RLECTRIC < ONDl I 1 i\ ll V. I) 17 



being however uniformly distributed tl 

 thai ili«' negath e charges of the anioi 

 charges of the cations. The electric curr< 

 conic cluii <n'd, the one positively, the oth< 

 tive force is exerted on the ions of oppoe t< 

 lively charged ions to migrate towards the i> 

 positively charged, towards the negativi 

 of t 1m- ions thai endows the solution with conducti 



In water, or in a solution of a nonelectrolyte, moli 1 1 1 1 •• non- 



electrolyte exisl thus: 



II II II 



II II II <» 



II II H,0 



In a solution of an electrolyte, the molecules split into ions I 



\a CI- Na CI Na CI- 

 \a el Na CI- Na CI- 



\a CI \- CI- Na CI- 



When an electric currenl passes through a solution 

 tin- ions tend i<» arrange themselves tl 



It follows from the above considerations tl 

 stanct in solution will <l> i>> ml on tfu </• 

 tion. Furthermore, if v. ime thai in 



phenomena are concerned, each ion behaves in thi 

 cule, tlifii it follows thai the electrical nal 



tn tl jctenl to w liicli the ■ »-- 1 n < > t 



peel it to I"' from the amounl <>f substance actual! 



In the Determination of the Conductiviu 

 use Btandard conditions of depth and width i 

 currenl is passed, and t<> ha\ •• bod 

 is thru know n i u 

 being the conducth it; 

 centimeter cube, w ould ofl 

 sides of the cube actii 



