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The radiating panel is backed by a larger acoustic enclosure (the back cavity).
It consists of a control force actuator and a sensor mounted at the actuator footprint on the radiating panel.
It is shown that convincing reductions of the TBL-induced vibrations of the radiating panel and the sound pressure inside the back cavity can be expected.
The structural-acoustic model encompasses a source panel (skin panel), coupled through an acoustic cavity to the radiating panel (trim panel).
Results verify earlier experimental investigations and indicate the application of control inputs to the radiating panel of the double panel system resulted in greater transmission loss (TL) due to its direct effect on the nature of the structural-acoustic (or radiation) coupling between the radiating panel and the receiving acoustic space.
Increased control performance was seen in a double panel system consisting of a stiffer radiating panel due to its lower modal density and also as a result of better impedance matching between the piezoelectric actuator and the radiating plate.
Similar(54)
Thus, the total sound radiated from the panel is reduced.
The transverse velocity is then calculated and utilized to obtain the sound radiated from the panel and subsequently the sound transmission loss.
The objective function of the optimisation is to reduce the sound radiating from the panels by selecting the optimal sizing and placement of the dome-shaped indentations.
The integral formulation of the Helmholtz equation allows the sound pressure level, radiated by a vibrating panel, to be determined.
The controller must reduce the noise radiated through the back panel when the front panel is excited by an external force that causes structural vibration.
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