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In this work, gas response properties of Pd modified TiO2 sensing films are discussed when exposed to H2 and O2. TiO2 films are surface modified in PdCl2-containing solution by the dipping method and treated for different treatment times to get different surface states. X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), scanning electron microscopy (SEM) and Kröger–Vink defect theory are used to characterize the sensing films. The gas response properties indicate that the sensor response time which related to the rate of change of sensor resistance is affected by the activation energy (E). In particular, the sensor treated at 900 °C for 2 h exhibits a response time of about 20–240 ms when exposed to H2 and 40–130 ms when exposed to O2 at 500–800 °C. 相似文献
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针对我国煤炭行业风机系统的应用现状,开发了基于高压变频器的风机自动控制系统.系统采用“二拖二,互为备用”方案,利用高压变频器对风机进行调速控制,实现了系统根据实际所需的风量来调节电机转速,提高了可靠性,获得了较好的控制性能和良好的节能效果. 相似文献
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不同于以往温度、应变与光纤Bragg光栅(FBG)峰值波长偏移量之间的数学模型,本文提出利用支持向量机(SVM,support vector machine)补偿温度的影响,并以FBG压力传感器为例,利用标定的压力传感器数据对SVM模型的惩罚系数C和径向基核函数(RBF)核参数γ进行优化,得到SVM温度补偿模型,选择核参数γ为100、惩罚系数C为16。经过补偿后,压力传感器的零位温度系数和灵敏度温度系数由补偿前的34.5%/℃和34.2%/℃减小到1.7×10-5%/℃和7.7×10-5/%/℃。充分说明,利用SVM补偿温度对FBG压力传感器的影响是有效的。 相似文献
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用数字散斑法测量铜/铝复层板拉伸变形 总被引:1,自引:1,他引:0
提出了一种基于数字散斑相关法和双目立体视觉技术的全场三维变形测量方法,实现了对爆炸焊接制备的铜/铝复层材料的变形测量。研究了该方法所涉及的数字散斑相关算法、三维坐标、位移和应变计算等关键技术,借助于VC++6.0开发环境,研制并开发了用于铜/铝复层板全场变形测量的试验系统及其软件。为了验证本文所述测量方法的可行性,进行了精度验证实验和铜/铝复层板单向拉伸试验,且对复层板拉伸试验结果与有限元软件Abaqus数值模拟结果进行了对比分析。结果表明:本文方法的应变测量精度优于0.5%,与引伸计测得的结果基本相当;测得的应变极值分布与有限元模拟结果很吻合;在板料发生颈缩前,塑性应力-应变模拟曲线与试验结果很吻合;整个变形过程中位移-载荷模拟曲线的变化趋势与试验结果一致,模拟得到的极限载荷的相对误差为0.06%~2.25%。实验结果说明,数字散斑方法是一种精确获得复层板料全场应变的有效手段。 相似文献
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我国新疆、甘肃、宁夏、内蒙、浙江、黑龙江、江苏、广东等都在大规模建设风电场,这些风电场建成后,其故障维护就有了很大市场.以新疆风电场为基础,尝试开发用于风力机故障智能诊断的系统.首先介绍了风力机及其变频器系统的结构,分析了变频器的故障机理.使用SOM神经网络对风机变流器进行了诊断,用数据验证了诊断结果.把传统的电力电子设备故障诊断技术与新疆风力机变频器的故障诊断相结合,为风电大面积推广应用产生了积极作用. 相似文献
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《Ceramics International》2016,42(7):8257-8262
A core-shell composite consisting of polypyrrole (PPy) nanofibers and TiO2 was synthesized by using PPy nanofibers as the core and TiO2 as the shell. The TiO2@PPy composite substrate was doped with Pd nanoparticles via chemical reduction. The resulting Pd–TiO2@PPy nanocomposite was characterized by scanning electron microscopy, transmission electron microscopy, X-ray diffraction, and Brunauer–Emmett–Teller (BET) adsorption analysis before it was utilized to fabricate a hydrogen sensor. Compared with sensors based on TiO2@PPy or PPy, the Pd–TiO2@PPy sensor was highly sensitive and selective to hydrogen gas, exhibiting a fast response time in air at room temperature. The Pd–TiO2@PPy-based sensor exhibited a sensitivity of 8.1% toward 1 vol% of H2 gas, which is much larger than the sensitivities of sensors based on only TiO2@PPy and PPy nanofibers. The excellent reproducibility, stability and selectivity of the Pd–TiO2@PPy nanocomposite make it a high potential candidate for hydrogen sensors. 相似文献
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《Ceramics International》2016,42(16):18597-18604
Pristine and TiO2 nanoparticle-decorated Fe2O3 nanorods were synthesized via thermal oxidation of Fe thin foils, followed by the solvothermal treatment with titanium tetra isopropoxide (TTIP) and NaOH for TiO2 nanoparticle-decoration. Subsequently, gas sensors were fabricated by connecting the nanorods with metal conductors. The structure and morphology of the pristine and TiO2 nanoparticle-decorated Fe2O3 nanorods were examined via X-ray diffraction and scanning electron microscopy, respectively. The gas sensing properties of the pristine and TiO2 nanoparticle-decorated Fe2O3 nanorod sensors with regard to H2S gas were examined. The TiO2 nanoparticle-decorated Fe2O3 nanorod sensor showed a stronger response to H2S than the pristine Fe2O3 nanorod sensor. The responses of the pristine and TiO2 nanoparticle-decorated Fe2O3 nanorod sensors were 2.6 and 7.4, respectively, when tested with 200 ppm of H2S at 300 °C. The TiO2 nanoparticle-decorated Fe2O3 nanorod sensor also showed a faster response and recovery than the sensor made from pristine Fe2O3 nanorods. Both sensors showed selectivity for H2S over NO2, SO2, NH3, and CO. The enhanced sensing performance of the TiO2 nanoparticle-decorated Fe2O3 nanorod sensor compared to that of the pristine Fe2O3 nanorod sensor might be due to enhanced modulation of the conduction channel width, the decorated nanorods’ increased surface-to-volume ratios and the creation of preferential adsorption sites via TiO2 nanoparticle decoration. The dominant sensing mechanism in the TiO2 nanoparticle-decorated Fe2O3 nanorod sensor is discussed in detail. 相似文献