## 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. |

### From inside the book

Results 1-3 of 84

Page 179

2 ) i = li = 1 where VX ( R ) is the interaction energy of

by distance Rj ; in the absence of any other

( derived from second - order quantum perturbation theory , Appendix A1 ) ( 4 .

2 ) i = li = 1 where VX ( R ) is the interaction energy of

**molecules**i and j separatedby distance Rj ; in the absence of any other

**molecules**. For van der Waals forces( derived from second - order quantum perturbation theory , Appendix A1 ) ( 4 .

Page 459

5 Theta - point of polymer

special importance in polymer solution thermodynamics . It is closely analogous

to the Boyle point for real gases ( Flory 1953 ) . An ideal gas , which notionally ...

5 Theta - point of polymer

**molecules**The A - point of polymer**molecules**is ofspecial importance in polymer solution thermodynamics . It is closely analogous

to the Boyle point for real gases ( Flory 1953 ) . An ideal gas , which notionally ...

Page 628

where pA and p are the instantaneous dipole moments of

defined in eqn ( A1 . ... 7 ) for Vine the general solution of Schrödinger ' s

equation for the two -

perturbation ...

where pA and p are the instantaneous dipole moments of

**molecules**A and B asdefined in eqn ( A1 . ... 7 ) for Vine the general solution of Schrödinger ' s

equation for the two -

**molecule**system is intractable and we must resort toperturbation ...

### What people are saying - Write a review

User Review - Flag as inappropriate

home

### 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 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