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MoSi_(2)含量对Ta_(0.8)Hf_(0.2)C-SiC-MoSi_(2)涂层抗烧蚀性能的影响
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作者 刘莹 李红 +4 位作者 姚彧敏 杨敏 陶银萍 任慕苏 孙晋良 《材料工程》 北大核心 2025年第6期235-243,共9页
Ta_(0.8)Hf_(0.2)C具有良好的热防护性能,适合在高温烧蚀环境中使用,MoSi_(2)是一种优异的烧结助剂且常用于抗烧蚀涂层中。为了研究MoSi_(2)含量对Ta_(0.8)Hf_(0.2)C-SiC-MoSi_(2)涂层抗烧蚀性能的影响,本研究采用料浆刷涂法在含有SiC... Ta_(0.8)Hf_(0.2)C具有良好的热防护性能,适合在高温烧蚀环境中使用,MoSi_(2)是一种优异的烧结助剂且常用于抗烧蚀涂层中。为了研究MoSi_(2)含量对Ta_(0.8)Hf_(0.2)C-SiC-MoSi_(2)涂层抗烧蚀性能的影响,本研究采用料浆刷涂法在含有SiC过渡涂层的C/C复合材料上制备了不同MoSi_(2)含量的Ta_(0.8)Hf_(0.2)C-SiC-MoSi_(2)涂层,并研究了不同涂层的相组成、微观形貌和烧蚀行为。结果表明,当MoSi_(2)质量分数为10%时,涂层的质量烧蚀率和线烧蚀率分别为1.24 mg·s^(-1)、0.02μm·s^(-1),表现出较好的抗烧蚀性能。这是因为涂层中MoSi_(2)的存在抑制了SiC的主动氧化,减少了SiC的消耗,在烧蚀过程中形成的液相层黏度较高,抵抗高温火焰的冲蚀的能力较强,有效地阻止了氧的扩散。 展开更多
关键词 C/C复合材料 Ta_(0.8)Hf_(0.2)C-SiC-MoSi_(2)涂层 料浆刷涂 烧蚀
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脉冲磁场对Al-0.8Mg-0.8Si-0.1La合金凝固组织和力学性能的影响
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作者 宫美娜 贺晨 +4 位作者 杨帆 赵宇辉 吴强 王淑青 麻永林 《中国稀土学报》 北大核心 2025年第6期1263-1270,共8页
本文研究脉冲磁场对Al-0.8Mg-0.8Si-0.1La合金凝固组织和力学性能的影响。结果表明,脉冲磁场凝固条件下Al-0.8Mg-0.8Si-0.1La合金α-Al晶粒较常规凝固条件下合金α-Al晶粒明显细化且分布均匀。经脉冲磁场处理后,合金的力学性能较常规凝... 本文研究脉冲磁场对Al-0.8Mg-0.8Si-0.1La合金凝固组织和力学性能的影响。结果表明,脉冲磁场凝固条件下Al-0.8Mg-0.8Si-0.1La合金α-Al晶粒较常规凝固条件下合金α-Al晶粒明显细化且分布均匀。经脉冲磁场处理后,合金的力学性能较常规凝固条件下的合金力学性能(屈服强度87 MPa,抗拉强度128 MPa和韧性4.5%)得到明显提升,且当占空比为20%,脉冲磁场频率为20 Hz时,α-Al晶粒最为细小均匀,力学性能最高(屈服强度为99 MPa,抗拉强度为157 MPa,延伸率为5.5%)。在电磁能作用下,熔体的偏析程度明显降低,减少了稀土脆性相LaAlSi和金属间化合物的形成,有效改善了合金的组织状态,显著提高了铸态铝合金的力学性能。 展开更多
关键词 Al-0.8Mg-0.8Si-0.1La 脉冲磁场 凝固 LaAlSi 偏析
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0.8m机载天线结构动力学仿真与实验验证
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作者 李晓普 张立军 +1 位作者 张硕 李聪聪 《河北省科学院学报》 2025年第3期20-26,34,共8页
针对机载天线在飞机飞行过程中的安全问题,本研究对某0.8 m机载天线进行了有限元动力学仿真分析。运用实体建模的方法,建立合理的有限元模型并对其进行模态分析和随机振动分析,得出天线关键部位的应力值与加速度值。然后运用测试分析软... 针对机载天线在飞机飞行过程中的安全问题,本研究对某0.8 m机载天线进行了有限元动力学仿真分析。运用实体建模的方法,建立合理的有限元模型并对其进行模态分析和随机振动分析,得出天线关键部位的应力值与加速度值。然后运用测试分析软件,通过在相应的测点上布置加速度传感器和应变片,真实测量关键部位的应力值和加速度值。通过仿真与实验结果对比分析可知,误差在允许的范围内,证明了仿真分析方法的可靠性。根据仿真结果对天线进行优化设计,并进行了振动试验,振动试验后的天线各项性能均满足要求。研究结果对于天线结构的动态特性的研究具有一定的指导意义。 展开更多
关键词 0.8 m机载天线 动力学仿真 测试分析 振动试验
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Cu-0.8Fe合金的热变形行为及组织演变
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作者 贺文浩 周孟 +1 位作者 田保红 景柯 《金属热处理》 北大核心 2025年第11期16-23,共8页
采用ZG-0.01型真空中频感应炉制备了Cu-0.8Fe合金,并通过Gleeble-1500D热模拟试验机对Cu-0.8Fe合金进行了等温热变形试验(应变速率为0.003~10 s^(-1),变形温度为600~950℃)。在此基础上,绘制了合金的真应力-真应变曲线,构建了本构方程... 采用ZG-0.01型真空中频感应炉制备了Cu-0.8Fe合金,并通过Gleeble-1500D热模拟试验机对Cu-0.8Fe合金进行了等温热变形试验(应变速率为0.003~10 s^(-1),变形温度为600~950℃)。在此基础上,绘制了合金的真应力-真应变曲线,构建了本构方程和热加工图,分析了合金在不同变形条件下的显微组织演变规律。结果表明:Cu-0.8Fe合金的热变形激活能为379.158 kJ/mol,相比纯Cu提高了24.8%;合金的最佳热加工参数为:应变速率0.018~0.449 s^(-1)、变形温度775~950℃;提高热变形温度或者降低应变速率均有利于该合金发生动态再结晶。TEM分析表明,该合金热变形过程中的主要析出相为α-Fe相。 展开更多
关键词 Cu-0.8Fe合金 本构方程 热加工图 显微组织
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Tailoring the morphology and charge transfer pathways of ultrathin Cd_(0.8)Zn_(0.2)S nanosheets via ionic liquid-modified Ti_(3)C_(2)MXenes towards remarkable photocatalytic hydrogen evolution 被引量:2
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作者 Qianqian Hu Haiyan Yin +5 位作者 Yifan Liu Abdusalam Ablez Zhuangzhuang Wang Yue Zhan Chengfeng Du Xiaoying Huang 《Journal of Materials Science & Technology》 2025年第1期47-59,共13页
