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首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Effect of crystallographic structure of MnO2 on its electrochemical capacitance properties
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Effect of crystallographic structure of MnO2 on its electrochemical capacitance properties

机译:MnO2的晶体结构对其电化学电容性能的影响

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摘要

MnO2 is currently under extensive investigations for its capacitance properties. MnO2 crystallizes into several crystallographic structures, namely, alpha, beta, gamma, delta, and lambda structures. Because these structures differ in the way MnO6 octahedra are interlinked, they possess tunnels or interlayers with gaps of different magnitudes. Because capacitance properties are due to intercalation/deintercalation of protons or cations in MnO2, only some crystallographic structures, which possess sufficient gaps to accommodate these ions, are expected to be useful for capacitance studies. In order to examine the dependence of capacitance on crystal structure, the present study involves preparation of these various crystal phases of MnO2 in nanodimensions and to evaluate their capacitance properties. Results of alpha-MnO2 prepared by a microemulsion route (alpha-MnO2(m)) are also used for comparison. Spherical particles of about 50 nm, nanorods of 30-50 nm in diameter, or interlocked fibers of 10-20 nm in diameters are formed, which depend on the crystal structure and the method of preparation. The specific capacitance (SC) measured for MnO2 is found to depend strongly on the crystallographic structure, and it decreases in the following order: alpha(m) > alpha congruent to 6 > gamma > lambda > beta. A SC value of 297 F g(-1) is obtained for alpha-MnO2(m), whereas it is 9 F g(-1) for beta-MnO2. A wide (-similar to 4.6 angstrom) tunnel size and large surface area of alpha-MnO2(m) are ascribed as favorable factors for its high SC. A large interlayer separation (similar to 7 angstrom) also facilitates insertion of cations in delta-MnO2 resulting in a SC close to 236 F g(-1). A narrow tunnel size (1.89 A) does not allow intercalation of cations into beta-MnO2. As a result, it provides a very small SC.
机译:MnO2的电容特性目前正在广泛研究中。 MnO2结晶成几种晶体结构,即α,β,γ,δ和λ结构。由于这些结构在MnO6八面体的互连方式上不同,因此它们具有隧道或夹层,其间隙大小不同。因为电容特性是由于MnO2中质子或阳离子的嵌入/去嵌入所致,所以只有一些具有足够间隙来容纳这些离子的晶体结构才有望用于电容研究。为了检查电容对晶体结构的依赖性,本研究涉及制备纳米尺寸的MnO2的这些不同晶体相并评估其电容特性。通过微乳化途径制备的α-MnO2的结果(α-MnO2(m))也用于比较。取决于晶体结构和制备方法,形成约50nm的球形颗粒,直径为30-50nm的纳米棒或直径为10-20nm的互锁纤维。发现对MnO2测得的比电容(SC)在很大程度上取决于晶体结构,并且按以下顺序减小:α(m)>α等于6>γ>λ>β。对于α-MnO2(m),SC值为297 F g(-1),而对于β-MnO2,SC值为9 F g(-1)。 α-MnO2(m)的宽(类似于4.6埃)隧道尺寸和大表面积被认为是其高SC的有利因素。较大的层间间距(类似于7埃)还有助于在δ-MnO2中插入阳离子,从而导致SC接近236 F g(-1)。狭窄的隧道尺寸(1.89 A)不允许将阳离子嵌入β-MnO2中。结果,它提供了非常小的SC。

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