Directionality of sound radiation from rectangular panels

Abstract In this paper, the directionality of sound radiated from a rectangular panel, attached with masses/springs, set in a baffle, is studied. The attachment of masses/springs is done based on the receptance method. The receptance method is used to generate new mode shapes and natural frequencies of the coupled system, in terms of the old mode shapes and natural frequencies. The Rayleigh integral is then used to compute the sound field. The point mass/spring locations are arbitrary, but chosen with the objective of attaining a unique directionality. The excitation frequency to a large degree decides the sound field variations. However, the size of the masses and the locations of the masses/springs do influence the new mode shapes and hence the sound field. The problem is more complex when the number of masses/springs are increased and/or their values are made different. The technique of receptance method is demonstrated through a steel plate with attached point masses in the first example. In the second and third examples, the present method is applied to estimate the sound field from a composite panel with attached springs and masses, respectively. The layup sequence of the composite panel considered in the examples corresponds to the multifunctional structure battery material system, used in the micro air vehicle (MAV) (Thomas and Qidwai, 2005). The demonstrated receptance method does give a reasonable estimate of the new modes.

[1]  Jie Pan,et al.  Actively created quiet zones for broadband noise using multiple control sources and error microphones , 1999 .

[2]  J. S. Lamancusa,et al.  SOUND POWER MINIMIZATION OF CIRCULAR PLATES THROUGH DAMPING LAYER PLACEMENT , 1998 .

[3]  W. Soedel,et al.  Natural frequencies and modes of cylindrical polygonal ducts using receptance methods , 1986 .

[4]  Alain Berry,et al.  A general formulation for the sound radiation from rectangular, baffled plates with arbitrary boundary conditions , 1990 .

[5]  Muhammad A. Qidwai,et al.  The design and application of multifunctional structure-battery materials systems , 2005 .

[6]  Mayuresh J. Patil,et al.  Aeroelastic Tailoring of Flapping Membrane Wings for Maximum Thrust and Propulsive Eciency , 2012 .

[7]  L. Cremer,et al.  Structure-Borne Sound: Structural Vibrations and Sound Radiation at Audio Frequencies , 1973 .

[8]  W. L. Li,et al.  ACOUSTIC RADIATION FROM A RECTANGULAR PLATE REINFORCED BY SPRINGS AT ARBITRARY LOCATIONS , 1999 .

[9]  Arthur W. Leissa,et al.  Vibration of Plates , 2021, Solid Acoustic Waves and Vibration.

[10]  W. L. Li Vibroacoustic analysis of rectangular plates with elastic rotational edge restraints , 2006 .

[11]  W. Soedel Vibrations of shells and plates , 1981 .

[12]  C. S. Jog Reducing Radiated Sound Power by Minimizing the Dynamic Compliance , 2002 .

[13]  W. Soedel,et al.  Reply by one of the authors , 1987 .

[14]  Jinwu Xu,et al.  Vibration analysis of submerged rectangular microplates with distributed mass loading , 2009, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[15]  Earl G. Williams,et al.  Numerical evaluation of the radiation from unbaffled, finite plates using the FFT , 1983 .

[16]  Pattabhi R. Budarapu,et al.  Aero-Elastic Analysis of Stiffened Composite Wing Structure , 2009 .

[17]  Jean C. Piquette Direct measurements of edge diffraction from soft underwater acoustic panels , 1994 .

[18]  Julian D. Maynard,et al.  Numerical evaluation of the Rayleigh integral for planar radiators using the FFT , 1982 .

[19]  Fernand Léon,et al.  Acoustic radiation of a submerged cylindrical shell in low frequency. , 2013, The Journal of the Acoustical Society of America.

[20]  Philip A. Nelson,et al.  The active minimization of harmonic enclosed sound fields, part III: Experimental verification , 1987 .

[21]  D. T. Huang,et al.  Study of the Forced Vibration of Shell-Plate Combinations Using the Receptance Method , 1993 .

[22]  Frank Fahy The Vibro-Acoustic Reciprocity Principle and Applications to Noise Control , 1995 .

[23]  David Thompson,et al.  Sound radiation from rectangular baffled and unbaffled plates , 2010 .

[24]  D. T. Soedel,et al.  Synthesizing reduced systems by complex receptances , 1995 .

[25]  T. Y. Yang,et al.  Eigenvalues of rings with radial spring attachments , 1988 .

[26]  Frank Fahy,et al.  Sound and Structural VibrationRadiation, Transmission and Response , 2007 .

[27]  W. Soedel,et al.  Simplified prediction of the modal characteristics of ring-stiffened cylindrical shells , 1976 .

[28]  W. Soedel,et al.  The receptance method applied to ring-stiffened cylindrical shells: Analysis of modal characteristics , 1976 .

[29]  A. Belegundu,et al.  Material tailoring of structures to achieve a minimum radiation condition , 1992 .

[30]  Venkata R. Sonti Sound radiation from a baffled rectangular plate under a variable line constraint , 2003 .

[31]  Xuefeng Zhang,et al.  A unified approach for predicting sound radiation from baffled rectangular plates with arbitrary boundary conditions , 2010 .

[32]  Wen L. Li,et al.  Reducing sound radiation from a plate through tuning/modifying boundary supports , 2009 .

[33]  Steven Dubowsky,et al.  A RADIATION EFFICIENCY FOR UNBAFFLED PLATES WITH EXPERIMENTAL VALIDATION , 1997 .

[34]  G. Koopmann,et al.  GLOBAL OPTIMUM ACTIVE NOISE CONTROL : SURFACE AND FAR-FIELD EFFECTS , 1991 .

[35]  S. Elliott,et al.  Radiation modes and the active control of sound power , 1993 .

[36]  Edward C. Ting,et al.  Vibration of plates with sub-structural deduction: a reverse receptance approach , 2004 .

[37]  W. Soedel,et al.  The receptance method applied to the free vibration of continuous rectangular plates , 1984 .

[38]  P.-O. Mattei Sound radiation by baffled and constrained plates , 1995 .

[39]  L. Rayleigh,et al.  The theory of sound , 1894 .

[40]  Venkata R. Sonti,et al.  Curved piezoactuator model for active vibration control of cylindrical shells , 1996 .