2021
DOI: 10.1002/celc.202100454
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Extreme Rate Capability Cycling of Porous Silicon Composite Anodes for Lithium‐Ion Batteries

Abstract: Silicon‐based anodes have the potential to increase the capacity of lithium‐ion batteries but suffer from irreversible damage due to their volume expansion. Capacity‐controlled cycling has emerged as a promising method for silicon‐based anodes; however, few studies have evaluated how high C‐rates affect cycle life under capacity‐controlled cycling. Here, we examine how a repetitive cycling at high C‐rates and long cycle numbers affects the electrochemical performance. This extreme rate capability test (cycling… Show more

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Cited by 4 publications
(4 citation statements)
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“…The reduction peak at 0.01 V during the first cycle is observed, which is due to the conversion of crystalline silicon to amorphous silicon. In the second cycle, two reduction peaks at 0.01 and 0.15 V correspond to the formation of Li-Si alloy, and two oxidation peak at 0.35 and 0.53 V are assigned to dealloying process of the Li-Si alloy [21][22][23] . In addition, the rate performances of the half-cells of PP-10 μm-LLZTO and bare PP separators are compared (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…The reduction peak at 0.01 V during the first cycle is observed, which is due to the conversion of crystalline silicon to amorphous silicon. In the second cycle, two reduction peaks at 0.01 and 0.15 V correspond to the formation of Li-Si alloy, and two oxidation peak at 0.35 and 0.53 V are assigned to dealloying process of the Li-Si alloy [21][22][23] . In addition, the rate performances of the half-cells of PP-10 μm-LLZTO and bare PP separators are compared (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Galvanostatic intermittent titration technique (GITT) and cyclic voltammetry (CV) tests were performed on prelithiated and control Si/PPAN half-cells after 3 formation cycles at 0.15 A g –1 , with Li metal as the reference and counter electrodes. For GITT, each current pulse (0.15 A g –1 ) was applied for 360 s, followed by a relaxation for 4500 s during lithiation and delithiation between 0.01 and 1 V. The amount of Li alloying with Si was calculated for each current pulse by applying eq , normalΔ δ = M normalB italiczF m normalB I τ where M B is the atomic weight of Si (g mol –1 ), z is the valence of mobile species (Li + ), F is the Faraday’s constant (A s mol –1 ), m B is the mass of Si in the electrode (g), I is the current applied (A), and τ is the pulse duration (s). The apparent diffusion coefficient of Li was also calculated by eq , D normalL normali + = 4 π τ true( m normalB V normalm M normalB A true) 2 true( normalΔ E normals normalΔ E τ true) 2 where D is the diffusion coefficient (cm 2 s –1 ), V m is the molar volume (cm 3 mol –1 ), A is the electrode area (cm 2 ), Δ E s is the change in steady state voltage, and Δ E τ is the change in transit voltage during pulse without Ohmic drop.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…For GITT, each current pulse (0.15 A g –1 ) was applied for 360 s, followed by a relaxation for 4500 s during lithiation and delithiation between 0.01 and 1 V. The amount of Li alloying with Si was calculated for each current pulse by applying eq , where M B is the atomic weight of Si (g mol –1 ), z is the valence of mobile species (Li + ), F is the Faraday’s constant (A s mol –1 ), m B is the mass of Si in the electrode (g), I is the current applied (A), and τ is the pulse duration (s). The apparent diffusion coefficient of Li was also calculated by eq , where D is the diffusion coefficient (cm 2 s –1 ), V m is the molar volume (cm 3 mol –1 ), A is the electrode area (cm 2 ), Δ E s is the change in steady state voltage, and Δ E τ is the change in transit voltage during pulse without Ohmic drop.…”
Section: Experimental Methodsmentioning
confidence: 99%
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