Abstract

The distribution of sound intensity in space (pattern function) from a line source of finite length is given by an integral involving the distribution of source strength along the line of the source (excitation function). Synthesizing a desired pattern function with a given length of source requires the solution of an integral equation for the excitation function. Practical solutions may be obtained by expressing the pattern function as a finite sum of “characteristic functions” and obtaining the excitation function as a similar sum of complementary functions. One such scheme relates the zeroes of the pattern function to the coefficients of the Fourier expansion of the excitation function. Equal-minor-lobe patterns may be approximated, but the solution is not obtained in closed form as with linear point-source arrays.

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.