Charged closed-cell polypropylene polymer foams are highly sensitive and br
oadband piezoelectric materials with a quasistatic piezoelectric d(33) coef
ficient about 250 pC/N and a dynamic d(33) coefficient of 140 pC/N at 600 k
Hz. The piezoelectric coefficient is much larger than that of ferroelectric
polymers, like polyvinylidene fluoride, and compares favorably with ferroe
lectric ceramics, such as lead zirconate titanate. The pyroelectric coeffic
ient p(3)=0.25 muC/m(2) K is small in comparison to ferroelectric polymers
and ferroelectric ceramics. The low density, small pyroelectric coefficient
and high piezoelectric sensitivity make charged polymer foams attractive f
or a wide range of sensor and transducer applications in acoustics, air-bor
ne ultrasound, medical diagnostics, and nondestructive testing. (C) 2001 Am
erican Institute of Physics.