Ionic conductivity in polymer-salt electrolytes occurs in the amorphou
s regions of the complex. Poly(ethylene oxide) (PEO) is the best polye
ther for complexing salts. Unfortunately, it is partially crystalline
at ambient temperatures. With inorganic (i.e., alumina) or organic (i.
e., poly(acrylamide) (PAAM)) fillers the crystallization of PEO is inh
ibited and the room temperature conductivity is enhanced in these mixe
d phase systems by over two orders of magnitude (ro similar to 10(-4)
S/cm) above the base PEO-salt system (<10(-6) S/cm). Even adding PAAM
to an initially amorphous system (oxymethylene-linked PEO-LiClO4) incr
eases the room temperature conductivity by 2 to 3 times. Various alkal
i metal salts (Li, Na) and NH4SCN are used with alpha-Al2O3, theta-Al2
O3, PAAM' and poly(N,N'-dimethyl acrylamide) as filters. The aluminas
stiffen the complex and increase T-g. The addition of the organic fill
ers lowers T-g, as is to be preferred. It is suggested that changes in
thr conductivity with changes in salt and filler concentration ari du
e to changes in the ultrastructure and morphology and are the result o
f an equilibrium between various Lewis acid - Lewis base reactions. Qu
alified success has been achieved in modelling ionic conductivity in t
hese composite electrolyte systems using an effective medium approach.
In this approach it has been assumed that the main conductivity enhan
cement takes place in thin amorphous levers of the polyether that coat
the dispersed polyacrylamide particles separated in a microphase. In
the best complexes this layer Is identified by a second T-g.