I I.I i IKK I 0ND1 « I l\ II \ . DIKKOI'I \ 



lion proceeds, therefore, the conducth it; 

 gressively increases, ;ni<l is a measure of th< 

 Applications of tin dissociation hypol in i>! 



explanation of such phei lena as tl 



during muscular, glandular, and nen i I i 



the application are nol as yel sufficiently understood I 



tempting to <h» more than indicate the 



problems are being im estigated. I 



currenl of action of muscle maj be explained in I 



hypothesis. To 'I" so we must delve a little further into pi ;• 



ical research, when we shall find thai th( 



cerning ionized molecules that musl I"- of import 



our problem. The firsl is thai th intribution which 



the equivalenl (or molecular conductivity o olution 

 of the other ion with which it is associated; ami th. 



differ « siderably in their conducting power. 3 



K , \'a.. ('|/, \< i ', carry charges of th.- Bame magnitude, • . 



not conduct t<> thr same degree, thej musl m< 



through the solution. We are driven, therefori 



exposed to the same electric force, different ions have diffi 



tics: that is to Bay, when an electric currenl p.isv.^ throuj 



an electrolyte, the positively charged ions mo 



differeni rate from thai at which the negativelj i 



towards the a !<■. Confirmation of this conclusion is 



ination of the concentration changes around th.- tw 

 electrolytic cell. The actual velocity ch ion • 



experimental means. 



•Thus Tar;: 

 same ratio a>. their chemical equivsh 



