A. Basili et al., Transference numbers of alkali chlorides and characterization of salt bridges for use in methanol plus water mixed solvents, J CHEM EN D, 44(5), 1999, pp. 1002-1008
Electromotive force measurements at 25 degrees C of the transference cells
Ag\AgCl\MeCl (m(2))\MeCl (m(1))\AgCl\Ag and MexHg1-x\MeCl (m(1))MeCl (m(1))
\Me,Hg1-x (where Me = Li, Na, K, and Rb and MexHg1-x denotes a flowing Me-a
malgam electrode at Me mole fraction x) have been made at various molalitie
s m(2) > m(1) (with m(1) fixed and m(2) varied) in methanol + water solvent
mixtures with methanol mass fractions w(m) up to 0.8. Supplementary emf me
asurements have been made of the cell Pt\LixHg1-x\LiCl (m(1))\AgCl\Ag\Pt to
obtain the required activity coefficients for LiCl at methanol mass fracti
ons w(M) = 0.2. The general trend of the ionic transference numbers of each
MeCl is a t degrees(Me+) increase with w(M), which is much more pronounced
for those Me+'s whose primary hydration sheaths are bigger (namely, Li+ an
d Na+). In particular, KCl becomes exactly equitransferent (t degrees(K+) =
t degrees(Cl-) = 0.5, i.e. an ideal salt bridge) at w(M) approximate to 0.
1, but at w(M) > 0.6 the KCl solubility becomes insufficient for a salt bri
dge function. The same drawback occurs also for RbCl, which is known to be
the most closely equitransferent salt in water (t degrees(Rb+). = 0.5007).
NaCl, which is quite unproposable as a salt bridge in water, may be useful
at high methanol concentrations, as its ionic transference numbers would ap
proach 0.5 at w(M) greater than or equal to 0.8.