MnO2/煤基碳纳米纤维的制备及其在柔性超级电容器中的应用

采用静电纺丝技术制备了柔性煤基碳纳米纤维(CBCNFs)。利用低温等离子体技术对CBCNFs进行改性,并将改性后的CBCNFs作为还原剂与KMn O4反应,以实现Mn O2的原位还原负载制备CBCNFs/Mn O2复合材料。通过X射线衍射、扫描电镜和透射电镜等手段对复合材料的结构与形貌进行了表征;另外,研究了其作为柔性超级电容器电极材料的性能。结果表明,KMn O4∶CBCNFs=2∶1(质量比)条件下制备的复合材料(CBCNFs/Mn O2-2)具有良好的电化学性能。在0.1A·g-1电流密度下,CBCNFs/Mn O2-2的比电容高达118F·g-1,为CBCNFs比电容(26F·g-1)的4.5倍,在1A·g-1电流密度下,循环1000次后比容量保持率为97%,表现出良好的循环稳定性。     

有序介孔碳负载NiCo2O4电极的制备及其超电容性能

以有序介孔碳(OMC)为载体,采用共沉淀法制备了OMC/NiCo2O4复合物.用X射线衍射(XRD)、傅里叶变换红外(FT-IR)光谱和透射电镜(TEM)研究其结构与形貌,发现NiCo2O4纳米颗粒均匀地负载在有序介孔碳上.循环伏安和恒流充放电测试表明,NiCo2O4质量分数为40%时,在1A·g-1的电流密度下,复合物电极的比电容可以达到577.0F·g-1,电流密度为8A·g-1时,比电容可以达到470.8F·g-1,并具有良好的循环稳定性.在2A·g-1的电流密度下,经过2000次循环后,比电容还可达到508.4F·g-1,电容保持率为92.7%.     

负载Cr_2O_3的H_2Ti_2O_5·H_2O纳米管的制备及其作为锂离子电池正极材料的电化学性能

限制纳米电极材料倍率性能的一个重要因素是,在大电流下充放电时,纳米结构可能坍塌,造成容量迅速衰减.通过异价离子的掺杂或第二相的负载有可能弥补纳米材料的这一缺陷.本文以含有Cr2O3的锐钛矿TiO2为原料,通过超声化学-水热法,制备了负载Cr2O3的H2Ti2O5·H2O纳米管.采用X射线衍射(XRD)和透射电镜(TEM)对制得的H2Ti2O5·H2O/Cr2O3纳米管的晶体结构和微观形貌进行了表征和分析.恒流充放电测试显示,H2Ti2O5·H2O/Cr2O3(5%(w,质量分数))纳米管作为锂离子电池阳极材料具有优异的循环稳定性及倍率性能.在150mA·g-1的电流密度下,H2Ti2O5·H2O/Cr2O3纳米管的首次放电容量达到288mAh·g-1;120次循环后,充放电容量仍保持在145mAh·g-1.在1500mA·g-1的电流密度下,首次放电容量为178mAh·g-1;600次循环后,充放电容量保持在80mAh·g-1以上;继续在150mA·g-1电流密度下充放电30个循环,充放电容量达到155mAh·g-1,显示出充放电容量的可回复性.循环伏安测试结果表明,H2Ti2O5·H2O/Cr2O3纳米管的充放电过程由法拉第赝电容反应控制.该一维纳米结构在锂离子电池和非对称电容器领域显示出良好的应用前景.     

薄层晶状α-MnO_2/活性炭复合电极材料的制备和电化学性质

以自制活性炭(AC)为载体,(NH4)2S2O8为氧化剂、MnSO4为还原剂和锰源、(NH4)2SO4为模板试剂,通过原位水热沉积法制备了α-MnO2/AC系列复合电极材料.分别采用X射线衍射、扫描电子显微镜、N2吸附/脱附等方法对试样的晶型结构、形貌、比表面积和孔结构进行了表征;用循环伏安、恒流充放电和交流阻抗等电化学方法研究了材料的电化学性质.结果表明,在MnSO4浓度为0.075mol·L-1的水热条件下,获得了薄层晶状α-MnO2/AC复合材料.在电流密度为3mA·cm-2时,该材料电化学性能优异,比电容为374.5F·g-1,较沉积前AC的252.7F·g-1有显著提高,增幅为48.2%;α-MnO2/AC复合电极有良好的充放电特性和循环稳定性,经1000次恒流充放电测试,容量保持率达到95%。     

