Abstract:An improved method of active structural acoustics control is presented that is based on the minimization of the total power radiated from any structure expressed in terms of a truncated series sum. Each term of this sum is related to the coupling between the orthogonal eigenvectors of the radiation impedance matrix (referred to as ‘‘basis functions’’ in this paper) and the structural surface velocity vector. The basis functions act as surface velocity filters. These acoustic basis functions are found to be wea… Show more
“…Johnson and Elliott 12 extended their earlier work by showing that a substantial reduction in the radiated power on planar structures was obtained at long wavelengths by volume velocity cancellation, clearly demonstrating a close relationship between volume velocity control and control of the dominant acoustic radiation mode. Naghshineh and Koopmann 13,14 applied the technique to structural active noise control, with the objective of forcing the structure to respond in a forced mode of vibration that coincided with an inefficient acoustic radiation mode ͑termed a ''weak radiator''͒. Naghshineh et al 15 demonstrated a design optimization technique such that a subject structure would naturally respond in a structural mode of vibration coinciding with a weak radiation mode, representing an application of the acoustic modal technique to passive control.…”
The use of a modal representation for the exterior acoustic field of a structure has received increasing attention in recent years. This modal approach generally seeks a set of orthogonal functions, representing independent surface velocity distributions, termed acoustic radiation modes, which diagonalize a radiation operator in the exterior domain of the structure. These orthogonal acoustic radiation modes may be found, among other methods, through an eigenvalue analysis of a radiation operator and possess a corresponding set of eigenvalues that are proportional to the radiation efficiencies of the acoustic radiation modes. In free space, the acoustic radiation modes of a sphere display a grouping characteristic in their radiation efficiencies, where each acoustic radiation mode's radiation efficiency within a group has the same frequency dependency. This is a consequence of the fact that the acoustic radiation modes of a sphere are the spherical harmonics. Further, the acoustic radiation modes of an arbitrary three-dimensional structure exhibit the same frequency grouping as those for the sphere. The basis for the arbitrary structure's grouping follows from the sphere's grouping. The observation that the acoustic radiation modes of an arbitrary body are dominated by spherical harmonics provides insight on the behavior of such modes. These results have significance for various applications of acoustic radiation modes, including active noise control design, radiation modeling, etc.
“…Johnson and Elliott 12 extended their earlier work by showing that a substantial reduction in the radiated power on planar structures was obtained at long wavelengths by volume velocity cancellation, clearly demonstrating a close relationship between volume velocity control and control of the dominant acoustic radiation mode. Naghshineh and Koopmann 13,14 applied the technique to structural active noise control, with the objective of forcing the structure to respond in a forced mode of vibration that coincided with an inefficient acoustic radiation mode ͑termed a ''weak radiator''͒. Naghshineh et al 15 demonstrated a design optimization technique such that a subject structure would naturally respond in a structural mode of vibration coinciding with a weak radiation mode, representing an application of the acoustic modal technique to passive control.…”
The use of a modal representation for the exterior acoustic field of a structure has received increasing attention in recent years. This modal approach generally seeks a set of orthogonal functions, representing independent surface velocity distributions, termed acoustic radiation modes, which diagonalize a radiation operator in the exterior domain of the structure. These orthogonal acoustic radiation modes may be found, among other methods, through an eigenvalue analysis of a radiation operator and possess a corresponding set of eigenvalues that are proportional to the radiation efficiencies of the acoustic radiation modes. In free space, the acoustic radiation modes of a sphere display a grouping characteristic in their radiation efficiencies, where each acoustic radiation mode's radiation efficiency within a group has the same frequency dependency. This is a consequence of the fact that the acoustic radiation modes of a sphere are the spherical harmonics. Further, the acoustic radiation modes of an arbitrary three-dimensional structure exhibit the same frequency grouping as those for the sphere. The basis for the arbitrary structure's grouping follows from the sphere's grouping. The observation that the acoustic radiation modes of an arbitrary body are dominated by spherical harmonics provides insight on the behavior of such modes. These results have significance for various applications of acoustic radiation modes, including active noise control design, radiation modeling, etc.
“…Since then the sound radiation efficiency and active control of thin plate had been studied [6,7]. Based on the acoustic radiation modes and further study about acoustic radiation, ADS (Acoustic Design Sensitivity) analysis [8,9,10] was presented to guide Low Noise Design of structures.…”
In this paper, optimization design for minimization sound radiation from thin plate based on ADS (Acoustic Design Sensitivity) analysis is studied. Firstly, the velocity distribution of structure surface is solved by analytical method and the surface sound pressure is computed by Rayleigh integral respectively. The sound radiation power of structure can be expressed as a positive definite quadratic form of the Hermitian by impedance matrix. Then, the relationship between the sound radiation power and thickness of thin plate is analyzed. The ADS analysis of thin plate can be translated into the analysis of structure dynamic sensitivity and impedance matrix sensitivity. Finally, optimization design for sound power minimization of thin plate base on the gradient-based optimization algorithms is presented. Thicknesses are chosen as design variables. Taking a simple supported thin plate as a simulation example, the results show the validity of the presented method and give the optimal design of thin plate.
“…Sensing strategies using velocity information can also be based on so-called radiation modes, 6 which are the vibration patterns of a structure that radiate sound independently in free space [7][8][9][10][11][12][13] or in enclosed spaces. 14,15 The resulting control strategy is optimal with respect to the number of error signals for the controller.…”
Efficient sensing schemes for the active reduction of sound radiation from plates are presented based on error signals derived from spatially weighted plate velocity or near-field pressure. The schemes result in near-optimal reductions as compared to weighting procedures derived from eigenvector or singular vector analysis of the radiation operator. Efficient control configurations are suggested using a, possibly analog, front-end implementing a bank of spatial weighting functions and a digital controller with a minimized number of input and output channels. The performance of different weighting functions is compared, as well as the performance of different frequency-dependent filtering functions. Design rules are given for the sensor spacing, the number of weighting functions, the number of actuators, and the corresponding controller dimensionality.
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