## 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 498

For small AA it is assumed that the force per

the size and shape of AA . This ratio is called the stress and is denoted by S ( x , h

) , where x is the position vector to the centre of the area element . As well as ...

For small AA it is assumed that the force per

**unit**area AF MA is independent ofthe size and shape of AA . This ratio is called the stress and is denoted by S ( x , h

) , where x is the position vector to the centre of the area element . As well as ...

Page 510

2 ) for the stress force per

make the physical significance of the viscous force term n Vav a little clearer , we

will rederive this term for a unidirectional flow , starting with the Newtonian ...

2 ) for the stress force per

**unit**volume becomes - Vp + nav . ( 9 . 6 . 4 ) In order tomake the physical significance of the viscous force term n Vav a little clearer , we

will rederive this term for a unidirectional flow , starting with the Newtonian ...

Page 511

We let F denote the total long - range force per

such force : F = pg , ( 9 . 6 . 5 ) where , as before , & is the gravitational

acceleration vector , directed vertically down . The total force per

...

We let F denote the total long - range force per

**unit**volume . If gravity is the onlysuch force : F = pg , ( 9 . 6 . 5 ) where , as before , & is the gravitational

acceleration vector , directed vertically down . The total force per

**unit**volume on a...

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### Contents

CHARACTERIZATION OF COLLOIDAL | 2 |

BEHAVIOUR OF COLLOIDAL DISPERSIONS | 49 |

PARTICLE SIZE AND SHAPE | 104 |

Copyright | |

11 other sections not shown

### 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 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