Small-sized Cd_(x) Zn_(1-x) S solid solution nanomaterial is an important candidate for efficient photocatalytic hydrogen evolution(PHE),but it still suffers from easy agglomeration,severe photo corrosion,and fast pho... Small-sized Cd_(x) Zn_(1-x) S solid solution nanomaterial is an important candidate for efficient photocatalytic hydrogen evolution(PHE),but it still suffers from easy agglomeration,severe photo corrosion,and fast photogenerated electron-hole recombination.To tackle these issues,herein,we propose a new strategy to modify Cd_(x) Zn_(1-x) S nanoreactors by the simultaneous utilization of ionic-liquid-assisted morphology engineering and MXene-incorporating method.That is,we designed and synthesized a novel hierarchi-cal Cd_(0.8) Zn_(0.2) S/Ti_(3) C_(2) Schottky junction composite through the in-situ deposition of ultrathin Cd_(0.8) Zn_(0.2) S nanosheets on unique IL-modified Ti_(3) C_(2) MXenes by a one-pot solvothermal method for efficiently PHE.The unique construction strategy tailors the thickness of ultrathin Cd_(0.8) Zn_(0.2) S nanosheets and prevents them from stacking and agglomeration,and especially,optimizes their charge transfer pathways during the photocatalytic process.Compared with pristine Cd_(0.8) Zn_(0.2) S nanosheets,Cd_(0.8) Zn_(0.2) S/Ti_(3) C_(2) has abun-dant photogenerated electrons available on the Ti_(3) C_(2) surface for proton reduction reaction,owing to the absence of deep-trapped electrons,suppression of electron-hole recombination in Cd_(0.8) Zn_(0.2) S and high-efficiency charge separation at the Cd_(0.8) Zn_(0.2) S/Ti_(3) C_(2) Schottky junction interface.Moreover,the hy-drophilicity,electrical conductivity,visible-light absorption capacity,and surficial hydrogen desorption of Cd_(0.8) Zn_(0.2) S/Ti_(3) C_(2) heterostructure are significantly improved.As a result,the heterostructure exhibits out-standing photocatalytic stability and super high apparent quantum efficiency,being rendered as one of the best noble-metal-free Cd-Zn-S-based photocatalysts.This work illustrates the mechanisms of mor-phology control and heterojunction construction in controlling the catalytic behavior of photocatalysts and highlights the great potential of the IL-assisted route in the synthesis of high-performance MXene-based heterostructures for photocatalytic hydrogen evolution. 展开更多
关键词 Ionic liquid Ultrathin Cd_(0.8)Zn_(0.2)S nanosheets MXene Schottky junction Photoexcited charge separation Photocatalytic H_(2)evolution
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Al-0.8Mg-0.9Si-0.6Cu-0.4Mn合金挤压型材的室温停放效应
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作者 王涛 刘德涛 +4 位作者 栾兴隆 王玉刚 李银柱 张沛鸿 田妮 《轻合金加工技术》 2025年第5期42-50,共9页
利用OM、TEM、显微硬度测试仪、导电率测试仪以及拉伸试验机等仪器和设备,研究了我国新一代高速列车车体及关键承力件用Al-0.8Mg-0.9Si-0.6Cu-0.4Mn合金挤压型材经565℃30 min固溶水淬后于室温分别停放5 min、120 min、360 min、1440 mi... 利用OM、TEM、显微硬度测试仪、导电率测试仪以及拉伸试验机等仪器和设备,研究了我国新一代高速列车车体及关键承力件用Al-0.8Mg-0.9Si-0.6Cu-0.4Mn合金挤压型材经565℃30 min固溶水淬后于室温分别停放5 min、120 min、360 min、1440 min和2880 min后的硬度及导电率,以及合金再经165℃24 h人工时效处理后的显微组织、导电率及力学性能。结果表明,合金挤压材经565℃30 min固溶处理水淬后于室温停放时间从5 min延长至120 min,合金的导电率单调降低,硬度逐渐增大。固溶水淬后至T6处理之间的室温停放时间对挤压型材中的过剩结晶相粒子、弥散相粒子、晶界析出相粒子以及晶粒组态无明显影响,但室温停放时间超过120 min,合金再经T6处理后的基体析出相粒子粗化、数量减少、间距增大。固溶水淬处理后室温停放5 min进行T6处理的挤压型材的抗拉强度、屈服强度和断后伸长率均最高,分别为422 MPa、384 MPa和14.5%。固溶水淬后于室温停放的时间超过120 min再进行T6处理会降低挤压材的硬度、强度和断后伸长率。 展开更多
关键词 Al-0.8Mg-0.9Si-0.6Cu合金挤压型材 室温停放时间 析出相 导电率 力学性能
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阳极支撑构型BaZr_(0.8)Y_(0.2)O_(3−δ)基质子导体固体氧化物燃料电池的制备及性能研究
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作者 陈美龙 李采丰 +4 位作者 吴学良 鲁欣洋 Dustin Banham 杜丽 陈旻 《陶瓷学报》 北大核心 2025年第3期506-514,共9页