活性炭基Li2SO4水系电解液超级电容器

采用中性Li2SO4水溶液代替H2SO4和KOH作为电解液制备了活性炭(AC)基对称型超级电容器,使水系超级电容器的工作电压由1.0V提高到了1.6V.采用循环伏安和充放电测试研究了电容器的稳定电化学窗口.电化学充放电测试表明电容器在0.25A.g-1电流密度下单电极比容量可达129F.g-1,在功率密度为160W.kg-1时能量密度达到10Wh.kg-1(以正负极活性物质的总质量计).1.6V恒压充电1h后电容器漏电流为0.22mA.超级电容器的库仑效率接近100%,充放电循环5000次后容量仍可保持在92%以上.研究了电解液的浓度对电容器电化学性能的影响,发现随着Li2SO4浓度的增大电容器的电荷转移电阻显著减小,大电流充放电性能提高.活性炭基Li2SO4水系电解液超级电容器具有工作电压高、能量密度高和对环境友好等优点,因此有很好的产业化前景.     

混合超级电容器AC/LiMn2O4体系的电化学性能

对AC/LiMnO4体系混合电容器进行研究,以活性炭(AC)为负极材料,尖晶石结构的LiMn2O4为正极材料,Li2SO4为电解液。该体系的原理与锂离子电池很相似,从本质上说属于一种特殊的锂离子电池。改变正负极的质量配比,根据其电化学性能确定了该体系最佳的正负极质量配比。对不同电解液浓度的电容器进行不同电流密度充放电测试,发现电解液浓度增加,会使容量和大电流性能得到明显改善,极化电阻的增大会大大降低放电电压平台。实验表明该体系具有较高的能量密度和功率密度,同时保持了良好的循环性能。     

一种活性炭比容量的测试

本文采用三电极有机锂盐体系对一种性炭(AC)的比容量进行测试、分析,发现在活性炭对称电容器中,正极活性炭的双电层容量为79.24F/g,活性炭做负极时,在不同的电位下表现出不同的容量性质,在较低电位下活性炭比容量为61.85F/g,而较高的电位比容量为96.54F/g.在对比活性炭对称电容器体系和AC/Li4Ti5O12、 LiMn2O4/AC两种不对称电容器体系,发现AC/Li4Ti5O12、LiMn2O4/AC不对称电容器测试出来的活性炭比容量比活性炭对称电容器的测试出来比容量提高约9.6%～17.8%不等.     

导电氧化物AZO对尖晶石型LiMn_2O_4高温性能的改善及研究

采用溶胶凝胶法对尖晶石型LiMn2O4正极材料进行铝掺杂氧化锌(AZO)包覆改性,并通过XRD、SEM、EDS、TEM、EIS、ICP-AES和充放电测试等手段对其结构,形貌及电化学性能进行表征。研究结果表明,AZO包覆层有效的阻止了LiMn2O4颗粒和电解液的直接接触,抑制了高温下锰溶解,明显改善了LiMn2O4的高温循环性能。1.5wt%AZO包覆的LiMn2O4正极材料在高温(55℃)1C时,首次放电比容量为114 mAh·g-1,经过100次循环后,容量保持率仍高达95.4%,远高于未包覆LiMn2O4的70.6%。此外,1.5wt%AZO包覆的LiMn2O4表现出了优越的大倍率放电性能,在10C下放电比容量能达到99 mAh·g-1。     

空心六边形镍钴硫化物/RGO复合物的合成及其超级电容性能

通过两步法制备了一种空心六边形镍钴硫化物(HHNCS)与还原氧化石墨烯(RGO)的纳米复合材料HHNCS/RGO。利用XRD,SEM,TEM和Raman光谱等对复合物进行表征,发现镍钴硫化物为空心六边形结构,并且均匀地附着在RGO的表面。该纳米复合物用作超级电容器电极表现出优异的电化学性能。在电流密度为1 A·g-1时比电容为927 F·g-1;当电流密度增大到20 A·g-1时,比电容仍高达724 F·g-1,表明材料拥有较好的倍率性能。此外,在电流密度5 A·g-1下循环2 000次后比电容保留有初始值的93%,显示出优异的循环稳定性。HHNCS/RGO优异的电容性能主要是由于RGO的存在不仅增强了材料的导电性,而且作为理想的载体分散HHNCS纳米片。HHNCS/RGO纳米复合物优异的电化学性能使其在超级电容器电极材料领域具有应用前景。     

