Modeling air gun signatures in marine seismic exploration considering multiple physical factors
Li Guo-Fa1,2, Cao Ming-Qiang1,2, Chen Hao-Lin3, and Ni Cheng-Zhou3
1. State Key Laboratory of Petroleum Resource and Prospecting (China University of Petroleum), Beijing 102249, China.
2. Key Laboratory of Geophysical Exploration of China National Petroleum Corporation, China University of Petroleum, Beijing 102249, China.
3. BGP Offshore, PetroChina, Tianjin 300280, China.
Abstract:
Based on analyzing the limit of Ziolkowski’s bubble oscillation formulation, a new model with various physical factors is established to simulate air gun signatures for marine seismic exploration. The practical effects of physical factors, such as heat transfer across the bubble wall, air gun port throttling, vertical rise of the bubble, fluid viscosity, and the existence of the air gun body were all taken into account in the new model. Compared with Ziolkowski’s model, the signatures simulated by the new model, with small peak amplitude and rapid decay of bubble oscillation, are more consistent with actual signatures. The experiment analysis indicates: (1) gun port throttling controls the peak amplitude of air gun pulse; (2) since the hydrostatic pressure decreases when the bubble rises, the bubble oscillation period changes; (3) heat transfer and fluid viscosity are the main factors that explain the bubble oscillation damping.
LI Guo-Fa,CAO Ming-Qiang,CHEN Hao-Lin et al. Modeling air gun signatures in marine seismic exploration considering multiple physical factors[J]. APPLIED GEOPHYSICS, 2010, 7(2): 158-165.
[1]
Chen, H. L., and Ni, C. Z., 2008, Simulation and application of far-field wavelet for air gun array: Oil Geophysical Prospecting (in Chinese), 43(6), 623 - 625.
[2]
Chen, H. L., Quan, H. Y., Chen,H.L., Quan,H.Y.,Yu,G.P., Li,W.D., and Liu,Y.Y., 2008, Summary of air gun source theory and technology: Equipment for Geophysical Prospecting (in Chinese), 18(4), 211 - 217.
[3]
Fricke, J. R., and Davis, J. M., 1985, A standard quantitative calibration procedure for marine seismic source: Geophysics, 50(1), 1525 - 1532.
[4]
Gilmore, F. R., 1952, Collapse of a spherical bubble: Hydrodynamics Laboratory, California Institute of Technology, Report No.26, 4.
Keller, J. B., and Kolodner, I. I., 1956, Damping of underwater explosion bubble oscillations: Jour. Applied Physics, 27(10), 1152 - 1161.
[7]
Landro, M., 1992, Modeling of GI gun signatures: Geophysics Prospecting, 40, 721 - 747.
[8]
Langhammer, M. L., 1993, Experimental study of viscosity effects on air gun signatures: Geophysics, 58(12), 1801 - 1808.
[9]
Laws, R. M., Hatton, L., and Haartsen, M., 1990, Computer modeling of clustered air guns: First Break, 18(9), 331 - 338.
[10]
Liu, B., 2005, Numerical simulation of air-gun array and its application: Ma. D. Thesis, Ocean University of China.
[11]
Prospereti, A., 1984, Bubble phenomena in sound fields: Ultrasonic, 22, 39 - 77.
[12]
Schulze-Gattermann, R., 1972, Physical aspects of the “airpulser” as a seismic energy source: Geophysical Prospecting, 20, 155 - 192.
[13]
Ziolkowski, A., 1970, A method for calculating the output pressure waveform from an air-gun: Geophys. J. R. Astr. Soc., 21, 137 - 161.
[14]
Ziolkowski, A., .Parks, G., Hatton L., and Haugland, T., 1982, The signature of an air-gun array: Computation from near-field measurements including interactions: Geophysics, 47(10), 1413 - 1421.
[15]
Ziolkowski, A., 1984, An air gun model which include heat transfer and bubble interaction: Geophysics, 59(11), 187 - 189.
[16]
Ziolkowski, A., 1998, Measurement of air-gun bubble oscillations: Geophysics, 63(6), 2009 - 2024.