Considering the characteristics of materials required for piezoelectric tra
nsformers, and introducing the maximum vibration velocity v(max) that gener
ates a fixed temperature rise, we can express the maximum output power of a
piezoelectric transformer as the product of this v(max)(2), the square of
the power coefficient on the output side A(2) and the load resistance R-L M
oreover, the power coefficient on the output side A(2) is proportional to t
he product of the square root of Young's modulus Y-E, the square root of th
e electromechanical coupling coefficient k, and the permittivity epsilon(33
) This is verified by using two types of piezoelectric transformers in an i
nverter where the output section may be of the Rosen type or the transverse
-effect type. It is shown that the contributions made by the structure of t
he piezoelectric transformer and the load resistance differ in each case. T
he Rosen structure is used in the piezoelectric transformer for the inverte
r, and it is shown that a material with large maximum vibration velocity v(
max) is useful in this case. (C) 1999 Scripta Technica, Electron Comm Jpn P
t 3, 82(11): 86-92, 1999.