碳包覆球形LiMn2O4的固相合成及电化学性能

以MnSO4为原料,采用溶液结晶法先制备球形MnO2。以所制得的MnO2和LiOH·H2O为原料,采用高温固相法制备了球形LiMn2O4粉体材料。将间苯二酚和甲醛按1:2的摩尔比均匀混合继续搅拌1h,在85℃下干燥后,球磨2h,得到橘红色碳凝胶粉末。以80:20的质量比将所制得的球形LiMn2O4和碳凝胶混合后,在550℃下烧结6h,得到碳包覆的球形LiMn2O4颗粒。从XRD结果可以看出,包覆碳前后的LiMn2O4结晶程度较好,没有杂质峰出现。在2?=18.76,36.28,44.17,58.36,64.14°分别出现对应于(111),(311),(400),(511),(440)晶面的衍射峰,可归属为单一的尖晶石结构。由于裂解碳属于无定型态并且含量较少,因此在XRD图谱中观察不出其衍射峰。但从图中可以看出,碳的存在并不影响尖晶石LiMn2O4的晶体结构。从SEM图像中可以看,球形颗粒的表面有一层致密的碳包覆层。EDX检测得出,锰、氧和碳含量分别为66.68%、26.9%、6.42%。组装的电池采用锂片作为负极,电解液为1mol·L-1 LiFP6/EC DEC(1:1体积比)。恒流充放电测试在3.2～4.4V范围内进行:以0.5C的电流密度,碳包覆球形LiMn2O4电极在25℃和55℃温度下首次放电容量分别为122 mAh·g-1和115 mAh·g-1,而未包覆的电极其对应的首次放电容量分别为119 mAh·g-1和112 mAh·g-1。同时测评两种电池的循环性能,25℃下碳包覆和未包覆电极循环100次后容量分别为111 mAh·g-1,102 mAh·g-1,容量保持率为91%和86%;55℃下,循环50次后容量衰减率分别为0.3%和0.5%。由此可见,碳包覆LiMn2O4材料的放电及循环性能都优于未包覆材料,可归结于以下原因:裂解的无定形碳提高了电极材料的电子电导率,增强了离子在电极表面的传递速度,两种协同作用使得含有少量碳的电极材料可以充放电完全,库仑效率较高,循环过程中减小电极表面的极化;在高温环境下,LiMn2O4电极容量衰减主要是由于电解液中含氟电解质电离出F-所形成的HF对电极具有强的腐蚀性。采用包覆的方法,在球形颗粒表面形成的碳层可以减少活性物质在电解液中的裸露面积从而减少其对电极的侵蚀,提高电池的循环寿命;另外,碳保护层可以使活性物质颗粒保持良好的接触,循环多次后仍能保持较高容量。利用交流阻抗技术及renew软件对所得阻抗谱进行拟合,可以得出包覆与未包覆的两种电极的电荷转移电阻为16.28O和45.02O。由此表明,碳包覆层增强了Li 在电极表面的脱嵌能力,抑制了Jahn-Teller效应以及电化学极化。     

Sc2MgGa2 and Y2MgGa2

Scandium magnesium gallide, Sc₂MgGa₂, and yttrium magnesium gallide, Y₂MgGa₂, were synthesized from the corresponding elements by heating under an argon atmosphere in an induction furnace. These intermetallic compounds crystallize in the tetragonal Mo₂FeB₂‐type structure. All three crystallographically unique atoms occupy special positions and the site symmetries of (Sc/Y, Ga) and Mg are m2m and 4/m, respectively. The coordinations around Sc/Y, Mg and Ga are pentagonal (Sc/Y), tetragonal (Mg) and triangular (Ga) prisms, with four (Mg) or three (Ga) additional capping atoms leading to the coordination numbers [10], [8+4] and [6+3], respectively. The crystal structure of Sc₂MgGa₂ was determined from single‐crystal diffraction intensities and the isostructural Y₂MgGa₂ was identified from powder diffraction data.     

Electrochemical study of (NEt4)2Cl2FeS2MoS2 and (NEt4)2Cl2FeS2MoS2FeCl2

Summary The ability of [MoS₄]^2–, anions to be used as ligands for transition metal ions has been widely demonstrated, especially with Fe²⁺. The present study has been restricted to linear complexes such as (NEt₄)₂ [Cl₂FeS₂MoS₂] and (NEt₄)₂[Cl₂FeS₂MoS₂FeCl₂]. Their electrochemical properties are described: upon electrochemical reduction, these compounds yield MoS₂, as a black precipitate, and an iron complex in solution, assumed to be [SFeCl₂]^2–. The electrochemical reduction goes through two electron transfers, coupled with the breakdown of the molecular skeleton: a DISPl and an ECE mechanism. Depending on the solvent, the following equilibrium may be observed: [Cl₄Fe₂MoS₄]^2–[Cl₂FeMoS₄]^2–+FeCl₂. The equilibrium constant, K_D, was evaluated by differential pulse polarography. K_D is tightly related to the donor number of the solvent.     

