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CN105929456B - Transient electromagnetic and nmr integration detection method based on new transmitted waveform - Google Patents

Transient electromagnetic and nmr integration detection method based on new transmitted waveform Download PDF

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CN105929456B
CN105929456B CN201610250686.9A CN201610250686A CN105929456B CN 105929456 B CN105929456 B CN 105929456B CN 201610250686 A CN201610250686 A CN 201610250686A CN 105929456 B CN105929456 B CN 105929456B
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李貅
戚志鹏
刘文韬
刘金鹏
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Abstract

本发明公开了一种基于新发射波形的瞬变电磁与核磁共振一体化探测方法,按如下步骤:S1:发射一种同时满足瞬变电磁和核磁共振激发条件的新波形,然后同时进行瞬变电磁和核磁共振的观测;S2:用瞬变电磁探测技术获取地下电性分布,在此基础上进行核磁共振反演,获得地下水的含水率分布;S3:按照设定的研究尺度,将研究空间离散化为网格单元,各网格内部物性均匀分布,得核磁共振初始振幅的计算公式。该方法通过给出了一种同时满足瞬变电磁与核磁共振二者激发条件的波形,实现了瞬变电磁与核磁共振的一体化探测。可以极大的提高观测效率,且节约成本。

The invention discloses a transient electromagnetic and nuclear magnetic resonance integrated detection method based on a new emission waveform. The steps are as follows: S1: launch a new waveform that satisfies the excitation conditions of transient electromagnetic and nuclear magnetic resonance at the same time, and then simultaneously perform transient Observation of electromagnetic and nuclear magnetic resonance; S2: use transient electromagnetic detection technology to obtain underground electrical distribution, and then perform nuclear magnetic resonance inversion on this basis to obtain the water content distribution of groundwater; S3: according to the set research scale, the research space It is discretized into grid units, and the internal physical properties of each grid are uniformly distributed, and the calculation formula of the initial amplitude of nuclear magnetic resonance is obtained. The method realizes the integrated detection of transient electromagnetic and nuclear magnetic resonance by providing a waveform that satisfies the excitation conditions of both transient electromagnetic and nuclear magnetic resonance at the same time. It can greatly improve the observation efficiency and save the cost.

Description

基于新发射波形的瞬变电磁与核磁共振一体化探测方法Transient electromagnetic and nuclear magnetic resonance integrated detection method based on new emission waveform

技术领域technical field

本发明涉及瞬变电磁探测技术,特别是一种基于新发射波形的瞬变电磁与核磁共振一体化探测方法。The invention relates to transient electromagnetic detection technology, in particular to a transient electromagnetic and nuclear magnetic resonance integrated detection method based on a new emission waveform.

背景技术Background technique

近年来,瞬变电磁法发展十分迅猛,包括地面瞬变电磁法、航空瞬变电磁法、矿井瞬变电磁法等。瞬变电磁法观测纯二次场,可在近区测量;工作装置灵活多样,包括重叠回线、中心回线、分离回线、大回线源、井地等工作装置;其具有对低阻体反应灵敏、体积效应小、纵横向分辨率高、施工方便效率高等优点。因而,该方法被广泛应用于金属矿勘探、煤矿水文地质调查和工程勘查等领域。另外,瞬变电磁也可以应用于隧道掌子面的观测。隧道施工中将可能面临诸多地质灾害,如突水突泥、岩爆、塌方、瓦斯突出等。其中突(涌)水、突(涌)泥灾害是隧道施工中的主要地质灾害之一,在国内外隧道特大事故中,突(涌)水、突(涌)泥灾害在死亡人数和发生次数上均居于前列,成为制约隧道等地下工程建设的瓶颈问题,给隧道施工带来了严重的安全问题和经济损失,并极易诱发次生地质灾害和生态环境问题。因此,隧道掌子面前方含水地质构造的超前探测已经成为亟待研究和解决的重要工程科技难题。In recent years, the development of transient electromagnetic method is very rapid, including ground transient electromagnetic method, aviation transient electromagnetic method, mine transient electromagnetic method and so on. The pure secondary field can be observed by transient electromagnetic method, which can be measured in the near area; the working devices are flexible and diverse, including overlapping loops, center loops, separated loops, large loop sources, wells and other working devices; it has low resistance It has the advantages of sensitive volume response, small volume effect, high vertical and horizontal resolution, convenient construction and high efficiency. Therefore, this method is widely used in metal ore exploration, coal mine hydrogeological investigation and engineering exploration and other fields. In addition, TEM can also be applied to the observation of the tunnel face. Tunnel construction may face many geological disasters, such as water and mud inrush, rock burst, landslide, gas outburst, etc. Among them, sudden (surge) water and sudden (surge) mud disasters are one of the main geological disasters in tunnel construction. It has become a bottleneck problem restricting the construction of tunnels and other underground projects, which has brought serious safety problems and economic losses to tunnel construction, and is very easy to induce secondary geological disasters and ecological environment problems. Therefore, the advanced detection of water-bearing geological structures in front of the tunnel face has become an important engineering and technological problem that needs to be studied and solved urgently.