质子导体固体氧化物燃料电池(H^(+)-SOFC)是一种采用全固态质子陶瓷导体为电解质的先进燃料电池技术。与传统氧离子导体SOFC相比,具有低运行温度、高性能稳定性、高燃料利用率等优点。然而,高化学稳定性BaZr_(0.8)Y_(0.2)O_(3−δ)(BZY20... 质子导体固体氧化物燃料电池(H^(+)-SOFC)是一种采用全固态质子陶瓷导体为电解质的先进燃料电池技术。与传统氧离子导体SOFC相比,具有低运行温度、高性能稳定性、高燃料利用率等优点。然而,高化学稳定性BaZr_(0.8)Y_(0.2)O_(3−δ)(BZY20)电解质的烧结活性差,导致BZY20基H^(+)-SOFC的电化学性能偏低。针对该问题,通过优化阳极支撑体和电解质膜在共烧结过程中的烧结收缩行为来促进BZY20电解质的致密化,研究了添加不同类型造孔剂的阳极支撑体孔结构和烧结收缩率,成功制备出构型为Ni-BZY20/BZY20/La_(0.6)Sr_(0.4)Co_(0.2)Fe_(0.8)O_(3−δ)BaCe_(0.7)Zr_(0.1)Y_(0.1)Yb_(0.1)O_(3−δ)纽扣电池。相比于玉米淀粉造孔剂,采用同等质量比的石墨造孔剂所制得电池的阳极孔隙率更高(~21%),且BZY20电解质膜的致密性好、晶粒较大,这些显微结构特征使其电化学性能也得到提升。在此基础上,进一步优化电解质膜制备工艺,将BZY20的厚度从39μm降至12μm,这一举措最终使得电池的欧姆电阻Ro降低了一半,且电池在600℃下的功率密度达到210 mW·cm^(−2)。 展开更多
关键词 质子导体固体氧化物燃料电池 造孔剂 阳极 BaZr_(0.8)Y_(0.2)O_(3−δ) 烧结收缩率
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Ag包覆对正极材料LiNi_(0.8)Co_(0.1)Mn_(0.1)O_(2)性能的影响
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作者 王树新 郑舒 《电源技术》 北大核心 2025年第3期543-548,共6页
为了提高LiNi_(0.8)Co_(0.1)Mn_(0.1)O_(2)的稳定性和倍率性能,采用湿法和高温煅烧法对其表面进行Ag包覆改性。利用X射线衍射、扫描电子显微镜和电化学充放电等测试,对材料结构进行表征和电化学性能测试,结果表明:单质Ag可以均匀包覆LiN... 为了提高LiNi_(0.8)Co_(0.1)Mn_(0.1)O_(2)的稳定性和倍率性能,采用湿法和高温煅烧法对其表面进行Ag包覆改性。利用X射线衍射、扫描电子显微镜和电化学充放电等测试,对材料结构进行表征和电化学性能测试,结果表明:单质Ag可以均匀包覆LiNi_(0.8)Co_(0.1)Mn_(0.1)O_(2)材料表面,且不影响材料的晶体结构,Ag包覆可提高材料在工作过程中的循环稳定性和倍率性能。实验所得材料常温1 C倍率下的放电比容量高达173.7 mAh/g,25℃下1 C循环2000次后容量保持率在89%以上。 展开更多
关键词 电化学性能 LiNi_(0.8)Co_(0.1)Mn_(0.1)O_(2)正极材料 煅烧法
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新型Ba_(0.5)Sr_(0.5)(Co_(0.8)Fe_(0.2))_(1-x)Ni_(x)O_(3-δ)质子导体固体氧化物燃料电池阴极材料研究
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作者 邹鑫朝 翁演鑫 +1 位作者 林世鸿 古月圆 《应用化工》 北大核心 2025年第6期1409-1414,1421,共7页
基于B位变价金属阳离子共掺杂而设计了一种新型Ba_(0.5)Sr_(0.5)(Co_(0.8)Fe_(0.2))_(1-x)Ni_(x)O_(3-δ)(x=0,0.05,0.1,0.2)阴极材料,对其物相结构、化学兼容性、电化学性能和抗CO 2毒化性能进行了系统评估。研究发现,与Ba_(0.5)Sr_(0.... 基于B位变价金属阳离子共掺杂而设计了一种新型Ba_(0.5)Sr_(0.5)(Co_(0.8)Fe_(0.2))_(1-x)Ni_(x)O_(3-δ)(x=0,0.05,0.1,0.2)阴极材料,对其物相结构、化学兼容性、电化学性能和抗CO 2毒化性能进行了系统评估。研究发现,与Ba_(0.5)Sr_(0.5)Co_(0.8)Fe_(0.2)O_(3-δ)(BSCF)相比,Ni的掺杂有利于氧空位的形成和氧还原反应活性的提升,然而,其金属氧化物碱度的增加牺牲了部分抗CO 2毒化性能。通过与电解质复合制备了复合阴极,并将其用于质子导体固体氧化物燃料电池(Proton conducting solid oxide fuel cells,H-SOFCs)。其中,Ba_(0.5)Sr_(0.5)(Co_(0.8)Fe_(0.2))_(0.9) Ni_(0.1) O_(3-δ)(BSCFN0.1)阴极表现出最优异的电化学性能。700℃时,BSCFN0.1阴极单电池的峰值功率密度高达1068 mW/cm^(2),比面积电阻低至0.059Ω·cm^(2)。BSCF衍生的BSCFN阴极材料展现出良好的性能,可能为质子导体固体氧化物燃料电池提供新的材料选择。 展开更多
关键词 固体氧化物燃料电池 阴极材料 电化学性能 Ba_(0.5)Sr_(0.5)(Co_(0.8)Fe_(0.2))_(1-x)Ni_(x)O_(3-δ)
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Enhanced Piezoelectric Properties of (1-x)(0.8PZT-0.2PZN)-xBZT Ceramics via Phase Boundary and Domain Engineering
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作者 CHEN Xiangjie LI Ling +2 位作者 LEI Tianfu WANG Jiajia WANG Yaojin 《无机材料学报》 北大核心 2025年第6期729-734,共6页
Pb(Zr,Ti)O_(3)-Pb(Zn_(1/3)Nb_(2/3))O_(3) (PZT-PZN) based ceramics, as important piezoelectric materials, have a wide range of applications in fields such as sensors and actuators, thus the optimization of their piezoe... Pb(Zr,Ti)O_(3)-Pb(Zn_(1/3)Nb_(2/3))O_(3) (PZT-PZN) based ceramics, as important piezoelectric materials, have a wide range of applications in fields such as sensors and actuators, thus the optimization of their piezoelectric properties has been a hot research topic. This study investigated the effects of phase boundary engineering and domain engineering on (1-x)[0.8Pb(Zr_(0.5)Ti_(0.5))O_(3)-0.2Pb(Zn_(1/3)Nb_(2/3))O_(3)]-xBi(Zn_(0.5)Ti_(0.5))O_(3) ((1-x)(0.8PZT-0.2PZN)- xBZT) ceramic to obtain excellent piezoelectric properties. The crystal phase structure and microstructure of ceramic samples were characterized. The results showed that all samples had a pure perovskite structure, and the addition of BZT gradually increased the grain size. The addition of BZT caused a phase transition in ceramic samples from the