1995
DOI: 10.1121/1.413666
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Local active control of diffracted diffuse sound fields

Abstract: The average spatial extent of the zone of quiet created by a local active control system in a diffuse enclosed sound field has been investigated using computer simulation and measured experimentally. The secondary source is modeled as a rigid sphere with a pulsating segment and its diffracting effect on a diffuse primary pressure field has been simulated. The diffraction effects of a hypothetical listener’s head, modeled as rigid sphere, on both the primary and secondary acoustic fields have also been calculat… Show more

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Cited by 33 publications
(28 citation statements)
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“…The presence of a rigid sphere affects the secondary sound field by imposing zero particle velocity, and thus zero pressure gradient. As has been shown by Garcia-Bonito and Elliott, this results in a beneficial flattening of the secondary field which tends to increase the spatial extent of the quiet zone close to the head [31]. In addition, it has been found for the studied configuration that increasing the size of the diaphragm loudspeaker is beneficial to increase the size of the quiet zone, as already observed by Joseph et al in the case of a single secondary loudspeaker and a single point in its near field.…”
Section: Discussionmentioning
confidence: 70%
“…The presence of a rigid sphere affects the secondary sound field by imposing zero particle velocity, and thus zero pressure gradient. As has been shown by Garcia-Bonito and Elliott, this results in a beneficial flattening of the secondary field which tends to increase the spatial extent of the quiet zone close to the head [31]. In addition, it has been found for the studied configuration that increasing the size of the diaphragm loudspeaker is beneficial to increase the size of the quiet zone, as already observed by Joseph et al in the case of a single secondary loudspeaker and a single point in its near field.…”
Section: Discussionmentioning
confidence: 70%
“…25 This optimisation problem has been solved using sequential quadratic programming, which is possible since the cost function is convex and the constraints are affine, 26 although other programming methods may also be used. 22 To ensure that the solution to the discrete problem given by equation 7 approximates the desired solution to the continuous problem it is important that K is large enough, such that the discretised frequency responses are accurately represented.…”
Section: Controller Optimisationmentioning
confidence: 99%
“…12. Although the general formulation could include the effects of diffraction around finite-sized secondary sources, and the head, in the definition of the transfer responses, 20,21 these effects are not included in the simulations presented here, so as to more clearly illustrate the principles of the method. The optimum control problem is first formulated in the frequency domain, to explore the geometrical limitations of control for relatively narrowband disturbances, but a time-domain formulation is also included for the calculation of causal broadband controllers.…”
Section: Introductionmentioning
confidence: 99%