Abstract

Using an in situ x-ray diffraction (XRD) technique, the electric-field induced change in the d-spacings Δd/d of the individual microcrystals or “crystallographic” strain is measured on lead magnesium niobate—lead titanate—barium titanate electrostrictive ceramics of composition 0.970(0.900PMN−0.100PT)−0.030BT from zero field to saturation. This crystallographic strain is then compared to the bulk longitudinal strain as measured by Δl/l using a photonic sensor. The crystallographic electric-field induced strain behavior for virgin samples could be fit to a constitutive model, where the induced strain is proportional to the square of the polarization with an electrostrictive coefficient Q determined to be 1.4 (×106 cm4/C2). Attempts to fit the bulk strain behavior on the same sample required lower values of the electrostrictive coefficient Q∼1, and generally yielded worse fits where the model predicted greater than the observed strain values at low electric fields. Subsequent in situ XRD measurements on previously electric-field cycled samples yielded much lower crystallographic strain values with a significantly different electric field dependence.

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