三圆弧谐波齿轮传动齿廓设计

基于谐波齿轮传动共轭精确求解方法，提出三圆弧谐波齿轮传动齿廓设计方法，并研究了三圆弧柔轮齿廓参数对谐波传动共轭区间的影响。研究结果表明，三圆弧谐波齿轮传动较双圆弧谐波齿轮传动具有更宽的共轭区间和更小的共轭间隔区间；减少凸齿廓圆弧半径有利于增加谐波传动共轭区间，但不利于减少共轭间隔区间；减少中间圆弧半径、夹角δ1和δ2既利于增加谐波传动共轭区间，也利于减少共轭间隔区间；凹齿廓圆弧半径对实际共轭区间影响很小。合理选择柔轮齿廓参数可有效减少共轭间隔区间，增加共轭区，减少尖点啮合，增加齿间共轭接触，从而提高谐波齿轮传动精度和扭转刚度

双圆弧谐波齿轮传动柔轮齿廓参数对侧隙的影响

在谐波齿轮传动中,空载啮合侧隙对其传动性能有显著影响。基于谐波传动共轭精确求解方法,研究了谐波齿轮传动共轭区间、刚轮理论共轭齿廓和侧隙随柔轮齿廓参数的变化规律。研究结果表明,柔轮齿廓参数对啮合共轭区间、刚轮理论共轭齿廓和侧隙具有决定性作用。减少凸齿廓圆弧半径有利于增加啮合共轭区间,但不利于减小侧隙;凹齿廓圆弧半径对共轭区间影响不明显,对侧隙影响较大;减小公切线倾角有利于增加共轭区间,也有利于减小侧隙值和改善侧隙分布;凸齿廓、凹齿廓圆弧半径对刚轮齿廓参数影响明显,公切线倾角对刚轮齿廓参数几乎无影响。合理选择柔轮齿廓参数能够获得更大的共轭区和更均匀的侧隙分布,从而提高承载能力和传动性能

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