目前,核磁共振方法是一种可直接探测水体的地球物理方法,它利用人工激发的电磁场使地下氢原子的宏观磁矩产生扳倒角,在断开电流之后,宏观磁矩在地磁场的作用下产生旋进运动,其频率为氢核所特有。用铺设在地面的线圈接收宏观磁矩产生的进动信号,就可以探测水体的存在。但核磁共振只能给出含水率的空间变化,对于赋存介质的电阻率分布却很难有准确的描述,这是由于核磁共振发射的是单频电磁波,且接收的信号是水体中的氢原子旋进衰减过程中释放的电磁波,而非电磁感应衰减过程释放的电磁信号,而电性介质的分布情况会直接影响频率域电磁波的传播和分布。因而对电性介质分布的了解程度,直接影响着核磁共振探测的解释精度。At present, the nuclear magnetic resonance method is a geophysical method that can directly detect water bodies. It uses artificially excited electromagnetic fields to make the macroscopic magnetic moments of hydrogen atoms in the ground chamfer. Under the precession, the frequency is unique to the hydrogen nucleus. The presence of water can be detected by receiving the precession signal generated by the macroscopic magnetic moment with a coil laid on the ground. However, nuclear magnetic resonance can only give the spatial variation of water content, and it is difficult to accurately describe the resistivity distribution of the existing medium. This is because nuclear magnetic resonance emits single-frequency electromagnetic waves, and the received signal is hydrogen in water. The electromagnetic waves released during the atomic precession attenuation process are not the electromagnetic signals released during the electromagnetic induction attenuation process, and the distribution of the electrical medium will directly affect the propagation and distribution of electromagnetic waves in the frequency domain. Therefore, the degree of understanding of the distribution of the electrical medium directly affects the interpretation accuracy of NMR detection.

瞬变电磁和核磁共振探测有很多优点,并且应用于很多方面。但是如今瞬变电磁和核磁共振都是分别进行观测的,如果想同时应用瞬变电磁和核磁共振的资料数据进行综合解释,就要分别进行瞬变电磁和核磁共振的激发,然后分别采集瞬变电磁和核磁共振的数据。TEM and NMR detection have many advantages and are used in many ways. However, nowadays transient electromagnetic and nuclear magnetic resonance are observed separately. If you want to use the data of transient electromagnetic and nuclear magnetic resonance at the same time for comprehensive interpretation, you must separately excite transient electromagnetic and nuclear magnetic resonance, and then collect the transient data separately. EM and NMR data.

发明内容Contents of the invention

本发明的目的在于,提供一种基于新发射波形的瞬变电磁与核磁共振一体化探测方法,可以极大的提高观测效率,且节约成本。The purpose of the present invention is to provide a transient electromagnetic and nuclear magnetic resonance integrated detection method based on a new emission waveform, which can greatly improve observation efficiency and save costs.

