2022
DOI: 10.3390/app122412692
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Geometrical Effect of Active Material on Electrode Tortuosity in All-Solid-State Lithium Battery

Abstract: In this study, the effect of the active material geometry on the tortuosity in the ion transport path of the electrode composite of an all-solid-state lithium battery was systematically analyzed in terms of the different design and process factors of an electrode. A direct current technique (i.e., chronoamperometry) using an electron-blocking cell was used to analyze the tortuosity to minimize the experimental error. In addition, aluminum oxide was selected as a hypothetical active material in a composite elec… Show more

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Cited by 8 publications
(2 citation statements)
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“…With the assumptions mentioned above, eq can be further simplified, yielding eq . In the simplified Bruggeman equation, the effective thermal conductivity κ eff is only a function of κ SE and ϕ SE , as follows κ eff = κ SE ϕ SE ( 1 + n ) / n = κ SE ϕ SE α If the pores are spherical in shape, n = 2, and an exponent of α = 1.5 is obtained. , While an exponent of 1.5 is the theoretical value for polydisperse, homogeneously distributed spheres, in battery materials, the exponent α = (1 + n )/ n is often used as a fitting parameter to cope with more complex pore microstructures, e.g., to describe the partial ionic conductivities of cathode composites , or thermal transport in solid electrolytes and batteries …”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…With the assumptions mentioned above, eq can be further simplified, yielding eq . In the simplified Bruggeman equation, the effective thermal conductivity κ eff is only a function of κ SE and ϕ SE , as follows κ eff = κ SE ϕ SE ( 1 + n ) / n = κ SE ϕ SE α If the pores are spherical in shape, n = 2, and an exponent of α = 1.5 is obtained. , While an exponent of 1.5 is the theoretical value for polydisperse, homogeneously distributed spheres, in battery materials, the exponent α = (1 + n )/ n is often used as a fitting parameter to cope with more complex pore microstructures, e.g., to describe the partial ionic conductivities of cathode composites , or thermal transport in solid electrolytes and batteries …”
Section: Resultsmentioning
confidence: 99%
“…If the pores are spherical in shape, n = 2, and an exponent of α = 1.5 is obtained. 45,47 While an exponent of 1.5 is the theoretical value for polydisperse, homogeneously distributed spheres, in battery materials, the exponent α = (1 + n)/n is often used as a fitting parameter to cope with more complex pore microstructures, e.g., to describe the partial ionic conductivities of cathode composites 27,50 or thermal transport in solid electrolytes 8 and batteries. 51 By using α to fit the measured relative density-dependent thermal conductivities, the scaling of the thermal conductivity of all materials with density (porosity) can be described with high accuracy (shown for room-temperature data, Figure 4).…”
Section: Characterization Of Thermal Transportmentioning
confidence: 99%