5 research outputs found

    Design and Analysis of Elastic Component of Resonant Cylinder Pressure Sensor

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    利用有限元分析软件AnSyS对振筒式压力传感器弹性元件——谐振筒进行了动态特性仿真分析,建立了谐振筒的参数化模型,基于模态分析选定合适的工作振型,重点利用谐响应分析讨论了谐振筒品质因数的影响因素。研究表明,当谐振筒的基模态为(4,1)模态时,品质因数随谐振筒外半径、有效长度以及壁厚的增加而减小,而工作时作用于谐振筒的激励载荷只改变了谐振筒振幅大小,对品质因数无明显影响。通过瞬态动力学分析计算得到谐振筒的调节时间,证明了谐振筒具有较好的动态响应特性。为谐振筒的结构设计和优化提供了参考。Simulation and analysis on dynamic behavior of resonant cylinder which composed the pressure sensor as the elastic component are conducted using the finite element analysis software ANSYS.Parametric model is established.Based on the modal analysis,an appropriate mode for work is selected out.Factors affecting quality factor are discussed mainly through harmonic response analysis.Results indicate that,when the cylinder worked on(4,1) mode,quality factor would decreases as radius,effective length or thickness increase,while the force only had an influence on the amplitude of the vibration rather than the quality factor.Adjusting time is obtained by transient dynamic analysis,thus proving the rapidity of resonant cylinder.The study provides reference both for structure design and optimization

    Electrohydrodynamic printing for head with retractable needle

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    设计了一种新型的基于电液动力学的喷头,该喷头内含一个可伸缩的针尖。由这种喷头组成的喷印系统,在不同的条件下可以产生离散的点和珠状结构两种喷射模式。结果表明:溶液浓度是区分这两种喷射模式的关键因素。当喷射溶液的浓度比较低时,喷印系统喷射出离散的圆点;当较高时,喷射出珠状结构。其珠状结构中珠子的直径随着系统供液速率的增加而变大,随着PEO溶液浓度的提高和针尖频率的增加而减小。改变收集板的移动速度,可以改变喷射沉积物形态,且该系统的喷射频率与可伸缩针尖的运动频率之间有很好的线性相关性。A novel electrohydrodynamic printing system with a retractable needle was designed,by which both ejection modes of dots and bead-on-string structures can be produced.Experimental results show that solution concentration is the key element to define the ejection mode.Dots can be obtained for lower solution concentration,otherwise bead-on-string structures would be produced.the diameter of deposition dots increases with the increasing of supply rate,and decreases with the increasing of PEO solution concentration and the frequency increasing of needle.By changing the speed of collector,different morphologies of depositions can be obtained.In addition,the deposition frequency has a close relationship with the retractable frequency of needle.中央高校基本科研业务费专项资金(2010121039);国家自然科学基金(51035002;50875222

    JUNO Sensitivity on Proton Decay pνˉK+p\to \bar\nu K^+ Searches

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    The Jiangmen Underground Neutrino Observatory (JUNO) is a large liquid scintillator detector designed to explore many topics in fundamental physics. In this paper, the potential on searching for proton decay in pνˉK+p\to \bar\nu K^+ mode with JUNO is investigated.The kaon and its decay particles feature a clear three-fold coincidence signature that results in a high efficiency for identification. Moreover, the excellent energy resolution of JUNO permits to suppress the sizable background caused by other delayed signals. Based on these advantages, the detection efficiency for the proton decay via pνˉK+p\to \bar\nu K^+ is 36.9% with a background level of 0.2 events after 10 years of data taking. The estimated sensitivity based on 200 kton-years exposure is 9.6×10339.6 \times 10^{33} years, competitive with the current best limits on the proton lifetime in this channel

    JUNO sensitivity on proton decay pνK+p → νK^{+} searches

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    JUNO sensitivity on proton decay p → ν K + searches*

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    The Jiangmen Underground Neutrino Observatory (JUNO) is a large liquid scintillator detector designed to explore many topics in fundamental physics. In this study, the potential of searching for proton decay in the pνˉK+ p\to \bar{\nu} K^+ mode with JUNO is investigated. The kaon and its decay particles feature a clear three-fold coincidence signature that results in a high efficiency for identification. Moreover, the excellent energy resolution of JUNO permits suppression of the sizable background caused by other delayed signals. Based on these advantages, the detection efficiency for the proton decay via pνˉK+ p\to \bar{\nu} K^+ is 36.9% ± 4.9% with a background level of 0.2±0.05(syst)±0.2\pm 0.05({\rm syst})\pm 0.2(stat) 0.2({\rm stat}) events after 10 years of data collection. The estimated sensitivity based on 200 kton-years of exposure is 9.6×1033 9.6 \times 10^{33} years, which is competitive with the current best limits on the proton lifetime in this channel and complements the use of different detection technologies
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