
is no ...
Page 543
Thus particles in the viscosity problem will exhibit less interaction than in the
sedimentation problem , and our dilute approximation should , therefore , be valid
for a greater concentration range than in the sedimentation problem . For a rigid ...
Thus particles in the viscosity problem will exhibit less interaction than in the
sedimentation problem , and our dilute approximation should , therefore , be valid
for a greater concentration range than in the sedimentation problem . For a rigid ...
Page 557
The earliest solution to this problem was given by Smoluchowski ( 1921 ) for the
ka > > 1 ( thin double - layer ) case . Smoluchowski reasoned that the problem of
determining the local flow in the double layer in this case is the same as the ...
The earliest solution to this problem was given by Smoluchowski ( 1921 ) for the
ka > > 1 ( thin double - layer ) case . Smoluchowski reasoned that the problem of
determining the local flow in the double layer in this case is the same as the ...
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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