Dynamic investigations revealed that lower order harmonic resonance phenomenon exists in the three ring gear transmission. That is, when the input speed is close to 1/3, 1/6, 1/9,…, 1/3 n of the primary natural frequ...Dynamic investigations revealed that lower order harmonic resonance phenomenon exists in the three ring gear transmission. That is, when the input speed is close to 1/3, 1/6, 1/9,…, 1/3 n of the primary natural frequency of the transmission, the loads on the bearings and gears are especially high. This paper explained this phenomenon from the viewpoint of parametric resonance in terms of perturbation technique. A conclusion was drawn that the basic reason for this phenomenon is the primary resonance caused by forcing excitation and parametric resonance caused by parametric change.展开更多
基金Supported by National Natural Science Foundation of China(61308056,61008025,11232015,11072271 and 11204044)the Research Fund for the Doctoral Program of Higher Education of China(20120171110005 and 20130171130003)+1 种基金Guangdong Natural Science Foundation(S2012010010172)Opening Project of Science and Technology on Reliability Physics and Application Technology of Electronic Component Laboratory(ZHD201203)
基金Partly supported by the Open Fund of theState Key Lab.of Mechanical TransmissionChongqing U niv
文摘Dynamic investigations revealed that lower order harmonic resonance phenomenon exists in the three ring gear transmission. That is, when the input speed is close to 1/3, 1/6, 1/9,…, 1/3 n of the primary natural frequency of the transmission, the loads on the bearings and gears are especially high. This paper explained this phenomenon from the viewpoint of parametric resonance in terms of perturbation technique. A conclusion was drawn that the basic reason for this phenomenon is the primary resonance caused by forcing excitation and parametric resonance caused by parametric change.
文摘通过1 064 nm激光泵浦KTP晶体光参量振荡(OPO)技术获得了高峰值功率2.7μm波段激光输出,对实验结果开展了详细的分析。泵浦源为电光调Q Nd:YAG激光器,光参量振荡器谐振腔采用单谐振结构,将两块相同的KTP晶体光轴相向放置以补偿走离效应,KTP晶体按?=0°,θ=62°切割以获得波长2.7μm波段激光输出,采用Ⅱ(B)类相位匹配(o→o+e)以利用较大的非线性系数。在泵浦能量为89 m J,脉宽10 ns的条件下,获得脉冲能量7.5 m J,波长2.67μm,脉宽8.5 ns的激光输出。
基金Supported by the National Natural Science Foundation of China under Grant No 10474105, and the National Basic Research Programme of China under Grant No 2006CB921202.
