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069-1.gif

a) 30 km range

 

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b) 60 km rangea

Fig. 5. Azimuthal distributions of the sound pressure level for different frequencies received at the center of the circles.

 

4. CONCLUSIONS

 

To develop the real-time ocean acoustic survey technology by using OAT system in deep water, explosive source has been deployed from the aircraft to survey a medium scale basin. The SUS, which may be not repeatable source in terms of explosion and subsequent bubble pulse, produced a peak signal that was easily detected by the VLA. Furthermore, the exact explosion time and depth of the charges could be determined by the empirical formula and the sonobuoy receiver which was placed within the direct-path zone. In conclusion, present experiments have been successful to locate the position of warm eddy and its temperature field in the East Sea of Korea.

 

REFERENCES

 

Arons, A. B., 1954, Underwater explosion shock wave parameters at large distance from the charges, J. Acoust. Soc. Am., 26: 343-346.

Blaik, M. and E.A. Christian, 1965, Near-surface measurement of deep explosions. I. Pressure pulses from small charges, J Acoust. Soc. Am., 38: 50-56.

Chapman, N. R., 1985, Measurement of the waveform parameters of shallow explosive charges, J. Acoust. Soc. Am., 78: 672-681.

Cole. R. H., 1948, Underwater Explosions, Dover Pub., Inc., New York. 437pp.

Lee, J.H., 1993, A review of tracer inverse problems in oceanography, Ocean Research,15: 53-69.

Lynch, J., D. Frye, K. Peal, S. Liberatore, S. Kery E. Hobart, A. Newhall and S. Smith, 1992, Real-Time Tomography Mooring, WHOI Tech. Report, WHOI-92-29, 146 pp.

Munk, W. and C. Wunsch, 1979, Ocean acoustic tomography: A scheme for large scale monitoring, Deep-Sea Res., 26: 123-161.

 

 

 

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