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ORNL-2106 - the Molten Salt Energy Technologies Web Site

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ANP PROJECT PROGRESS REPORT<br />

<strong>the</strong> AgCI at <strong>the</strong> end was<br />

(1) N + m + mNt;l, - Nt;, ,<br />

where m is <strong>the</strong> AgCI in one mole at <strong>the</strong> start and<br />

N is <strong>the</strong> AgCl from <strong>the</strong> electrode reaction. If m and<br />

N are subtracted from expression 1 and <strong>the</strong> remainder<br />

is divided by N, <strong>the</strong> relative transference<br />

of Ag' is seen to be<br />

(2)<br />

ti, = ti, - mtLa .<br />

By a similar argument it may be seen that<br />

(3)<br />

tEl = 1 - rig .<br />

These relative transference numbers are all that<br />

can be obtained unambiguously from <strong>the</strong> Hittorf<br />

experiment, in which N faradays of electricity are<br />

passed, <strong>the</strong> electrode compartments are analyzed,<br />

and <strong>the</strong> AgCI content of <strong>the</strong> electrode compartment<br />

is compared with that initially present in <strong>the</strong> same<br />

amount of NaCI. They are also <strong>the</strong> only numbers<br />

needed for <strong>the</strong>rmodynamic use.<br />

Useful correlations of <strong>the</strong> relative transference<br />

numbers with electric conductance may also be<br />

made. For <strong>the</strong>se carelations, X (<strong>the</strong> ionic conductance)<br />

is defined so that, for pure NaCI,<br />

XNo + XcI = dC, where K is <strong>the</strong> specific conductance<br />

and C is <strong>the</strong> concentration in equivalents<br />

per cubic centimeter. For <strong>the</strong> NaCI-ASCI mixture,<br />

';la =<br />

= cNaXNa -+ 'Ag'Ag + CClhCl *<br />

cNaXNa<br />

K<br />

'A gXA g<br />

. K<br />

*<br />

,<br />

and, when <strong>the</strong>se values are substituted in Eq. 2,<br />

it may be seen that<br />

110<br />

'Ag - 'No<br />

= 'Ag K<br />

ern<br />

'Ag - 'No<br />

K'CNa<br />

From Eq. 4 it is evident that <strong>the</strong> relative transfer<br />

of <strong>the</strong> silver ion is proportional to <strong>the</strong> concentration<br />

of <strong>the</strong> silver ion and to <strong>the</strong> difference in <strong>the</strong><br />

mobilities of Ag+ and of No', and hence <strong>the</strong> relative<br />

transfer may be ei<strong>the</strong>r positive or negative. If<br />

it is negative, tk, will be greater than unity.<br />

For application to a concentration cell with<br />

transference, consider <strong>the</strong> cell<br />

Ag, AgCl in . . AgCI in NaCI,<br />

NaCI; mA mole . Ag; mB mole<br />

AgCl/mole NaCl : . Ag/mole NaCl<br />

t' t'+dt'<br />

At <strong>the</strong> cathode <strong>the</strong> opposite processes occur, with<br />

each A replaced by B. In <strong>the</strong> section with a con-<br />

centration gradient between A and B, in each<br />

element, such as between <strong>the</strong> dotted lines, <strong>the</strong><br />

gain of AgCl is ti and <strong>the</strong> loss is tig + dtig,<br />

which gives a net foss of dtig mole AgCI in <strong>the</strong><br />

element, and<br />

If tr is constant this simplifies to<br />

however, as shown in Eq. 4, t' is not expected to<br />

be constant.<br />

.<br />

.<br />

t

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