为了实现上述任务,本发明通过以下技术方案得以实现:In order to achieve the above tasks, the present invention is achieved through the following technical solutions:

一种基于新发射波形的瞬变电磁与核磁共振一体化探测方法,其特征在于,包括如下步骤:A transient electromagnetic and nuclear magnetic resonance integrated detection method based on a new emission waveform is characterized in that it includes the following steps:

S1:发射一种同时满足瞬变电磁和核磁共振激发条件的新波形,然后同时进行瞬变电磁和核磁共振的观测;S1: launch a new waveform that satisfies both transient electromagnetic and nuclear magnetic resonance excitation conditions, and then simultaneously conduct transient electromagnetic and nuclear magnetic resonance observations;

S2:用瞬变电磁探测技术获取地下电性分布,在此基础上进行核磁共振反演,获得地下水的含水率分布;S2: Use transient electromagnetic detection technology to obtain underground electrical distribution, and then perform NMR inversion on this basis to obtain the water content distribution of groundwater;

S3:按照设定的研究尺度,将研究空间离散化为网格单元,各网格内部物性均匀分布,得核磁共振初始振幅的计算公式:S3: According to the set research scale, the research space is discretized into grid units, and the internal physical properties of each grid are uniformly distributed, and the calculation formula of the initial amplitude of NMR is obtained:

其中,N为剖分单元个数,Kj为第j个单元内所含水产生的初始振幅,nj为第j个单元的含水率;Among them, N is the number of subdivision units, K j is the initial amplitude generated by the water contained in the jth unit, and n j is the water content of the jth unit;

在多个脉冲距激发下,上式(1)可以矩阵形式表示:Under the excitation of multiple pulse distances, the above formula (1) can be expressed in matrix form:

Kn=E (2)Kn=E (2)

其中,Kij为第i个脉冲距激发下,第j个单元内水量产生的初始振幅;in, K ij is the initial amplitude generated by the water volume in the jth unit under the excitation of the ith pulse distance;

求解线性方程组(2)即可获得各单元含水率值。The moisture content of each unit can be obtained by solving the linear equation group (2).

所述S1步骤中:In the S1 step:

S11:所述的新波形为:梯形波上升沿(0~t1段)与拉莫尔频率的余弦波(t1~t2段)以及梯形波下降沿(t2~t3段)的组合;直流分量I0为5~50A,余弦波振幅I1为0.5~5A,持续时间Δt1(即t2-t1)为100~1000ms,关断时间Δt2(即t3-t2)为10~500us。S11: The new waveform described is: the rising edge of the trapezoidal wave (0-t 1 segment), the cosine wave of the Larmor frequency (t 1 -t 2 segment) and the trapezoidal wave falling edge (t 2 -t 3 segment) Combination; DC component I 0 is 5-50A, cosine wave amplitude I 1 is 0.5-5A, duration Δt 1 (ie t 2 -t 1 ) is 100-1000ms, off time Δt 2 (ie t 3 -t 2 ) is 10 ~ 500us.

S12、通过新波形,同此激发瞬变电磁和核磁共振响应,一次观测同时采集瞬变电磁与核磁共振的数据。S12. Simultaneously excite transient electromagnetic and nuclear magnetic resonance responses through the new waveform, and simultaneously collect transient electromagnetic and nuclear magnetic resonance data in one observation.

所述S2步骤中核磁共振反演的步骤为:The steps of NMR inversion in the S2 step are:

S21、在垂直于地磁场方向的外加磁场,使宏观磁矩和外加磁场的相互作用产生一力矩,使得宏观磁矩不再平行于地磁场,而是与地磁场产生一个扳倒角;S21. In an external magnetic field perpendicular to the direction of the earth's magnetic field, the interaction between the macroscopic magnetic moment and the applied magnetic field produces a torque, so that the macroscopic magnetic moment is no longer parallel to the earth's magnetic field, but produces a reversing angle with the earth's magnetic field;

S22、撤去外加磁场后,使宏观磁矩将与地磁场作用而使得宏观磁矩逐渐恢复到施加磁场之前的状态,过程中,释放出等于拉莫尔频率的自由衰减信号;S22. After the external magnetic field is removed, the macroscopic magnetic moment will interact with the earth's magnetic field so that the macroscopic magnetic moment gradually returns to the state before the magnetic field is applied. During the process, a free attenuation signal equal to the Larmor frequency is released;

S23、根据自由衰减信号的初始振幅推断地下含水体的分布和含水率。S23. Deduce the distribution and water content of the underground water-bearing body according to the initial amplitude of the free decay signal.

