Pyroelectric charge in minerals develops on the opposite faces of asymmetric crystals. The direction in which the propagation of the charge tends toward is usually constant throughout a pyroelectric material, but in some materials this direction can be changed by a nearby electric field. These materials are said to exhibit ferroelectricity. All pyroelectric materials are also piezoelectric, the two properties being closely related.
Very small changes in temperature produce pyroelectric charge. Motion detection devices are often designed around pyroelectric materials, as the heat of a human or animal from several feet away is enough to generate a difference in charge.
Progress has been made in creating artificial pyroelectric materials, usually in the form of a thin film, out of gallium nitride (GaN), cesium nitrate (CsNO3), polyvinyl fluorides, derivatives of phenylpyrazine, and cobalt phthalocyanine.
The first reference to the pyroelectric effect is in writings by Theophrast in 314 BC, who noted that tourmaline becomes charged when heated. Sir David Brewster gave the effect the name it has today in 1824. Both William Thomson in 1878 and Voight in 1897 helped develop a theory for the processes behind pyroelectricity. Pierre Curie and his brother, Jacques, studied pyroelectricity in the 1880s, leading to their discovery of some of the mechanisms behind piezoelectricity. Pyroelectricity is definitely not a new concept, but research and application of the useful property continues to this day.
There are applications of Piezoelctric fibers in the active fiber reinforced composites that can be used as sensor and actuator also. These composites have been used in Rotor blade applications