Revisiting the blocking force test on ferroelectric ceramics using high energy x-ray diffraction

The blocking force test is a standard test to characterise the properties of piezoelectric actuators. The aim of this study is to understand the various contributions to the macroscopic behaviour observed during this experiment that involves the intrinsic piezoelectric effect, ferroelectric domain switching, and internal stress development. For this purpose, a high energy diffraction experiment is performed in-situ during a blocking force test on a tetragonal lead zirconate titanate (PZT) ceramic (Pb0.98Ba0.01(Zr0.51Ti0.49)0.98Nb0.02O3). It is shown that the usual macroscopic linear interpretation of the test can also be performed at the single crystal scale, allowing the identification of local apparent piezoelectric and elastic properties. It is also shown that despite this apparent linearity, the blocking force test involves significant non-linear behaviour mostly due to domain switching under electric field and stress. Although affecting a limited volume fraction of the material, domain switching is responsible for a large part of the macroscopic strain and explains the high level of inter- and intra-granular stresses observed during the course of the experiment. The study shows that if apparent piezoelectric and elastic properties can be identified for PZT single crystals from blocking stress curves, they may be very different from the actual properties of polycrystalline materials due to the multiplicity of the physical mechanisms involved. These apparent properties can be used for macroscopic modelling purposes but should be considered with caution if a local analysis is aimed at.

[1]  J. Koruza,et al.  Determination of the True Operational Range of a Piezoelectric Actuator , 2014 .

[2]  P. Withers,et al.  Identification of crystalline elastic anisotropy in PZT ceramics from in-situ blocking stress measurements , 2014 .

[3]  J. Rödel,et al.  Simultaneous Enhancement of Fracture Toughness and Unipolar Strain in Pb(Zr,Ti)O3‐ZrO2 Composites Through Composition Adjustment , 2014 .

[4]  P. Withers,et al.  A multiscale model for reversible ferroelectric behaviour of polycrystalline ceramics , 2014 .

[5]  Jacob L. Jones,et al.  Nonlinear stress-strain behavior and stress-induced phase transitions in soft Pb(Zr1−xTix)O3at the morphotropic phase boundary , 2013 .

[6]  X. Tan,et al.  Optimal working regime of lead–zirconate–titanate for actuation applications , 2013 .

[7]  Jiadong Zang,et al.  Giant electric-field-induced strains in lead-free ceramics for actuator applications – status and perspective , 2012, Journal of Electroceramics.

[8]  M. Kosec,et al.  Compositional Dependence of R-curve Behavior in Soft Pb(Zr1−xTix)O3 Ceramics , 2011 .

[9]  Jacob L. Jones,et al.  Origins of Electro‐Mechanical Coupling in Polycrystalline Ferroelectrics During Subcoercive Electrical Loading , 2011 .

[10]  J. Rödel,et al.  High temperature blocking force measurements of soft lead zirconate titanate , 2010 .

[11]  Jacob L. Jones,et al.  Electric-field-induced phase-change behavior in (Bi0.5Na0.5)TiO3-BaTiO3-(K0.5Na0.5)NbO3: A combinatorial investigation , 2010 .

[12]  E. Bourhis,et al.  In situ diffraction strain analysis of elastically deformed polycrystalline thin films, and micromechanical interpretation , 2009 .

[13]  Jacob L. Jones,et al.  Subcoercive Cyclic Electrical Loading of Lead Zirconate Titanate Ceramics II: Time-Resolved X-Ray Diffraction , 2009 .

[14]  L. Daniel,et al.  Generic formalism for homogenization of coupled behavior: Application to magnetoelectroelastic behavior , 2008 .

[15]  A. Safari,et al.  Piezoelectric and Acoustic Materials for Transducer Applications , 2008 .

[16]  Ragini,et al.  Origin of high piezoelectric response of Pb(ZrxTi1-x)O3 at the morphotropic phase boundary : Role of elastic instability , 2008, 0803.1968.

[17]  H. Kungl,et al.  In situ synchrotron diffraction investigation of morphotropic Pb[Zr1- xTix]O3 under an applied electric field , 2007 .

[18]  Jacob L. Jones,et al.  Texture and Anisotropy of Polycrystalline Piezoelectrics , 2007 .

[19]  Jacob L. Jones,et al.  Time-resolved diffraction measurements of electric-field-induced strain in tetragonal lead zirconate titanate , 2007 .

[20]  A. Steuwer,et al.  Analysis of elastic strain and crystallographic texture in poled rhombohedral PZT ceramics , 2006 .

[21]  A. Steuwer,et al.  Micromechanics of residual stress and texture development due to poling in polycrystalline ferroelectric ceramics , 2005 .

[22]  Jacob L. Jones,et al.  Domain texture distributions in tetragonal lead zirconate titanate by x-ray and neutron diffraction , 2005 .

[23]  M. Daymond The determination of a continuum mechanics equivalent elastic strain from the analysis of multiple diffraction peaks , 2004 .

[24]  A. Steuwer,et al.  A high energy synchrotron x-ray study of crystallographic texture and lattice strain in soft lead zirconate titanate ceramics , 2004 .

[25]  Dragan Damjanovic,et al.  FERROELECTRIC, DIELECTRIC AND PIEZOELECTRIC PROPERTIES OF FERROELECTRIC THIN FILMS AND CERAMICS , 1998 .

[26]  A. P. Hammersley,et al.  Two-dimensional detector software: From real detector to idealised image or two-theta scan , 1996 .