morphotropic phase boundary (MPB) towards the tetragonal phase region, which is crucial for optimizing piezoelectric properties. By adjusting content of BZT and precisely controlling position of the phase boundary, the piezoelectric performance can be optimized. Domain structure is one of the key factors affecting piezoelectric performance. By using domain engineering techniques to optimize grain size and domain size, piezoelectric properties of ceramic samples have been significantly improved. Specifically, excellent piezoelectric properties (piezoelectric constant d_(33)=320 pC/N, electromechanical coupling factor kp=0.44) were obtained simultaneously for x=0.08. Based on experimental results and theoretical analysis, influence mechanisms of phase boundary engineering and domain engineering on piezoelectric properties were explored. The study shows that addition of BZT not only promotes grain growth, but also optimizes the domain structure, enabling the polarization reversal process easier, thereby improving piezoelectric properties. These research results not only provide new ideas for the design of high-performance piezoelectric ceramics, but also lay a theoretical foundation for development of related electronic devices. 展开更多
关键词 phase boundary 0.8PZT-0.2PZN domain engineering piezoelectric property
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固溶温度对Ti-0.3Mo-0.8Ni钛合金微观组织与拉伸性能的影响
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作者 梁飞龙 张明玉 +2 位作者 宋一新 岳旭 同晓乐 《稀有金属与硬质合金》 北大核心 2025年第2期88-93,152,共7页
选取Ti-0.3Mo-0.8Ni钛合金作为试验材料,对其进行不同温度的固溶处理。通过光学显微镜(OM)、扫描电子显微镜(SEM)、X射线衍射仪(XRD)以及拉伸性能测试,研究了固溶温度对Ti-0.3Mo-0.8Ni钛合金微观组织与拉伸性能的影响。结果表明:合金原... 选取Ti-0.3Mo-0.8Ni钛合金作为试验材料,对其进行不同温度的固溶处理。通过光学显微镜(OM)、扫描电子显微镜(SEM)、X射线衍射仪(XRD)以及拉伸性能测试,研究了固溶温度对Ti-0.3Mo-0.8Ni钛合金微观组织与拉伸性能的影响。结果表明:合金原始组织为经过两相区锻造加工而形成的等轴组织,由大量初生α相(α_(p))以及少量β转变组织(β_(T))构成。随着固溶温度升高,固溶合金组织中α_(p)相逐渐变小,最后完全溶解消失,而析出的α′相含量有所增加且尺寸逐渐增大;合金强度随之提高,而塑性则随之降低;合金断口微观形貌由韧窝转变为结晶状形貌,逐渐出现撕裂棱,断裂特征由韧性断裂向脆性断裂转变。 展开更多
关键词 Ti-0.3Mo-0.8Ni钛合金 固溶处理 温度 微观组织 拉伸性能 断口微观形貌
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S-scheme Cd_(0.8)Zn_(0.2)S nanowires/CeO_(2)nanocubes heterojunction for efficient photocatalytic hydrogen evolution
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作者 Yuqing Yan Yonghui Wu +3 位作者 Jun Wang Jinrong Huo Kai Yang Kangqiang Lu 《Chinese Journal of Catalysis》 2025年第12期231-239,共9页
Constructing S-scheme heterojunctions preserves the intrinsic redox capabilities of both semiconductors while promoting the separation of photogenerated electrons and holes,making it a promising approach for enhancing... Constructing S-scheme heterojunctions preserves the intrinsic redox capabilities of both semiconductors while promoting the separation of photogenerated electrons and holes,making it a promising approach for enhancing the properties of semiconductors.In this study,an S-scheme Cd_(0.8)Zn_(0.2)S-CeO_(2)(CZS-CeO_(2))heterojunction was successfully fabricated via the in-situ growth of CZS nanowires on CeO_(2)nanocubes.The S-scheme charge-transfer mechanism of the CZS-CeO_(2)composites during photocatalytic reactions was confirmed through in-situ X-ray photoelectron spectroscopy and density functional theory calculations.These results demonstrate that the interfacial electric field(IEF)significantly facilitates charge separation and transport within the heterojunction.Consequently,the CZS-CeO_(2)composites exhibited excellent photocatalytic hydrogen production performance under simulated sunlight irradiation,surpassing that of blank CZS.Particularly,the optimal