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Measuring Vibration of Body with Speckle Interferometry
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作者 WANG Yunshan(Shandong Polytechnique University, Jinan 250014 CHN) 《Semiconductor Photonics and Technology》 CAS 1996年第1期33-36,48,共5页
Speckle interferometry is an efficient method to analyze a vibration. In certain conditions, this technique has some outstanding advantage, and need not strict shock--proof condition, compared with the holographic met... Speckle interferometry is an efficient method to analyze a vibration. In certain conditions, this technique has some outstanding advantage, and need not strict shock--proof condition, compared with the holographic method for measuring vibration. Therefore,it is suitable to analyze a vibration with a large amplitude.Real-time interferometry is a rapid and simple method for measuring vibration of a body, gives speckle pattern containing amplitude distribution of body-surface. By means of time-averaged method, the speckle pattern is recorded in Fourier transform plane, or vibration lines are seen directly with eyes, so as to analyze efficiently amplitude, phase, and model of a vibration. This paper deduces the intensity distribution function with real-time method, and gives experimental demonstration of vibration body-the vibration lines with different frequencies. 展开更多
关键词 vibration Measurement Speckle Pattern Interferometry vibration line Real-time Method
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Na_(2)高振动态与CO_(2)间碰撞转移概率分布的实验测量
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作者 王淑英 尤德昌 +5 位作者 马文佳 杨若凡 张仰志 於子雷 赵小芳 沈异凡 《光谱学与光谱分析》 SCIE EI CAS CSCD 北大核心 2023年第6期1760-1764,共5页
受激发射泵浦激发Na_(2)至Na_(2)(ν″=30,J″=11)和Na_(2)(ν″=45,J″=11)。Na_(2)(ν″)与CO_(2)碰撞,研究了CO_(2)(00~00)的全态可分辨转动分布及不同的Na_(2)振动能对碰撞猝灭动力学的影响。光学吸收法测量Na_(2)(ν″)与CO_(2)碰... 受激发射泵浦激发Na_(2)至Na_(2)(ν″=30,J″=11)和Na_(2)(ν″=45,J″=11)。Na_(2)(ν″)与CO_(2)碰撞,研究了CO_(2)(00~00)的全态可分辨转动分布及不同的Na_(2)振动能对碰撞猝灭动力学的影响。光学吸收法测量Na_(2)(ν″)与CO_(2)碰撞后的弛豫过程,在一次碰撞的条件下,确定了ν″,ν″-1及ν″-2各振动能级上的转动态分布,而高于ν″的振动能级没有观察到,从而得到碰撞过程中Na_(2)转动能的改变。在碰撞发生1μs后,测量CO_(2)低J态的瞬时线轮廓,利用双Guass函数拟合,得到两个Doppler增宽轮廓,一个是存在于J态粒子的Doppler半宽,一个是被碰撞出J态粒子的Doppler半宽。从存在于J态的Doppler半宽,得到在Na_(2)(ν″)/CO_(2)碰撞中质心平移速度,从而确定平均平移能的增加〈ΔE_(rel)〉。Na_(2)(ν″)振动能的增加与CO_(2)平动能的增加有很大关系,Na_(2)振动能增加35%,而平动能增加56%。从CO_(2)的其他转动态碰到J态的出现速率系数k^(J)_(app)由测量碰撞前和碰撞1μs后的泛频激光感应荧光强度得到总的出现速度系数k_(app)=Σ_(J)k_(app)^(J)=(6.6±1.5)×10^(-10)cm^(3)·molecule^(-1)·s^(-1)[对Na_(2)(ν″=30)]和(5.9±1.3)×10^(-10) cm^(3)·molecule^(-1)·s^(-1)[对Na_(2)(ν″=45)]。因此Na_(2)(ν″)/CO_(2)的碰撞频率对Na_(2)的振动能不是很敏感的。取k_(app)作为参考速率系数,得到了全部能量转移概率分布P(ΔE),这里的ΔE包括了CO_(2)转动能和平动能的变化以及Na_(2)转动能的变化,对于Na_(2)分子振动能的较小增加,会引起P(ΔE)曲线的迅速增宽,在ΔE>500 cm^(-1)以后,Na_(2)(ν″=30)/CO_(2)的P(ΔE)曲线移到了Na_(2)(ν″=45)/CO_(2)的P(ΔE)曲线的下面。P(ΔE)对ΔE在0~3 000 cm^(-1)之间的数值积分给出〈ΔE〉_(trans)=590 cm^(-1)[对Na_(2)(ν″=30)],而对Na_(2)(ν″=45)则给出〈ΔE〉_(trans)=880 cm^(-1)。 展开更多
关键词 碰撞能量转移 激光诱导荧光 瞬时线轮廓 速率系数 能量增加分布函数 Na_(2)高振动激发态 CO_(2)
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DYNAMIC ANALYSIS OF FLEXIBLE BODY WITH DEFINITE MOVING ATTITUTE
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作者 杨元明 张伟 +1 位作者 宋天霞 陈传尧 《Applied Mathematics and Mechanics(English Edition)》 SCIE EI 2006年第1期133-140,共8页
The nonlinear dynamic control equation of a flexible multi-body system with definite moving attitude is discussed. The motion of the aircraft in space is regarded as known and the influence of the flexible structural ... The nonlinear dynamic control equation of a flexible multi-body system with definite moving attitude is discussed. The motion of the aircraft in space is regarded as known and the influence of the flexible structural members in the aircraft on the motion and attitude of the aircraft is analyzed. By means of a hypothetical mode, the defor mation of flexible members is regarded as composed of the line element vibration in the axial direction of rectangular coordinates in space. According to Kane' s method in dynamics, a dynamic equation is established, which contains the structural stiffness matrix that represents the elastic deformation and the geometric stiffness matrix that represents the nonlinear deformation of the deformed body. Through simplification the dynamic equation of the influence of the planar flexible body with a windsurfboard structure on the spacecraft motion is obtained. The numerical solution for this kind of equation can be realized by a computer. 展开更多
关键词 flexible body line element vibration dynamic equation Kane's method
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A numerical approach based on the meshless collocation method in elastodynamics 被引量:1
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作者 Alireza Sadeghirad Iradj Mahmoudzadeh Kani +1 位作者 Mohammad Rahimian Ali Vaziri Astaneh 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 2009年第6期857-870,共14页
In this paper, a collocation technique with the modified equilibrium on line method (ELM) for imposition of Neumann (natural) boundary conditions is presented for solving the two-dimensional problems of linear ela... In this paper, a collocation technique with the modified equilibrium on line method (ELM) for imposition of Neumann (natural) boundary conditions is presented for solving the two-dimensional problems of linear elastic body vibrations. In the modified ELM, equilibrium over the lines on the natural boundary is satisfied as Neumann boundary condition equations. In other words, the natural boundary conditions are satisfied naturally by using the weak formulation. The performance of the modified version of the ELM is studied for collocation methods based on two different ways to construct meshless shape functions: moving least squares approximation and radial basis point interpolation. Numerical examples of two-dimensional free and forced vibration analyses show that by using the modified ELM, more stable and accurate results would be obtained in comparison with the direct collocation method. 展开更多
关键词 Free and forced vibration. Meshless collocation method . Modified equilibrium on line method ~Moving least squares (MLS) - Radial basis functions (RBF)
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