外文翻译-关于这份指南的介绍.docx
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1、Chapter 1The Electrokinetic ConnectionParticle Charge Prevents CoagulationThe key to effective coagulation and floccu-lation is an understanding of how individ-ual colloids interact with each other. Tur-bidity particles range from about .01 to 100microns in size. The larger fraction isrelatively eas
2、y to settle or filter. Thesmaller, colloidal fraction, (from .01 to 5microns), presents the real challenge. Theirsettling times are intolerably slow and theyeasily escape filtration.The behavior of colloids in water is stronglyinfluenced by their electrokinetic charge.Each colloidal particle carries
3、 a like charge,which in nature is usually negative. Thislike charge causes adjacent particles torepel each other and prevents effectiveagglomeration and flocculation. As aresult, charged colloids tend to remaindiscrete, dispersed, and in suspension.On the other hand, if the charge is signifi-cantly
4、reduced or eliminated, then thecolloids will gather together. First formingsmall groups, then larger aggregates andfinally into visible floc particles which settlerapidly and filter easily.Uncharged Particles are free to collide and agregate.Charged Particles repel each other1Chapter 1The Electrokin
5、etic ConnectionMicroscopic Electrical ForcesThe Double LayerThe double layer model is used to visualizethe ionic environment in the vicinity of acharged colloid and explains how electricalrepulsive forces occur. It is easier to under-stand this model as a sequence of stepsthat would take place aroun
6、d a singlenegative colloid if the ions surrounding itwere suddenly stripped away.We first look at the effect of the colloid onthe positive ions, which are often calledcounter-ions. Initially, attraction from thenegative colloid causes some of the positiveions to form a firmly attached layer aroundth
7、e surface of the colloid. This layer ofcounter-ions is known as the Stern layer.Additional positive ions are still attracted bythe negative colloid but now they are re-pelled by the positive Stern layer as well asby other nearby positive ions that are alsotrying to approach the colloid. A dynamicequ
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