The alkali hypophosphites KH2PO2, RbH2PO2 and CsH2PO2

The structures of the hypophosphites KH₂PO₂ (potassium hypophosphite), RbH₂PO₂ (rubidium hypophosphite) and CsH₂PO₂ (caesium hypophosphite) have been determined by single‐crystal X‐ray diffraction. The structures consist of layers of alkali cations and hypophosphite anions, with the latter bridging four cations within the same layer. The Rb and Cs hypophosphites are isomorphous.     

Zur Kenntnis der Dialkalimetalldichalkogenide β-Na2S2, K2S2, α-Rb2S2, β-Rb2S2, K2Se2, Rb2Se2, α-K2Te2, β-K2Te2 und Rb2Te2

On Dialkali Metal Dichalcogenides β-Na₂S₂, K₂S₂, α-Rb₂S₂, β-Rb₂S₂, K₂Se₂, Rb₂Se₂, α-K₂Te₂, β-K₂Te₂ and Rb₂Te₂ The first presentation of pure samples of α- and β-Rb₂S₂, α- and β-K₂Te₂, and Rb₂Te₂ is described. Using single crystals of K₂S₂ and K₂Se₂, received by ammonothermal synthesis, the structure of the Na₂O₂ type and by using single crystals of β-Na₂S₂ and β-K₂Te₂ the Li₂O₂ type structure will be refined. By combined investigations with temperature-dependent Guinier-, neutron diffraction-, thermal analysis, and Raman-spectroscopy the nature of the monotropic phase transition from the Na₂O₂ type to the Li₂O₂ type will be explained by means of the examples α-/β-Na₂S₂ and α-/β-K₂Te₂. A further case of dimorphic condition as well as the monotropic phase transition of α- and β-Rb₂S₂ is presented. The existing areas of the structure fields of the dialkali metal dichalcogenides are limited by the model of the polar covalence.     

Formal [(2+2)+2] and [(2+2)+(2+2)] nonconjugated dienediyne cascade cycloadditions

[reaction: see text] Fluoranthene 2 and heptacycle 3 are easily accessible from the reaction of diyne 1 and norbornadiene (NBD) in the presence of the rhodium catalyst. The unusual [(2+2)+(2+2)] adduct 3 was confirmed by the X-ray crystal structure analysis.     

Crystal Structures of [Bu2Sn(O2PPh2)2], [Ph2Sn(O2PPh2)2], and [PhClSn(O2PPh2)OMe]2. Raman Spectra of [Ph2Sn(O2PPh2)2] and [PhClSn(O2PPh2)OMe]2

[(n‐Bu)₂Sn(O₂PPh₂)₂] ( 1 ), and [Ph₂Sn(O₂PPh₂)₂] ( 2 ) have been synthesized by the reactions of R₂SnCl₂ (R=n‐Bu, Ph) with HO₂PPh₂ in Methanol. From the reaction of Ph₂SnCl₂ with diphenylphosphinic acid a third product [PhClSn(O₂PPh₂)OMe]₂ ( 3 ) could be isolated. X‐ray diffraction studies show 1 to crystallize in the monoclinic space group P2₁/c with a = 1303.7(1) pm, b = 2286.9(2) pm, c = 1063.1(1) pm, β = 94.383(6)°, and Z = 4. 2 crystallizes triclinic in the space group , the cell parameters being a = 1293.2(2) pm, b = 1478.5(4) pm, c = 1507.2(3) pm, α = 98.86(3)°, β = 109.63(2)°, γ = 114.88(2)°, and Z = 2. Both compounds form arrays of eight‐membered rings (SnOPO)₂ linked at the tin atoms to form chains of infinite length. The dimer 3 consists of a like ring, in which the tin atoms are bridged by methoxo groups. It crystallizes triclinic in space group with a = 946.4(1) pm, b = 963.7(1) pm, c = 1174.2(1) pm, α = 82.495(6)°, β = 66.451(6)°, γ = 74.922(6)°, and Z = 1 for the dimer. The Raman spectra of 2 and 3 are given and discussed.     

Die Photoionenspektren von SCl2, S2Cl2 und S2Br2

Photoionization Mass Spectra of SCl₂, S₂Cl₂, and S₂Br₂ Photoionization mass spectra of SCl₂, S₂Cl₂, and S₂Br₂ have been measured. Heats of formation, bond energies, and ionization potentials of fragments have been calculated from appearance potentials.