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机构地区:[1]后勤工程学院,重庆401331
出 处:《物理学报》2015年第22期284-293,共10页Acta Physica Sinica
基 金:国家自然科学基金(批准号:11474361;11274388)资助的课题~~
摘 要:采用界面弹簧模型对圆管结构的管间界面特性进行描述,推导出含弱界面的圆管结构中声波沿周向传播时的位移场及应力场的数学表达式.在此基础上采用导波的模式展开分析方法,给出了与管间界面特性及激励源密切相关的周向超声导波模式展开系数的解析表达式.数值分析了管间界面特性的变化对周向超声导波的频散和声场产生的影响.理论与数值分析结果表明,通过选择适当的驱动频率及周向导波模式,可使周向超声导波的相速度及圆管外表面的位移场随管间界面特性的变化表现出非常敏感且单调的性质.这一结果有助于采用周向超声导波方法准确定征圆管结构的管间界面特性.The mathematical expressions both of displacement and stress fields of circumferential wave propagation in circular tube structure with a weak interface are derived on condition that the interracial properties between the two circular tubes are characterized by the interracial spring model. Based on the said displacement and stress expressions derived, the dispersion equation of ultrasonic guided circumferential wave (UGCW) modes is formally presented by using the corresponding mechanical boundary conditions. According to the technique of modal expansion analysis for waveguide excitation, for a given excitation source used to generate circumferential wave in circular tube structure, the corresponding field of circumferential wave propagation can be decomposed into a series of UGCW modes. Using the reciprocity relations and mode orthogonality, the analytical expression of UGCW mode expansion coefficient is derived, which is closely related to the given excitation source for UGCW generation and the interfacial properties between the two tubes. The influences of change in the interfacial property on dispersion and acoustic field of the UGCW propagation are numerically analyzed. In the cases of perfect and sliding interfaces, for a given UGCW mode, the relative change rate of phase velocity is defined, and then its curve versus frequency is calculated, through which the specific frequency can be determined where the UGCW phase velocity appears to be most sensitive to the change in the interfacial property. For a given UGCW mode and driving frequency, it is numerically found that the displacement field on the outside surface of the circular tube structure changes sensitively and monotonically with change in interfacial property between the tubes. Clearly, through choosing the appropriate driving frequency and the mode of UGCW propagation, both the UGCW phase velocity and the displacement field on the outside surface of the circular tube structure will be monotonic and sensitive to change in interfacial property. I
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