所述自由衰减信号的初始振幅公式为:The initial amplitude formula of the free decay signal is:

式中,E0为自由衰减信号的初始振幅,ω0为当地的拉莫尔频率,M0为质子磁矩,I为发射电流,γ为质子磁旋比,n为r点处的含水率,q为发射脉冲距,B为外加磁场垂直于地磁场的分量。where E 0 is the initial amplitude of the free decay signal, ω 0 is the local Larmor frequency, M 0 is the proton magnetic moment, I is the emission current, γ is the proton magnetic gyro ratio, and n is the water content at point r , q is the transmitted pulse distance, B is the component of the external magnetic field perpendicular to the geomagnetic field.

所述自由衰减信号的初始振幅的计算方法为:利用有限元法求取外加磁场的分布;采用直立六面体剖分、线性插值获得总体矩阵,然后求解左端包含电性分布信息、右端包含源项信息的方程组即可求得磁场值分布;通过半空间场值来反算源项的方法形成右端项,然后根据有限元法计算的磁场值即可获得模型的核磁共振响应。The calculation method of the initial amplitude of the free attenuation signal is: use the finite element method to obtain the distribution of the external magnetic field; use the upright hexahedron subdivision and linear interpolation to obtain the overall matrix, and then solve the left end containing electrical distribution information and the right end containing source item information The distribution of magnetic field values can be obtained by the equations; the right-hand term is formed by back-calculating the source term through the half-space field value, and then the NMR response of the model can be obtained according to the magnetic field value calculated by the finite element method.

所述S2步骤中,瞬变电磁方法中,信号接收装置是由多匝导线绕成的线圈或探头,接收到的是二次磁场随时间的变化率,依据等效导电平面理论有:In the S2 step, in the transient electromagnetic method, the signal receiving device is a coil or a probe wound by a multi-turn wire, and what is received is the rate of change of the secondary magnetic field with time, according to the equivalent conductive plane theory:

其中,S为纵向电导,K为与发射接收有关的常数,I为发射电流,a为发射回线半径,F为一个与时间和电导都有关的函数,F的表达式为:Among them, S is the longitudinal conductance, K is a constant related to transmission and reception, I is the transmission current, a is the radius of the transmission loop, F is a function related to both time and conductance, and the expression of F is:

其中,h为薄板深度,t为接收时刻;Among them, h is the depth of the thin plate, and t is the receiving time;

纵向电导S可依下式求取:The longitudinal conductance S can be calculated according to the following formula:

所述(6)式是关于纵向电导S的非线性方程,求解该方程即得纵向电导S。The formula (6) is a nonlinear equation about the longitudinal conductance S, and the longitudinal conductance S can be obtained by solving this equation.

根据纵向电导的定义,有电阻率值ρτ(h)=dh/dS,对应深度为:According to the definition of longitudinal conductance, there is a resistivity value ρ τ (h)=dh/dS, and the corresponding depth is:

本发明的基于新发射波形的瞬变电磁与核磁共振一体化探测方法,通过给出的新波形,实现瞬变电磁和核磁共振的一体化探测,提高了工作效率,节省了成本。The integrated detection method of transient electromagnetic and nuclear magnetic resonance based on the new emission waveform of the present invention realizes the integrated detection of transient electromagnetic and nuclear magnetic resonance through the given new waveform, improves work efficiency and saves costs.

附图说明Description of drawings

图1是发射的新波形示意图。Figure 1 is a schematic diagram of the new waveform transmitted.

具体实施方式Detailed ways

为了使本发明的目的及优点更加清楚明白,以下结合附图和实施例对本发明进行进一步详细说明。应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。In order to make the objects and advantages of the present invention clearer, the present invention will be further described in detail below in conjunction with the accompanying drawings and embodiments. It should be understood that the specific embodiments described here are only used to explain the present invention, not to limit the present invention.

本具体实施给出的一种基于新发射波形的瞬变电磁与核磁共振一体化探测方法,该方法首先给出一种新的能够同时满足瞬变电磁与核磁共振二者探测的激发条件的波形;在此基础上,通过一次观测同时采集瞬变电磁与核磁共振的数据;分别对瞬变电磁和核磁共振数据进行处理;最后根据瞬变电磁和核磁共振资料对探测结果综合分析进行综合解释。This specific implementation provides an integrated detection method of transient electromagnetic and nuclear magnetic resonance based on a new emission waveform. This method first provides a new waveform that can simultaneously satisfy the excitation conditions of both transient electromagnetic and nuclear magnetic resonance detection. On this basis, the data of transient electromagnetic and nuclear magnetic resonance are collected at the same time through one observation; the data of transient electromagnetic and nuclear magnetic resonance are processed separately; finally, the comprehensive analysis of the detection results is comprehensively interpreted according to the data of transient electromagnetic and nuclear magnetic resonance.

