A remote optical technique is proposed as a valid alternative to conventional electroacoustic excitation of sound inside an acoustic resonator. Efficient photoacoustic conversion of an amplitude-modulated light beam, impinging on the interior solid surface of the resonator wall, into a stationary acoustic field is achieved. The reported results were obtained in a cylindrical stainless steel resonator with a volume of about 572 cm3 ; the radiation source is the 514 nm line of an Ar+ laser. The laser beam can be focused on different points of the resonator internal surface. The signal frequency dependence is well interpreted in terms of gas-microphone detection theory. The precision obtained in the measurement of resonance frequency fN and halfwidth gN of the cavity modes is on the order of 10-6 of fN and is likely to be further improved by minor refinements of the experimental apparatus.
Photoacoustic Excitation of the Interior Surface of an Acoustic Resonator for Speed of Sound Measurement / Benedetto, G; Gavioso, Roberto; Spagnolo, R.. - (1997). (Intervento presentato al convegno 13th Symposium on Thermophysical Properties tenutosi a Boulder nel 22-27 June 1997).
Photoacoustic Excitation of the Interior Surface of an Acoustic Resonator for Speed of Sound Measurement
GAVIOSO, ROBERTO;
1997
Abstract
A remote optical technique is proposed as a valid alternative to conventional electroacoustic excitation of sound inside an acoustic resonator. Efficient photoacoustic conversion of an amplitude-modulated light beam, impinging on the interior solid surface of the resonator wall, into a stationary acoustic field is achieved. The reported results were obtained in a cylindrical stainless steel resonator with a volume of about 572 cm3 ; the radiation source is the 514 nm line of an Ar+ laser. The laser beam can be focused on different points of the resonator internal surface. The signal frequency dependence is well interpreted in terms of gas-microphone detection theory. The precision obtained in the measurement of resonance frequency fN and halfwidth gN of the cavity modes is on the order of 10-6 of fN and is likely to be further improved by minor refinements of the experimental apparatus.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.