Showing posts with label Ferroelectrics. Show all posts
Showing posts with label Ferroelectrics. Show all posts

Tuesday, 25 March 2025

Examining the Electrothermal Effects in Ferroelectric Materials | Chapter 7 | Current Research Progress in Physical Science Vol. 5

Aims: The initial process of electric poling and the conditions of electrical boundaries significantly affect the physical properties of lead-zirconate-titanate (PZT) piezoelectric ceramics. This chapter explores electrothermal coupling in piezoelectrics and ferroelectrics, considering both static and dynamic thermodynamics. It highlights thermal differences in unpoled and poled PZT along the poling direction under open- and short-circuit conditions. To develop high power-density piezoelectrics, it is essential to understand thermal diffusivity to grasp the temperature profile of a high-voltage-driven specimen. Essentially, high thermal diffusivity is crucial for high-power piezoelectric materials.

 

Methodology: By examining the transient temperature profile at the "insulated side" of the disk sample, the thermal diffusivity \(\alpha_T\) can directly be measured by finding the time constant T experimentally from fitting the temperature profile \(\theta_0[1-e^{-t/\tau}]\) at x = L.

 

Results: The "secondary electrothermal" coupling factor \(k^\lambda\) is introduced, akin to the electromechanical coupling factor k, to account for why thermal diffusivity is greater under short-circuit conditions than open-circuit conditions. Conversely, the unpoled specimen shows the lowest thermal diffusivity. In a uniform ferroelectric specimen with a steady temperature distribution, equilibrium and dynamic phenomenology determine heat capacitance and specific heat capacity. On the other hand, spatially non-uniform (space-gradient) phenomenology leads to thermal diffusivity and conductivity.

 

Conclusion: The article confirms that heat flow analysis with an exponential trend over time, such as \((1-\theta/\theta_s)=e^{-t/\tau}\), is an approximation rather than an exact solution. The secondary electrothermal coupling factor \(k^\lambda\) is introduced, which appears to be significantly larger than the primary electrothermal coupling factor \(k^{{ET}^2}=\frac{p^2}{(C^E_p/T)\varepsilon_0\varepsilon^X}\). Finally, the dynamic heat generation profile in practical piezoelectric devices is analyzed and discussed to aid in the development of high-power piezoelectric devices.

 

Author (s) Details

Kenji Uchino
Department of Electrical Engineering, The Pennsylvania State University, University Park, PA 16802, USA.

 

Please see the book here:- https://doi.org/10.9734/bpi/crpps/v5/3176

Tuesday, 14 February 2023

Structural, Thermal and Surface Morphological Properties of Lead Based Perovskites| Chapter 6 | New Frontiers in Physical Science Research Vol. 7

 The brightest star-gel system was used to create tetragonal lead titanate porcelain nanoparticles. A solution of lead acetate and titanium isopropoxide was gelated in a financially sound system of intoxicating and acetyl acetone. The gel was fiery for 5 hours in a normal air kiln at 120oC to produce ceramic powder, that was then calcined for two hours at 600oC and sintered to 1100oC. The calcined and sintered powders were from thermal chemical analysis X-ray diffraction and Scanning energized matter microscopic reasoning.

Author(s) Details:

Anju Dixit,
Department of Physics, School of Basic Sciences, UIET, CSJM University Kanpur, India.

P. S. Dobal,
Department of Physics, VSSD College Kanpur, India.

Please see the link here: https://stm.bookpi.org/NFPSR-V7/article/view/9415