photocatalytic hydrogen generation rate for CZS-15%CeO_(2)reached 58 mmol·g^(-1)·h^(-1),approximately 8.8 times higher than that of blank CZS.After five consecutive cycles of testing,CZS-15%CeO_(2)retained a relatively high level of activity.This enhanced stability can be attributed to the fabrication of S-scheme heterojunctions,which effectively suppressed hole-induced photocorrosion of CZS.This investigation provides a beneficial reference for the rational design of S-scheme heterojunction photocatalysts for efficient and stable photocatalytic hydrogen production. 展开更多
关键词 Photocatalytic hydrogen evolution CeO_(2) Cd_(0.8)Zn_(0.2)S S-scheme heterojunction Built-in electric field
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锂离子电池正极材料Li[Ni_(0.8)Co_(0.1)Mn_(0.1)]O_(2)的可控合成与Ca掺杂改性
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作者 安鹏燕 王舒冉 +5 位作者 董默涵 傅世郑 张一龙 王家顺 张德柳 刘朝孟 《电力科技与环保》 2025年第2期194-205,共12页
【目的】锂离子电池因其在循环寿命、能量密度及成本方面的优势,受到了广泛关注。正极材料是实现锂离子电池高能量存储的关键。其中,高镍三元材料因其成本低和容量高等优点成为正极材料的首选,但由于镍元素的存在,发生锂镍混排,电池循... 【目的】锂离子电池因其在循环寿命、能量密度及成本方面的优势,受到了广泛关注。正极材料是实现锂离子电池高能量存储的关键。其中,高镍三元材料因其成本低和容量高等优点成为正极材料的首选,但由于镍元素的存在,发生锂镍混排,电池循环稳定性极差。因此,对三元L[i Ni_(0.8)Co_(0.1)Mn_(0.1)]O_(2)(NCM811)材料的制备和钙掺杂改性进行研究。【方法】采用共沉淀法制备三元材料NCM811的前驱体,通过分析不同静置时间对颗粒形貌、结构以及电化学性能的影响,得到最佳合成条件,并以Ca(OH)_(2)作为钙源对NCM811三元材料进行掺杂改性。【结果】研究表明,静置10 h的倍率下表现出更好的性能,但静置时间为1 h的首次放电比容量较高;静置1 h和10 h在100次循环后的放电比容量和容量保持率十分接近;钙掺杂为3%时反而会出现相反的影响,导致阳离子混排加剧,循环和倍率性能变差,最终得出2%为钙掺杂的最佳掺杂量;最优掺杂量2%的NCM材料在0.1 C的首圈放电比容量为178.25 mA·h/g,库伦效率为81.55%,1 C倍率循环100圈后放电比容量为154.64 mA·h/g和容量保持率为86.37%;材料合成时静置时间10 h具有更好的倍率性能;【结论】适量的钙掺杂可以降低阳离子混排程度,大幅提高了三元材料的放电比容量和容量保持率,改善三元材料的循环和倍率性能。 展开更多
关键词 Li[Ni_(0.8)Co_(0.1)Mn_(0.1)]O_(2) 锂离子电池 正极材料 电化学性能 钙掺杂
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Pr_(0.8)Sr_(0.2)BaCo_(2)O_(5+δ)固体氧化物燃料电池阴极材料的制备及性能研究
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作者 刘妍 韩飞 +3 位作者 夏海涛 张智健 周启楠 徐必 《长春师范大学学报》 2025年第6期29-34,共6页
通过固相反应法合成了Pr_(0.8)Sr_(0.2)BaCo_(2)O_(5+δ)(PSr_(0.2)BC)阴极材料,通过XRD、扫描电镜、热重、电子顺磁共振、电化学阻抗等测试对其进行了性能分析。XRD和扫描电镜测试结果显示,样品结晶度良好,具有多孔结构,阴极材料具备... 通过固相反应法合成了Pr_(0.8)Sr_(0.2)BaCo_(2)O_(5+δ)(PSr_(0.2)BC)阴极材料,通过XRD、扫描电镜、热重、电子顺磁共振、电化学阻抗等测试对其进行了性能分析。XRD和扫描电镜测试结果显示,样品结晶度良好,具有多孔结构,阴极材料具备大小合适的粒径,有利于氧气传输。热重与热膨胀测试发现,材料具有适宜的氧空位浓度与热膨胀系数。电化学阻抗测试可知,PSr_(0.2)BC/SDC/PSr_(0.2)BC半电池在800℃的极化电阻为0.078Ω·cm^(2)。NiO+SDC/SDC/PSr_(0.2)BC单电池在800℃的最大功率密度为293 mW·cm^(-2)。 展开更多
关键词 掺杂 Pr_(0.8)Sr_(0.2)BaCo_(2)O_(5+δ) 氧空位 功率密度
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Ti_(3)C_(2)T_(x)纳米片用于增强Cd_(0.8)Zn_(0.2)S纳米材料的光催化制氢性能研究
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作者 许堡荣 侯雪兰 +1 位作者 卫鈿 杨贵东 《化学反应工程与工艺》 2025年第1期207-215,共9页
探索高效、低成本的助催化剂以提高光催化制氢性能,在能源利用技术发展中具有重要的意义。本研究以Ti_(3)AlC_(2)为原料,通过选择性刻蚀方法及随后的液相剥离过程,成功制备了二维Ti_(3)C_(2)T_(x)纳米片。采用经典的水热法,在Ti_(3)C_(2... 探索高效、低成本的助催化剂以提高光催化制氢性能,在能源利用技术发展中具有重要的意义。本研究以Ti_(3)AlC_(2)为原料,通过选择性刻蚀方法及随后的液相剥离过程,成功制备了二维Ti_(3)C_(2)T_(x)纳米片。采用经典的水热法,在Ti_(3)C_(2)T_(x)纳米片表面原位修饰了Cd_(0.8)Zn_(0.2)S纳米颗粒,合成了一种新型的异质结光催化剂。得益于Ti_(3)C_(2)T_(x)纳米片优异的电子传输作用,所制备的Cd_(0.8)Zn_(0.2)S/Ti_(3)C_(2)T_(x)纳米材料表现出较强的光生空穴-电子对分离与迁移能力,并展现出优异的光催化析氢活性。在可见光照射下,Cd_(0.8)Zn_(0.2)S/Ti_(3)C_(2)T_(x)纳米材料的产氢速率可达1954.2μmol/(g·h),是相同条件下纯Cd_(0.8)Zn_(0.2)S纳米材料的4.2倍。 展开更多
关键词 Ti_(3)C_(2)T_(x)纳米片 Cd_(0.8)Zn_(0.2)S 异质结 助催化剂 光催化制氢
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Proton transport in unsintered BaCe_(0.8)Y_(0.2)O_(3-α) for easily prepared electrochemical devices
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作者 Xi Wang Yushi Ding +2 位作者 Ying Li Gaopeng Zhou Wenlong Huang 《Journal of Rare Earths》 2025年第1期133-145,I0006,共14页
