消防喷淋末端支管全自动精准测量施工技术

本文结合实际工程,介绍了消防喷淋末端支管全自动精准测量施工工艺流程及施工技术要点.该施工技术提高了消防喷淋末端追位的施工质量,解决了天花板上极易出现点位位置偏移、喷淋头凹陷或者凸出等问题,提高了集中预制加工生产效率,可为同类工程提供参考.     

2,5-二氢噻吩-3,4-二羧酸酐的合成工艺优化

以3-氧代-4-甲酸甲酯四氢噻吩与氰化钠为原料,通过氰醇化、脱水、水解等反应合成了2,5-二氢噻吩-3,4-二羧酸酐(4),化合物4通过~1H NMR、~(13)C NMR、高分辨质谱(HRMS)等表征。研究了溶剂、反应温度以及不同配比的溶剂对合成2,5-二氢噻吩-3-4-二羧酸酐中间体的影响。制备3-氰基-4-甲酸甲酯-2,5-二氢噻吩(2)的较优条件为:POCl_3∶3-氰基-3-羟基-4-甲酸甲酯四氢噻吩(1)=2.5(物质的量比);制备2,5-二氢噻吩-3,4-二羧酸(3)的较优条件为:温度80℃,化合物2 1 g,乙酸2.9 mL,浓盐酸4.8 mL。对3-氰基-4-甲酸甲酯-2,5-二氢噻吩进行了~1H NMR、~(13) C NMR、HRMS表征。     

液相沉淀-煅烧法制备大粒径球形四氧化三钴

以硫酸钴为原料,碳酸氢铵为沉淀剂,采用液相沉淀法合成了大粒径球形碳酸钴,考察了不同晶种量、pH和硫酸钴溶液流量对碳酸钴形貌、粒度分布、振实密度和硫元素质量分数的影响,并探究了碳酸钴的生长机理。通过分步煅烧,并设置不同升温时间使碳酸钴热分解,得出优化四氧化三钴理化指标的煅烧条件。结果表明,当晶种量为2 kg,pH在7.2～7.5,硫酸钴溶液流量为500 mL/h时,采用分段式热分解碳酸钴,各温区按统一时间(60 min)升温,所得四氧化三钴形貌为球形,中值粒径为16.52μm,振实密度达2.26 g/cm3。     

基于SCAE⁃ACGAN的直升机行星齿轮裂纹故障诊断

直升机行星传动轮系结构复杂、工况多变,其振动信号受工况影响大,在故障样本较少的情况下导致行星齿轮箱故障诊断准确率不高,早期故障诊断困难。针对上述问题,提出将堆栈收缩自动编码网络(stacked contractive autoencoder,简称SCAE)与辅助分类生成式对抗网络(auxiliary classifier generative adversarial networks,简称ACGAN)相结合的SCAE-ACGAN故障诊断方法。ACGAN的生成器产生与真实样本具有类似分布的生成样本,扩展训练样本集,并与真实样本一起输入至判别器进行训练。ACGAN采用SCAE作为判别器,利用SCAE良好的抗数据波动能力,从扩展样本集中挖掘出有效的深度特征,并实现样本的真伪与类别的判定。ACGAN的判别器和生成器在对抗学习训练机制下交替优化,提高方法的样本生成质量与故障判定能力。将SCAE-ACGAN应用于直升机行星轮裂纹故障诊断,结果表明,SCAE-ACGAN的故障诊断性能好,在样本数量少与工况变化情况下具有较好的健壮性和适应性。     

基于变功率因数的分散式风电场优化运行策略

提出一种考虑负荷类型和风电机组无功极限的分散式风电场优化运行策略。建立基于静态电压特性的典型负荷通用模型;挖掘分散式风电机组无功能力,采用机端并联电容器平衡并提高双馈感应发电机无功调节能力;分析风电机组功率因数对配电网各节点电压、有功和无功网损影响规律;在此基础上,提出基于改进萤火虫算法的分散式风电场最优功率因数运行方法。基于IEEE-33节点模型进行仿真计算,结果表明:分散式风电场小范围功率因数优化调节可有效减小配电网网损,提高电压稳定性。     

Enhancement of optical emission generated from femtosecond double-pulse laser-induced glass plasma at different sample temperatures in air

In double-pulse laser-induced breakdown spectroscopy(DP-LIBS), the collinear femtosecond double-pulse laser configuration is experimentally investigated with different initial sample temperatures using a Ti:sapphire laser. The glass sample is ablated to produce the plasma spectroscopy. During the experiment, the detected spectral lines include two Na(I) lines(589.0 nm and 589.6 nm) and one Ca(I) line at the wavelength of 585.7 nm. The emission lines are measured at room temperature(22 ℃) and three higher initial sample temperatures(T_s?=?100 ℃, 200 ℃, and 250 ℃). The inter-pulse delay time ranges from-250 ps to 250 ps.The inter-pulse delay time and the sample temperature strongly influence the spectral intensity,and the spectral intensity can be significantly enhanced by increasing the sample temperature and selecting the optimized inter-pulse time. For the same inter-pulse time of 0 ps(single-pulse LIBS), the enhancement ratio is approximately 2.5 at T_s?=?200 ℃ compared with that obtained at T_s?=?22 ℃. For the same inter-pulse time of 150 ps, the enhancement ratio can be up to 4 at T_s?=?200 ℃ compared with that obtained at T_s?=?22 ℃. The combined enhancement effects of the different initial sample temperatures and the double-pulse configuration in femtosecond LIBS are much stronger than that of the different initial sample temperatures or the double-pulse configuration only.