Authors: Jun Yang, Xu Shi Lu, Jia Fan Zhang, Hua Jiang Ouyang
Abstract: A necessary and sufficient condition is proposed for the incremental mass and stiffness matrices that modify some eigenpairs while keeping other eigenpairs unchanged, which requires the knowledge of only the few eigenpairs to be modified of the original undamped vibration system. The application prospects are proposed based on this formulation.
475
Authors: Hai Yang Gao, Xing Lin Guo, Pei Jun Hou, Cheng Wei Wu, Hua Jiang Ouyang
Abstract: This paper presents a two-stage scheme of damage identification for plate-type structure. In the first stage, probable damaged regions and their relative severities can be detected based on lock-in thermography technique. In the second stage, the relation between the damage level and its corresponding natural frequencies of the plate is constructed by means of Kriging surrogate model based on dynamic analysis. The inverse problem of damage quantification over the surrogate model is then solved by using a robust stochastic particle swarm optimization algorithm. Experimental study on a double-damaged plate demonstrates the feasibility and effectiveness of the proposed scheme.
839
Authors: M. N. Abdul Rani, D. Stancioiu, M.A. Yunus, Hua Jiang Ouyang, H. Deng, S. James
Abstract: Dynamic behaviour of a welded structure made from thin metal sheets which has a large flat surface and has been assembled together by a number of scattered spot welds is investigated. An impact hammer and roving accelerometers are used in the modal tests to provide data to update the FE model. NASTRAN Solution 103 is used to compute natural frequencies and modes of interest. The large error of the initial FE model is largely reduced mainly by adjusting a crucial parameter of the bending moment of inertia ratio, 12I/T**3.
117
Authors: Nurulakmar Abu Husain, Andy Snaylam, Hamed Haddad Khodaparast, S. James, Geoff Dearden, Hua Jiang Ouyang
Abstract: Finite Element (FE) model updating is initially developed to update numerical models of structures to match their experimentally measured modal properties (i.e., natural frequencies and modes). In FE model updating, uncertain physical parameters of a structure are modified so that the discrepancies between the numerically estimated and experimentally measured modal properties are minimized. The process of updating is employed not only in parameter identification; it can also be developed for structural damage identification.
In this work, a welded structure that is intended to represent a common configuration used in automotive body construction is investigated. It is known that presence of any damage in the welds of such a structure could affect its dynamic behavior. So, in theory modal test data can allow damage to be assessed accurately. As a typical automotive body contains thousands of welds, the effects of damage in the welds could be influential.
The FE model updating process using experimental data is presented. It is carried out using NASTRAN optimization code. The procedure aims to adjust the uncertain properties of the FE model (from the weld joints) by minimizing the differences between the measured modal properties and the corresponding numerical predictions. The initial parameter values used in the numerical model are the nominal values. The procedure brings the numerical results of the structure as close as possible to the experimental ones, according to an objective function, therefore altering some of the FE model parameters of the structure. It may be concluded that when the identified values of certain parameters deviates from the nominal values to certain extent, there is a fault or damage at that particular joint.
393
Authors: Luis Baeza, Hua Jiang Ouyang
Abstract: This paper presents a method for the vibration of a beam with a breathing crack under harmonic excitation. The infinitely thin crack is characterised by a parameter that takes into account the shape and the depth of the crack. The closed- and open-crack states are both modelled by a modal approach: two sets of equations of motion cast in the modal coordinates of their individual mode shapes. The state change (from closed to open or vice versa) involves the calculation of the modal coordinates associated with the new state from the modal coordinates of the previous state. By imposing the continuity of displacement and velocity the beam at the instant of the state change, the matrix that transforms the modal coordinates from one state to the other is determined and proved to be the Modal Scale Factor matrix. This analytical approach takes advantage of exact nature and mathematical convenience of beam modes and is time-efficient. Forced vibration at various values of crack parameter is determined. It is found that as decreases (crack length increases) the vibration becomes increasingly erratic and finally chaotic.
39
Authors: Hua Jiang Ouyang, John E. Mottershead
Abstract: The vibration of a beam excited by a moving simple oscillator is an extensively studied
problem. However, the vibration of a beam excited by an elastic body with conformal contact has
attracted much less attention. This is the subject of the present paper. The established model is a big
improvement to the moving oscillator model and has many engineering applications.
Because the moving body is flexible, the moving loads at the contact interface are not known a
priori and must be determined together with the dynamics of the whole system. Considerable
mathematical complication arises as a result, compared with the moving-oscillator problem, even if
the contact is assumed to be complete. In this paper, the equation of motion of the beam and the
moving body are established separately using an analytical-numerical combined approach. The
equation for the moving loads is established through the displacement continuity at the contact
interface. It is found from the simulated numerical results that the deflection of the beam displays
several cycles of oscillation during the passage of the moving body and can exceed the maximum
static deflection at moderate speeds, but is close to the static deflection when the speed is either
very low or very high.
457
Authors: Matthew Oldfield, Hua Jiang Ouyang, John E. Mottershead, Andreas Kyprianou
421
Authors: Q. Cao, Michael I. Friswell, Hua Jiang Ouyang, John E. Mottershead, S. James
269
Authors: S. James, Hua Jiang Ouyang, D.J. Brookfield, John E. Mottershead
237
Authors: John E. Mottershead, Andreas Kyprianou, Hua Jiang Ouyang
157