Structural Health Monitoring Structural Health Monitoring Using Using PZT Impedance Measurements PZT Impedance Measurements
- M. D. Heibel
Structural Health Monitoring Structural Health Monitoring Using - - PowerPoint PPT Presentation
Structural Health Monitoring Structural Health Monitoring Using Using PZT Impedance Measurements PZT Impedance Measurements M. D. Heibel 4/19/2005 Structural Health Monitoring Using PZT Impedance Measurements Structural Health Monitoring
Principles of the Impedance Method
The constitutive relations for piezoelectric materials under small field condition are (Sirohi and Chopra 2000): where D (3x1) = electric displacement vector (C/m2), S (6x1) = strain vector, E (3x1) = applied external electric field vector (V/m), and T (6x1) = stress vector (N/m2), εij T = εij T (1−δj) (3x3) = complex dielectric permittivity at constant stress; dimd (3x6) and djkc (6x3) = matrices of the piezoelectric strain coefficients; and skmE = skmE (1−ηj) (6x6) = matrix of the complex elastic compliance at constant electric field. d denotes the dielectric loss factor and η the mechanical loss factor. The superscripts T and E indicate that the quantity has been measured at constant stress and constant electric field, respectively. The first subscript denotes the direction of the electric field and the second the direction of the associated mechanical strain. Commercially, the piezoelectric materials are available as ceramics, such as lead–zirconate–titanate (PZT) and polymers, such as polyvinvylidene fluoride.
(RMSD) compares differences between individual peaks (Park, et al, 2003)
to the baseline
the greater the change between curves