BaCe_(0.8)Y_(0.2)O_(3)-αceramics exhibit superior conductivity among related materials.However,the hightemperature sintering makes it difficult to prepare electrochemical devices with a BaCe_(0.8)Y_(0.2)O_(3)-αmulti... BaCe_(0.8)Y_(0.2)O_(3)-αceramics exhibit superior conductivity among related materials.However,the hightemperature sintering makes it difficult to prepare electrochemical devices with a BaCe_(0.8)Y_(0.2)O_(3)-αmultilayer film,and very few studies have examined the conductivity and transport properties of unsintered BaCe_(0.8)Y_(0.2)O_(3)-α.In nominally dry conditions,the instability of this material in a watercontaining atmosphere can be minimized,allowing the unsintered BaCe_(0.8)Y_(0.2)O_(3)-αto be applied in some particular test environment as a component of electrochemical devices.Hence,the conductivity of unsintered BaCe_(0.8)Y_(0.2)O_(3)-αin dry conditions was measured via AC impedance spectroscopy in the temperature range of 500-800℃.The unsintered BaCe_(0.8)Y_(0.2)O_(3)-αexhibits high conductivity and hydration ability,as well as low proton activation energy.In addition,it shows high oxygen vacancy and low proton transport numbers at high temperature,limited by its grain boundaries.This work provides insights into the conductivity and proton transport of unsintered BaCe_(0.8)Y_(0.2)O_(3)-αand demonstrates its potential as a proton-conducting electrolyte. 展开更多
关键词 Protonic conductor Unsintered material BaCe_(0.8)Y_(0.2)0^(3-α) CONDUCTIVITY Transport number Rare earths
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In-situ deposition and comparative study of electromagnetic absorption performance of MXene(Ti_(3)C_(2)T_(x))@nano-Fe_(1)Co_(0.8)Ni_(1) composites with different compositions
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作者 Hong Li Hongyang Li +7 位作者 Zhenfeng Shen Shentao Zeng Feng Yang Qing Cai Wenqi Xu Ran Wang Cui Luo Ying Liu 《International Journal of Minerals,Metallurgy and Materials》 2025年第5期1259-1269,共11页
Three sets of MXene(Ti_(3)C_(2)T_(x))@nano-Fe_(1)Co_(0.8)Ni_(1)composites with 15,45,and 90 mg MXene were prepared by in-situ liquid-phase deposition to effectively investigate the impact of the relationship between M... Three sets of MXene(Ti_(3)C_(2)T_(x))@nano-Fe_(1)Co_(0.8)Ni_(1)composites with 15,45,and 90 mg MXene were prepared by in-situ liquid-phase deposition to effectively investigate the impact of the relationship between MXene(Ti_(3)C_(2)T_(x))and nano-Fe_(1)Co_(0.8)Ni_(1)magnetic particles on the electromagnetic absorption properties of the composites.The microstructure,static magnetic properties,and electromag-netic absorption performance of these composites were studied.Results indicate that the MXene@nano-Fe_(1)Co_(0.8)Ni_(1)composites were primarily composed of face-centered cubic crystal structure particles and MXene,with spherical Fe_(1)Co_(0.8)Ni_(1)particles uniformly distrib-uted on the surface of the multilayered MXene.The alloy particles had an average particle size of approximately 100 nm and exhibited good dispersion without noticeable particle aggregation.With the increase in MXene content,the specific saturation magnetic and coer-civity of the composite initially decreased and then increased,displaying typical soft magnetic properties.Compared with those of the Fe_(1)Co_(0.8)Ni_(1)magnetic alloy particles alone,MXene addition caused an increasing trend in the real and imaginary parts of the dielectric constant of the composite.Meanwhile,the real and imaginary parts of the magnetic permeability exhibit decreasing trend.With the in-crease in MXene addition,the