2022
DOI: 10.1016/j.ceramint.2022.05.256
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Effect of Mn-doping on the morphological and electrical properties of (Ba0·7Sr0.3) (MnxTi1−x)O3 materials for energy storage application

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Cited by 16 publications
(4 citation statements)
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“…The average grain size, experimental densities (ρ m ), theoretical density (ρ th ), and relative densities (ρ r ) with content x are also displayed in Table 1. The ρ r is calculated using the following formula: 32 ρrbadbreak=ρmρrgoodbreak×100%,$$\begin{equation*} {\rho }_r = \frac{{{\rho }_m}}{{{\rho }_r}} \times 100\% ,\end{equation*}$$where ρ m is measured via the Archimedes drainage method, and ρ th is calculated according to the formula ρth=M×ZV×NA${\rho }_{th} = \frac{{M \times Z}}{{V \times {N}_A}} $ ( M , Z , V , and N A are the molecular mass, formula units per unit cell, the volume of the unit cell and Avogadro constant, respectively). All the samples show consistent structures with distinct grain boundaries and a compact microstructure (ρ r > 95%), which is advantageous for improving the energy storage properties.…”
Section: Resultsmentioning
confidence: 99%
“…The average grain size, experimental densities (ρ m ), theoretical density (ρ th ), and relative densities (ρ r ) with content x are also displayed in Table 1. The ρ r is calculated using the following formula: 32 ρrbadbreak=ρmρrgoodbreak×100%,$$\begin{equation*} {\rho }_r = \frac{{{\rho }_m}}{{{\rho }_r}} \times 100\% ,\end{equation*}$$where ρ m is measured via the Archimedes drainage method, and ρ th is calculated according to the formula ρth=M×ZV×NA${\rho }_{th} = \frac{{M \times Z}}{{V \times {N}_A}} $ ( M , Z , V , and N A are the molecular mass, formula units per unit cell, the volume of the unit cell and Avogadro constant, respectively). All the samples show consistent structures with distinct grain boundaries and a compact microstructure (ρ r > 95%), which is advantageous for improving the energy storage properties.…”
Section: Resultsmentioning
confidence: 99%
“…A specific amount of stored energy of such capacitor is consumed during the depolarization process, designated as energy loss density ( W loss ). [ 39 ] Introducing lower ZnO@APTES content in PVDF (30 vol%) increases recoverable energy storage density and the difference between W rec and W loss (Figure 11A). Capacitors with high efficiency should possess a sufficient difference between W rec and W loss , where W rec > W loss .…”
Section: Resultsmentioning
confidence: 99%
“…Also, its biocompatible and lead-free feature increased its investigation into dielectric, energy storage properties, and energy harvesting applications. [7,83,84] Another lead-free piezoelectric material is potassium sodium niobate (KNN). Its excellent piezoelectric coefficient (d 33 = 490 pC N À1 ) competes and easily substitutes PZT as a piezoelectric filler.…”
Section: Piezoelectric Fillersmentioning
confidence: 99%
“…Piezoelectric ceramic exhibits exceptional dielectric permittivity and piezoelectric coefficient. [7,8] However, the rigid and tough skeleton of ceramic inhibits the potential for easy fabrication into energy harvesting devices attributing to the absence of design flexibility. [9] Among the various piezoelectric materials, polyvinylidene fluoride (PVDF) is a flexible, biocompatible polymer with piezoelectric properties.…”
mentioning
confidence: 99%