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半航空频率域电磁测深2.5D正演模拟中几个关键问题

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基于伪随机发射的半航空频率域电磁测深方法具有信号强、采集速度快、成本低廉的勘探优势,近年来得到迅速发展,实际应用取得了较好的勘探效果.本文针对该领域在2.5D数值模拟中存在的一些核心问题.采用有限单元数值方法,分析讨论了电偶源加载方式、网格剖分、边界处理、观测区域、以及感应磁场随收发距和频率的分布特征.模型计算表明,采用均匀网格剖分、增加吸收边界条件能够提高有限单元法模拟精度.发现电偶极场源和长导线场源产生的感应磁场三分量Hx、Hy、Hz的场值在距离地面20 m的空气中具有如下特征:(1)当场源为电偶极源时,Hy 对异常不敏感,而Hx和Hz及其转换的视电阻率异常特征明显,Hx在低阻体上方表现为"高阻特征",且低频段特征比高频段特征明显;Hz的异常比较复杂,在AB偶极源中垂线两侧的异常会出现"对称特征":左侧的低阻体特征为"先低后高",右侧的低阻体为"先高后低",左侧的高阻体特征为"先低后高",右侧的高阻体为"先高后低".(2)当场源为供电长导线时,感应磁场三分量对异常体都有反映,Hx异常特征复杂,Hy 和Hz特征明显,低阻体上方表现为低场值特征,高阻体上方表现为高场值特征,Hz的异常特征强于Hy.接地电磁场源的偶极长度影响电磁场特征,特别是感应磁场三分量影响较大,且有限单元法的网格、边界也会影响电磁场特征.当场源为偶极电源时,感应磁场Hx特征明显,而Hy特征不敏感,Hz异常明显但特征比较复杂.本次研究丰富了非理想电偶极源(近似点源)时一些电磁场特征,为半航空电磁法的发展提供科学依据.
Several key issues in 2.5D forward modeling of semi-airborne electromagnetic sounding in the frequency domain
The semi-aerial frequency domain electromagnetic sounding method based on pseudo-random transmission has the advantages of strong signal,fast acquisition speed and low cost.It has been developed rapidly in recent years,and its practical application has achieved good exploration results.This paper addresses some core issues in 2.5D numerical simulation in this field.Using the finite element numerical method,the loading mode of the galvanic couple source,grid division,boundary treatment,observation area,and distribution characteristics of the induced magnetic field with the transmitting and receiving distance and frequency are analyzed and discussed.Model calculations show that the simulation accuracy of finite element method can be improved by adopting uniform mesh division and adding absorbing boundary conditions.It is found that the field values of the three components Hx,Hy,and Hz of the induced magnetic field generated by the electric dipole field source and the long wire field source have the following characteristics in the air at a distance of 20 m from the ground:(1)When the field source is an electric dipole source,Hy has the following characteristics:The abnormality is not sensitive,but Hx and Hz and their converted apparent resistivity have obvious anomalous characteristics.The abnormality on both sides of the vertical line in the AB dipole source will appear"symmetrical characteristics":the low-resistance body on the left is characterized by"lower first and then higher",the lower resistance body on the right is"higher and then lower",and the left The high-resistance body is characterized as"low first,then high",and the high-resistance body on the right is"high first,then low".(2)When the field source is a long power supply wire,the three components of the induced magnetic field all reflect the abnormal body,the Hx abnormal feature is complex,the Hy and Hz features are obvious,the low-resistance body is characterized by low field value,and the high-resistance body is characterized by High field value features,the abnormal features of Hz are stronger than those of H.The dipole length of the grounded electromagnetic field source affects the characteristics of the electromagnetic field,especially the three components of the induced magnetic field,and the grid and boundary of the finite element method also affect the characteristics of the electromagnetic field.When the field source is a dipole power supply,the Hx characteristic of the induced magnetic field is obvious,but the Hy characteristic is insensitive,and the Hz anomaly is obvious but the characteristic is more complicated.This study enriches some electromagnetic field characteristics of non-ideal electric dipole sources(approximate point sources),and provides a scientific basis for the development of semi-airborne electromagnetic methods.

Electric dipole sourceGround long lead sourceSemi-airborne frequency domain soundingMulti-component induced magnetic fieldFinite element method

徐晶、强建科、张钱江、肖晓

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中南大学有色金属成矿预测与地质环境监测教育部重点实验室,长沙 410083

中南大学地球科学与信息物理学院,长沙 410083

桂林理工大学地球科学学院,桂林 541004

香港中文大学(深圳)城市地下空间及能源研究院,深圳 518172

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电偶极源 接地长导线源 半航空频率域测深 感应磁场多分量 有限单元法

国家自然科学基金&&

42074087GDNRC[2021]57

2024

地球物理学进展
中国科学院地质与地球物理研究所 中国地球物理学会

地球物理学进展

CSTPCD北大核心
影响因子:1.761
ISSN:1004-2903
年,卷(期):2024.39(1)
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