It is experimentally shown that the electrooptic properties of the ferroelectric phase of the new tungsten-bronze compositions can be treated as a biased quadratic electrooptic effect

. This is done by directly measuring the electrooptic behavior above the transition temperature in KSr
2Nb
5O
15. A term linear in electric field is not found. Thus the crystal has a center of inversion. We find

m
4/C
2. This value is very similar to that obtained for a number of compounds containing NbO
6and similar octahedra. This value is also in good agreement with the effective room-temperature linear electrooptic coefficient r
c, if it is assumed that r
ccan be considered to arise from a biased quadratic effect. Then we use these considerations systematically on other tungsten-bronze ferroelectrics, KSr
2Nb
5O
15, NaBa
2Nb
5O
15, Sr
0.25Ba
0.75Nb
2O
6, and Sr
0.5Ba
0.5Nb
2O
6. We calculate g
33and g
13separately and also find

m
4/C
2for all of these materials. Thus all these ferroelectrics give similar values to those found elsewhere for oxygen octahedra compounds. We also calculate values for the spontaneous polarization or the induced change in the indices of refraction.