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低频高压大容量气枪气泡压力子波特性研究

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随着海洋勘探逐渐向深海发展,大容量低频气枪的研究变得更加重要,降低探测波高频能量、提高低频能量成为气枪设计中亟待解决的核心问题。本文基于气泡动力学统一方程建立了大尺度低频气枪气泡动力学模型,该模型考虑了大尺度气枪气泡的迁移现象,通过模型对比证明了该模型的预测结果与真实大尺度低频气枪气泡的运动规律更加接近。本文基于该模型研究了气枪容积、工作压力、沉放深度及自由液面虚反射系数对气枪气泡迁移及压力子波等特性的影响。此外,深海勘探多使用气枪阵列增强探测压力波的能量,本文开展了不同间距和排列方式的双枪、三枪及四枪的压力子波特性研究。本文旨为新型大容量低频单枪枪体设计以及多枪组阵设计提供参考。
Study on the pressure wave characteristics of bubbles in low frequency,high pressure,and large capacity air guns
With the gradual development of deep-sea exploration,research on high-capacity air guns has become increasingly important.How to reduce high-frequency energy and enhance low-frequency energy is the core issue that urgently needs to be addressed in the design of air guns.In this study,we have established a large-scale low-frequency air gun bubble dynamics model based on the unified equation of bubble dynamics,considering the migration phenomenon of large-scale air gun bubbles.It has been proven that the model's predictions more closely match the motion patterns of real large-scale air gun bubbles through model comparison.Based on this model,the influence of air gun chamber volume,operating pressure,depth,and reflection coefficient on air gun bubble migration and pressure wave characteristics is investigated.In addition,air gun arrays are commonly used to enhance the energy of pressure waves in deep-sea exploration.In this study,the effects of the spacing between double,triple,and quadruple air guns in air gun arrays,as well as different arrangements on the characteristics of pressure waves of air guns,are studied.The findings of this study may contribute to the design of new high-capacity,low-frequency single air guns and the combined design of air gun arrays.

large-scale air gun bubblethe unified equation of bubble dynamicsbubble migrationair gun formationpressure wave

宁亦池、张帅、邱永成、刘毅、李帅、张阿漫

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哈尔滨工程大学南海研究院,三亚 572024

哈尔滨工程大学船舶工程学院,哈尔滨 150001

中海油田服务股份有限公司物探事业部,天津 300451

大尺度气枪气泡 气泡统一方程 气泡迁移 气枪阵列 压力子波

2024

中国科学(物理学 力学 天文学)
中国科学院

中国科学(物理学 力学 天文学)

CSTPCD北大核心
影响因子:0.644
ISSN:1674-7275
年,卷(期):2024.54(12)