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利用振动特性变化对结构进行无损检测,是近期损伤检测领域的热门研究课题.振动特性能够反映结构的状态,损伤的产生会导致桥梁某些振动参数的变化.为了研究应用加速度反应功率谱密度这一振动特性进行钢桥损伤识别方法,本文采用废止铁路线钢桥为试件,并人工预置6种工况损伤.利用正弦扫频波激振钢桥,分析其损伤前后加速度反应功率谱密度的变化.实验结果表明,利用加速度反应功率谱密度变化能够准确识别并定位钢桥损伤的位置.  相似文献   
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利用HI-13串列加速器提供的19 MeV 质子照射麻醉小鼠2, 4, 8和16 Gy , 照射后不同时间麻醉处死小鼠进行病理组织学观察。 结果显示, 照射后各组小鼠腰背部开始环状脱毛, 病理改变为表皮细胞坏死、 脱落, 皮下水肿, 心、 肝出现小灶性坏死或伴出血, 肝细胞明显再生, 肺组织可出现充血及肺泡间隔明显增厚, 肾小球出现明显固缩、 坏死及消失。 这些病理改变在大剂量照射组尤为明显。 通过观察质子照射小鼠组织病理损伤效应, 为质子损伤的防治研究提供参考依据。Space radiation come from galactic cosmic rays and solar particle events which contain considerable protons is an invisible killer to astronauts. Furthermore, many wounded persons were injured by proton and other heavy ion radiation in a nuclear warhead or nuclear terrorism attack. However, the damage effect of proton radiation is known little in our country. In this study, the proton induced histopathologic changes of mice were observed primarily. naesthetic mice were irradiated with the 19 MeV protons dili vered by HI 13 tandem accelerator at CIAE in different doses(2, 4, 8, 16 Gy). In order to observe the da mage effect, mice were killed by anaesthetic at different time point after radiation, and the tissue sections were analyzed by a histopathologic method. The results show that all of the mice’s backs began displaying ringed depilation at post irradiation day 7. Many epidermal cells necrosis and exfoliation happened, and subcutaneous dropsy was observed. There were some focal necrosis or even followed with bleeding in heart and liver. Hepatocyte evidently regenerated. A hyperaemia was seen in lung tissue and alveolar septum was obviously thickening. Acinus renis represented notable pyknosis, necrosis and disappearance. Especially, these pathologic alteration clearly displayed in high dose groups. In conclusion, proton radiation can induce different grade injury to skin, heart, liver, lung, kidney and other organs. Further studies should be made to deeply understand the mechanism about the proton radiation damage.  相似文献   
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报道了一种内腔光参量振荡器,该器件通过改变多通道MgO∶PPLN极化晶体的极化周期和温度,可以快速实现3.2~4.1μm中红外参量光可调谐连续输出.采用1.064μm谐振腔与多光参量振荡腔折叠型复合结构,考虑晶体热效应及宽范围调谐参量光振荡过程中光斑模式匹配,通过对两个子腔谐振结构的数值模拟分析,确定最佳腔型结构参数.基于该谐振腔结构,实验研究了多周期MgO∶PPLN晶体的温度和极化周期对参量光波长的影响,实验中克服了MgO∶PPLN晶体在3.8~4.1μm中红外波段较为严重的本征吸收以及量子亏损导致的效率降低问题,获得2.78~4.18μm中红外激光连续调谐输出,调谐范围达1.399μm.在3.2μm、3.5μm、3.8μm、4.1μm四个典型波长下实现了参量光输出,功率分别为1.72W、1.39W、0.79W和0.442W,对应转化效率分别为7.17%、5.4%、3.1和1.84%.  相似文献   
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本文在室温下利用射频磁控溅射技术在(001)蓝宝石衬底上制备了不同厚度的β-Ga2O3薄膜,随后将其置于氩气气氛中800℃退火1 h.利用XRD,SEM,UV-Vis分光光度计、PL光致发光光谱仪和Keithley 4200-SCS半导体表征系统等考察薄膜厚度对所得氧化镓薄膜相组成、表面形貌、光学性能以及光电探测性能的影响.结果表明,随着薄膜厚度的增加,薄膜结晶质量提高,840 nm薄膜最佳,1050 nm薄膜结晶质量略有降低.不同厚度β-Ga2O3薄膜在波长200—300 nm日盲区域内均具有明显的紫外光吸收,禁带宽度随着薄膜厚度的增加而增加.PL谱中各发光峰峰强随着薄膜厚度的增加而减小,表明氧空位及其相关缺陷受到抑制.在β-Ga2O3薄膜基础上制备出日盲紫外光电探测器的探测性能(光暗电流比,响应度,探测率,外量子效率)也随薄膜厚度的增加呈先增后减的趋势.厚度约为840 nm的β-Ga2O3紫外光电探测器,在5...  相似文献   
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