material attenuation constant increased and the impedance matching decreased.The minimum reflection loss increased,and the maximum effective absorption bandwidth decreased.When the MXene addition was 90 mg,the composite exhib-ited a minimum reflection loss of-46.9 dB with a sample thickness of 1.1 mm and a maximum effective absorption bandwidth of 3.60 GHz with a sample thickness of 1.0 mm.The effective absorption bandwidth of the composites and their corresponding thicknesses showed a decreasing trend with the increase in MXene addition,reducing by 50%from 1.5 mm without MXene addition to 1 mm with 90 mg of MXene addition. 展开更多
关键词 MXene nano-Fe_(1)Co_(0.8)Ni_(1)alloy particles static magnetic properties electromagnetic wave absorption effective absorption bandwidth
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Photothermal dry reforming of methane reaction over (Ni/Ce_(0.8)Zr_(0.2)O_(2))@SiO_(2) catalysts: The Ni content regulation
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作者 Xiaoyan Tian Yu Shi +1 位作者 Jianming Zhang Fagen Wang 《Green Energy & Environment》 2025年第8期1751-1763,共13页
Dry reforming of methane(DRM)converts CH4 and CO_(2) to syngas.Photothermal DRM,which integrates temperature and light,is a sustainable method for storing solar energy in molecules.However,challenges such as limited l... Dry reforming of methane(DRM)converts CH4 and CO_(2) to syngas.Photothermal DRM,which integrates temperature and light,is a sustainable method for storing solar energy in molecules.However,challenges such as limited light absorption,low photocarrier separation efficiency,Ni sintering,and carbon deposition hinder DRM stability.Herein,we regulated Ni contents in(Ni/Ce_(0.8)Zr_(0.2)O_(2))@SiO_(2) catalysts to enhance the optical characteristics while addressing Ni sintering and carbon deposition issues.The(3Ni/Ce_(0.8)Zr_(0.2)O_(2))@SiO_(2) catalyst had insufficient Ni content,while the(9Ni/Ce_(0.8)Zr_(0.2)O_(2))@SiO_(2) catalyst showed excessive carbon deposition,leading to lower stability compared to the(6Ni/Ce_(0.8)Zr_(0.2)O_(2))@SiO_(2) catalyst,which achieved CH4 and CO_(2) rates to 231.0 μmol gcat^(-1)s^(-1) and 294.3 μmol gcat^(-1)s^(-1) ,respectively,at 973 K,with only 0.2 wt.%carbon deposition and no Ni sintering.This work adjusted Ni contents in(Ni/Ce_(0.8)Zr_(0.2)O_(2))@SiO_(2) catalysts to enhance DRM performance,which has implications for improving other reactions. 展开更多
关键词 PHOTOTHERMAL DRM (Ni/Ce_(0.8)Zr_(0.2)O_(2))@SiO_(2)catalyst Ni regulation Carbon deposition
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Design and conductivity optimization of La_(0.3)Sr_(0.7)TiO_(3)/L_(a0.8)Sr_(0.2)MnO_(3) bi-layer structures as tubular segmented-in-series solid oxide fuel cell interconnect
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作者 Rui Shi Yan'an Li +5 位作者 Jiutao Gao Ziyang Chen Xin Zhang Shanlin Zhang Zaheer Ud Din Babar Chengxin Li 《Journal of Rare Earths》 2025年第9期1920-1928,共9页
This study focused on meeting the stringent stability requirements of tubular segmented-in-series solid oxide fuel cells(SOFCs) in reducing and oxidizing atmospheres.To address this challenge,a bi-layer perovskite cer... This study focused on meeting the stringent stability requirements of tubular segmented-in-series solid oxide fuel cells(SOFCs) in reducing and oxidizing atmospheres.To address this challenge,a bi-layer perovskite ceramic interconnect was designed by controlling the oxygen partial pressure,because of the strong correlation between the conductivity of strontium-doped lanthanum titanate(LST) and