## 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 205

The only exceptions to this approximation are the ferromagnetic materials , where

u ( w ) can be ~ 10°40 or more . naproximations of the permeability Note that the

velocity of light in vacuo is

The only exceptions to this approximation are the ferromagnetic materials , where

u ( w ) can be ~ 10°40 or more . naproximations of the permeability Note that the

velocity of light in vacuo is

**given**by c = ( Eoko ) - 112 ( 4 . 7 . 23 ) a result we ...Page 404

3 . 10 ) from the midplane where X = 0 and Q = 0 to obtain corresponding values

of Q and X . When I reaches the value Qs , the corresponding X value ...

**Given**any arbitrary ym ( with lym < lyol ) one can integrate ( numerically ) egn ( 7 .3 . 10 ) from the midplane where X = 0 and Q = 0 to obtain corresponding values

of Q and X . When I reaches the value Qs , the corresponding X value ...

Page 515

1 ) , we find the local Cartesian components of Au are

From the formula ( 9 . 5 . 9 ) for the rate of strain tensor , we see that the only non -

zero components of e at 0 are 112 and 221 , both of which are

1 ) , we find the local Cartesian components of Au are

**given**by and Av2 = ( 21 .From the formula ( 9 . 5 . 9 ) for the rate of strain tensor , we see that the only non -

zero components of e at 0 are 112 and 221 , both of which are

**given**by ( 9 . 7 .### What people are saying - Write a review

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### Contents

CHARACTERIZATION OF COLLOIDAL | 2 |

BEHAVIOUR OF COLLOIDAL DISPERSIONS | 49 |

PARTICLE SIZE AND SHAPE | 104 |

Copyright | |

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### Other editions - View all

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 angle 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 stress surface surface tension suspension Table temperature tension term theory unit usually volume zero