## 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 86

Page 343

... is balanced by an excess of anions or a deficit of cations . In the absence of

specific adsorption the balance is determined solely by the Poisson - Boltzmann

equation and it can be shown ( Parsons 1957 ) that , in that case (

... is balanced by an excess of anions or a deficit of cations . In the absence of

specific adsorption the balance is determined solely by the Poisson - Boltzmann

equation and it can be shown ( Parsons 1957 ) that , in that case (

**Exercise**6 . 4 .Page 441

8 . 3 ) ar where v is the particle concentration and D is the diffusion coefficient .

The solution to this equation for the appropriate boundary conditions is (

7 . 8 . 1 ) : v = VO 940r ( 7 . 8 . 4 ) where vo is the ( bulk ) particle concentration far

...

8 . 3 ) ar where v is the particle concentration and D is the diffusion coefficient .

The solution to this equation for the appropriate boundary conditions is (

**Exercise**7 . 8 . 1 ) : v = VO 940r ( 7 . 8 . 4 ) where vo is the ( bulk ) particle concentration far

...

Page 580

Mi , the total monomer concentration , now becomes (

3 . 23 ) ? ( 1 - XO2 and thus 112 ( [ x ] ) " = 1 – K [ vi ] ( 10 . 3 . 24 ) Mi so that if ( xi )

is measured experimentally ( Mukerjee and Ghosh 1970 ) , K may be evaluated ...

Mi , the total monomer concentration , now becomes (

**Exercise**10 . 3 . 5 ) : ( 10 .3 . 23 ) ? ( 1 - XO2 and thus 112 ( [ x ] ) " = 1 – K [ vi ] ( 10 . 3 . 24 ) Mi so that if ( xi )

is measured experimentally ( Mukerjee and Ghosh 1970 ) , K may be evaluated ...

### 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 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