A scaling law for distinct electrocaloric cooling performance in low-dimensional organic, relaxor and anti-ferroelectrics

Electrocaloric (EC) materials show promise in eco-friendly solid-state refrigeration and integrable on-chip thermal management. While direct measurement of EC thin-films still remains challenging, a generic theoretical framework for quantifying the cooling properties of rich EC materials including n...

Full description

Bibliographic Details
Main Authors: Shi, Y, Huang, L, Soh, A, Weng, G, Liu, S, Redfern, S
Format: Journal article
Language:English
Published: Springer Nature 2017
_version_ 1797070352195518464
author Shi, Y
Huang, L
Soh, A
Weng, G
Liu, S
Redfern, S
author_facet Shi, Y
Huang, L
Soh, A
Weng, G
Liu, S
Redfern, S
author_sort Shi, Y
collection OXFORD
description Electrocaloric (EC) materials show promise in eco-friendly solid-state refrigeration and integrable on-chip thermal management. While direct measurement of EC thin-films still remains challenging, a generic theoretical framework for quantifying the cooling properties of rich EC materials including normal-, relaxor-, organic- and anti-ferroelectrics is imperative for exploiting new flexible and room-temperature cooling alternatives. Here, we present a versatile theory that combines Master equation with Maxwell relations and analytically relates the macroscopic cooling responses in EC materials with the intrinsic diffuseness of phase transitions and correlation characteristics. Under increased electric fields, both EC entropy and adiabatic temperature changes increase quadratically initially, followed by further linear growth and eventual gradual saturation. The upper bound of entropy change (∆Smax) is limited by distinct correlation volumes (V cr ) and transition diffuseness. The linearity between V cr and the transition diffuseness is emphasized, while ∆Smax = 300 kJ/(K.m3) is obtained for Pb0.8Ba0.2ZrO3. The ∆Smax in antiferroelectric Pb0.95Zr0.05TiO3, Pb0.8Ba0.2ZrO3 and polymeric ferroelectrics scales proportionally with V cr −2.2, owing to the one-dimensional structural constraint on lattice-scale depolarization dynamics; whereas ∆Smax in relaxor and normal ferroelectrics scales as ∆Smax ~ V cr −0.37, which tallies with a dipolar interaction exponent of 2/3 in EC materials and the well-proven fractional dimensionality of 2.5 for ferroelectric domain walls.
first_indexed 2024-03-06T22:37:36Z
format Journal article
id oxford-uuid:5a709f0a-e7ef-4cab-876f-3657063cc1e9
institution University of Oxford
language English
last_indexed 2024-03-06T22:37:36Z
publishDate 2017
publisher Springer Nature
record_format dspace
spelling oxford-uuid:5a709f0a-e7ef-4cab-876f-3657063cc1e92022-03-26T17:15:47ZA scaling law for distinct electrocaloric cooling performance in low-dimensional organic, relaxor and anti-ferroelectricsJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:5a709f0a-e7ef-4cab-876f-3657063cc1e9EnglishSymplectic Elements at OxfordSpringer Nature2017Shi, YHuang, LSoh, AWeng, GLiu, SRedfern, SElectrocaloric (EC) materials show promise in eco-friendly solid-state refrigeration and integrable on-chip thermal management. While direct measurement of EC thin-films still remains challenging, a generic theoretical framework for quantifying the cooling properties of rich EC materials including normal-, relaxor-, organic- and anti-ferroelectrics is imperative for exploiting new flexible and room-temperature cooling alternatives. Here, we present a versatile theory that combines Master equation with Maxwell relations and analytically relates the macroscopic cooling responses in EC materials with the intrinsic diffuseness of phase transitions and correlation characteristics. Under increased electric fields, both EC entropy and adiabatic temperature changes increase quadratically initially, followed by further linear growth and eventual gradual saturation. The upper bound of entropy change (∆Smax) is limited by distinct correlation volumes (V cr ) and transition diffuseness. The linearity between V cr and the transition diffuseness is emphasized, while ∆Smax = 300 kJ/(K.m3) is obtained for Pb0.8Ba0.2ZrO3. The ∆Smax in antiferroelectric Pb0.95Zr0.05TiO3, Pb0.8Ba0.2ZrO3 and polymeric ferroelectrics scales proportionally with V cr −2.2, owing to the one-dimensional structural constraint on lattice-scale depolarization dynamics; whereas ∆Smax in relaxor and normal ferroelectrics scales as ∆Smax ~ V cr −0.37, which tallies with a dipolar interaction exponent of 2/3 in EC materials and the well-proven fractional dimensionality of 2.5 for ferroelectric domain walls.
spellingShingle Shi, Y
Huang, L
Soh, A
Weng, G
Liu, S
Redfern, S
A scaling law for distinct electrocaloric cooling performance in low-dimensional organic, relaxor and anti-ferroelectrics
title A scaling law for distinct electrocaloric cooling performance in low-dimensional organic, relaxor and anti-ferroelectrics
title_full A scaling law for distinct electrocaloric cooling performance in low-dimensional organic, relaxor and anti-ferroelectrics
title_fullStr A scaling law for distinct electrocaloric cooling performance in low-dimensional organic, relaxor and anti-ferroelectrics
title_full_unstemmed A scaling law for distinct electrocaloric cooling performance in low-dimensional organic, relaxor and anti-ferroelectrics
title_short A scaling law for distinct electrocaloric cooling performance in low-dimensional organic, relaxor and anti-ferroelectrics
title_sort scaling law for distinct electrocaloric cooling performance in low dimensional organic relaxor and anti ferroelectrics
work_keys_str_mv AT shiy ascalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT huangl ascalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT soha ascalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT wengg ascalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT lius ascalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT redferns ascalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT shiy scalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT huangl scalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT soha scalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT wengg scalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT lius scalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics
AT redferns scalinglawfordistinctelectrocaloriccoolingperformanceinlowdimensionalorganicrelaxorandantiferroelectrics