Application of Pulse Gas-Discharge Electroacoustic Transducer for Non-Destructive Testing

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This paper presents the results of a gas-discharge electro acoustic transducer of two configurations, operating on the basis of a pulsed discharge in air at atmospheric pressure. The influence of the electrode configuration on the acoustic characteristics of the transducer is considered. It is shown that a change in the volume of the discharge chamber and the inter electrode gap have a significant effect on the radiation intensity of the transducer. The features that arise when using open and closed type electro acoustic transducers in flaw detection problems are revealed. It is shown that an open type gas-discharge electroacoustic transducer is a sufficiently powerful broadband source of the excitation signal and has prospects for use in non-destructive testing. A closed type gas-discharge electroacoustic transducer has advantages when testing materials with special requirements for surface cleanliness or the magnitude of the applied external electric field.

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作者简介

D. Derusova

Tomsk Polytechnic University

Email: red@tpu.ru
俄罗斯联邦, Tomsk

V. Nekhoroshev

Tomsk Polytechnic University; Institute of High Current Electronics of the Siberian Branch of the Russian Academy of Sciences

Email: nvo@lnp.hcei.tsc.ru
俄罗斯联邦, Tomsk; Tomsk

V. Shpilnoy

Tomsk Polytechnic University

Email: vshpilnoy@list.ru
俄罗斯联邦, Tomsk

A. Raut

Peoples’ Friendship University of Russia

编辑信件的主要联系方式.
Email: amolvr23@gmail.com
俄罗斯联邦, Moscow

参考

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2. Fig. 1. Simplified scheme of open-type (a) and closed-type (b) GEAPs, as well as photos of the corresponding return electrodes of open-type with a hole (c) and closed-type (d): 1 - point electrode; 2 - insulator; 3 - return current conductor; 4 - disc electrode (membrane); 5 - schematic position of the discharge channel

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3. Fig. 2. Functional scheme of the laboratory unit for the study of the GEAT

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4. Fig. 3. Detailed (a) and general (b) views of oscillograms of voltage on the gas-discharge gap

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5. Fig. 4. Voltage amplitude required for the development of breakdown on the dielectric surface at different values of the interelectrode gap

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6. Fig. 5. Vibration displacement signals on the membranes of the closed and open type GEAPs. During the experiment, the value of the interelectrode gap was 1 mm at the discharge channel volume of 80 mm3

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7. Fig. 6. Amplitude-frequency spectra of closed- and open-type HEAPs measured in the frequency range from 100 Hz to 100 kHz. The diameter of the hole in the membrane of the open-type HEAP is 3 mm

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8. Fig. 7. Vibration displacement amplitudes of the membrane surface at different volumes of the GEAT discharge chamber

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9. Fig. 8. Dependence of the vibration displacement amplitude in the centre of a duralumin membrane with a 3 mm hole on the interelectrode gap of the GEAT

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10. Fig. 9. Location of the GEAT and the investigated specimen with the model defect during the experiment

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11. Fig. 10. Amplitude-frequency spectra of sample vibrations in the defect region and defect-free zone recorded using closed-type (a) and open-type (b) GEATs

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12. Fig. 11. Vibrogram obtained during acoustic stimulation using a closed-type GEAT at a frequency of 9.8 kHz

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13. Fig. 12. Vibrograms of a PMMA plate during acoustic stimulation using open-type GEATs recorded at the natural frequencies of plate oscillations: 1681 Hz (a); 2356 Hz (b); 4094 Hz (c); 6656 Hz (d), as well as resonance frequencies of the defect 10062 Hz (e); 20519 Hz (f)

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