the oxygen partial pressure.The LST powder was prepared using solid-phase and sol-gel methods,and their influence on particle size and sintering behavior was compared.LST/lanthanum strontium manganite(LSM) bi-layer ceramic interconnects with varying thicknesses were fabricated through screen printing and co-sintering.The results demonstrate favorable interfacial bonding and excellent chemical compatibility between the ceramic layers.The conductivity of the bi-layer interconnect exhibits a temperature-dependent behavior,peaking at 550℃.Simulation calculations and research findings validate that the co nductivity of the bi-layer interconnect is determined by the thickness of the LSM layer and the oxygen partial pressure at the interconnect interface.Optimal conductivity is achieved with a bilayer interconnect consisting of approximately 15 μm of LST and 4 μm of LSM.This can be attributed to the efficient regulation of oxygen partial pressure at the interface,effectively mitigating LSM decomposition caused by low oxygen partial pressure and the subsequent reduction in conductivity.These results provide valuable fundamental data and methodology for the development of high-performance interconnects for tubular segmented-in-series SOFCs. 展开更多
关键词 Tubular SOFCs Interconnects BI-LAYER La_(0.3)Sr_(0.7)TiO_(3)/L_(a0.8)Sr_(0.2)MnO_(3) Electrical conductivity Rareearths
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Elevated temperature resilience of pouch LiNi_(0.8)Co_(0.1)Mn_(0.1)O_(2)/graphite batteries through siloxane-induced cathode electrolyte interphase optimization
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作者 Xiang Gao Peiqi Zhou +6 位作者 Haijia Li Xueyi Zeng Xin He Weizhen Fan Wenlian Wang Zhen Ma Junmin Nan 《Journal of Energy Chemistry》 2025年第5期202-213,共12页
As a potential candidate for high-energy lithium-ion batteries (LIBs),nickel-rich cathodes encounter significant challenges due to structural instability arising from interphases.In this work,tris(ethenyl)-tris(etheny... As a potential candidate for high-energy lithium-ion batteries (LIBs),nickel-rich cathodes encounter significant challenges due to structural instability arising from interphases.In this work,tris(ethenyl)-tris(ethenyl)silyloxysilane (HVDS) with Si–O bonds and unsaturated bonds is introduced as additive designing functional electrolyte to enhance the long-cycle stability of LiNi_(0.8)Co_(0.1)Mn_(0.1)O_(2)(NCM811)/graphite LIBs at elevated temperature.The preferential oxidization and component of HVDS facilitate the generation of an extremely robust and ultra-thin cathode electrolyte interphase (CEI) comprising a chemically bonded silane polymer.This interphase effectively suppresses side-reactions of electrolyte,mitigates HF erosion,and reduces irreversible phase transitions.Benefiting from the above merits,the batteries’capacity retention shows a remarkable increase from 20% to 92% after nearly 1550 cycles conducted at room temperature.And under elevated temperature conditions (45℃),the capacity retention remains 80%after 670 cycles,in comparison to a drop to 80%after only 250 cycles with the blank electrolyte.These findings highlight HVDS’s potential to functionalize the electrolyte,marking a breakthrough in improving the longevity and reliability of NCM811/graphite LIBs under challenging conditions. 展开更多
关键词 High temperature performance Tris(ethenyl)-tris(ethenyl)silyloxysilane additive LiNi_(0.8)Co_(0.1)Mn_(0.1)O_(2)/graphite battery Cathode electrolyte interphase
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