## 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 208

In Lifshitz theory , the temperature enters explicitly . Note that , as T→0 , the

spacing 20kTlh between successive values in the frequency sum ( eqn ( 4 . 7 . 32

) ) tends to zero and the sum tends to a frequency

271 ...

In Lifshitz theory , the temperature enters explicitly . Note that , as T→0 , the

spacing 20kTlh between successive values in the frequency sum ( eqn ( 4 . 7 . 32

) ) tends to zero and the sum tends to a frequency

**integral**( 4 . 7 . 34 ) ' f ( E . ) 70271 ...

Page 209

The functions De and DM are the electric and magnetic dispersion relations

corresponding to e . m . radiation with transverse ( i . e . parallel to the half -

space surface ) wave vector Q . The

free energy ...

The functions De and DM are the electric and magnetic dispersion relations

corresponding to e . m . radiation with transverse ( i . e . parallel to the half -

space surface ) wave vector Q . The

**integral**in eqn ( 4 . 7 . 36 ) represents thefree energy ...

Page 336

30 ) фа The quantity Kj is called the

layer and egn ( 6 . 3 . 30 ) shows that for low potentials the diffuse layer behaves

like a parallel plate condenser with a spacing of 1 / k between the plates , a ...

30 ) фа The quantity Kj is called the

**integral**capacitance of the ( diffuse ) doublelayer and egn ( 6 . 3 . 30 ) shows that for low potentials the diffuse layer behaves

like a parallel plate condenser with a spacing of 1 / k between the plates , 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 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