摆动支点可变的平底从动件凸轮连杆机构的综合

研究了在烟草机械清洗设备中使用的一种摆动支点可变的平底从动件凸轮连杆组合机构。该机构将摆动从动件的枢轴安装在轨迹方向可调的滑块上，从动件进行复杂的平面运动，其输出角度的运动范围可根据输出要求进行调整。为了综合该机构，首先，建立了相关模型；然后，采用反转法和包络理论，推导了凸轮轮廓坐标求解模型；最后，选择相应的从动件运动规律，计算相应的凸轮轮廓坐标，通过插值得到整个凸轮轮廓曲线。利用该过程设计了实例机构的运动凸轮，并通过运动仿真进行了验证。研究工作解决了实际装备的设计问题，也丰富了凸轮-连杆机构的设计理论

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

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 $p\to \bar\nu K^+$ 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 $p\to \bar\nu K^+$ 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 $9.6 \times 10^{33}$ years, competitive with the current best limits on the proton lifetime in this channel

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

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 $p\to \bar{\nu} K^+$ 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 $p\to \bar{\nu} K^+$ is 36.9% ± 4.9% with a background level of $0.2\pm 0.05({\rm syst})\pm$$0.2({\rm stat})$ events after 10 years of data collection. The estimated sensitivity based on 200 kton-years of exposure is $9.6 \times 10^{33}$ years, which is competitive with the current best limits on the proton lifetime in this channel and complements the use of different detection technologies