具体按如下步骤:Specifically follow the steps below:

S1、发射一种同时满足瞬变电磁和核磁共振激发条件的新的波形,然后同时进行瞬变电磁和核磁共振的观测.S1. Launch a new waveform that satisfies the excitation conditions of transient electromagnetic and nuclear magnetic resonance at the same time, and then observe transient electromagnetic and nuclear magnetic resonance at the same time.

S2、用瞬变电磁探测技术获取地下电性分布,在此基础上进行核磁共振反演;S2. Use transient electromagnetic detection technology to obtain underground electrical distribution, and perform nuclear magnetic resonance inversion on this basis;

S1步骤中的新波形如图1所示,新波形是梯形波的上升沿+拉莫尔频率的余弦波【I1COS(wot)+I0】+梯形波的下降沿组合形状。The new waveform in step S1 is shown in Figure 1. The new waveform is the combination shape of the rising edge of the trapezoidal wave + the cosine wave of the Larmor frequency [I 1 COS(wot)+I 0 ] + the falling edge of the trapezoidal wave.

其中0~t1段为梯形波的上升沿,t1~t2段为拉莫尔频率的余弦波,t2~t3段为梯形波的下降沿;直流分量I0为5~50A,余弦波振幅I1为0.5~5A,持续时间Δt1(即t2-t1)为100~1000ms,关断时间Δt2(即t3-t2)为10~500us。Among them, the 0~ t1 section is the rising edge of the trapezoidal wave, the t1 ~ t2 section is the cosine wave of Larmor frequency, the t2 ~ t3 section is the falling edge of the trapezoidal wave; the DC component I 0 is 5~50A, The amplitude I 1 of the cosine wave is 0.5-5A, the duration Δt 1 (ie t 2 -t 1 ) is 100-1000ms, and the turn-off time Δt 2 (ie t 3 -t 2 ) is 10-500us.

通过新波形,同此激发瞬变电磁和核磁共振响应,一次观测同时采集瞬变电磁与核磁共振的数据。Through the new waveform, the transient electromagnetic and nuclear magnetic resonance responses are excited at the same time, and the transient electromagnetic and nuclear magnetic resonance data are collected at the same time in one observation.

所述S2步骤中核磁共振反演的步骤为:The steps of NMR inversion in the S2 step are:

S21、在垂直于地磁场方向的外加磁场,使宏观磁矩和外加磁场的相互作用产生一力矩,使得宏观磁矩不再平行于地磁场,而是与地磁场产生一个扳倒角;S21. In an external magnetic field perpendicular to the direction of the earth's magnetic field, the interaction between the macroscopic magnetic moment and the applied magnetic field produces a torque, so that the macroscopic magnetic moment is no longer parallel to the earth's magnetic field, but produces a reversing angle with the earth's magnetic field;

S22、撤去外加磁场后,使宏观磁矩将与地磁场作用而使得宏观磁矩逐渐恢复到施加磁场之前的状态,过程中,释放出等于拉莫尔频率的自由衰减信号;S22. After the external magnetic field is removed, the macroscopic magnetic moment will interact with the earth's magnetic field so that the macroscopic magnetic moment gradually returns to the state before the magnetic field is applied. During the process, a free attenuation signal equal to the Larmor frequency is released;

S23、根据自由衰减信号的初始振幅进行核磁共振的反演。S23. Perform nuclear magnetic resonance inversion according to the initial amplitude of the free decay signal.

所述自由衰减信号的初始振幅公式为:The initial amplitude formula of the free decay signal is:

式中,E0为自由衰减信号的初始振幅,ω0为当地的拉莫尔频率,M0为质子磁矩,I为发射电流,γ为质子磁旋比,n为r点处的含水率,q为发射脉冲距,B为外加磁场垂直于地磁场的分量。where E 0 is the initial amplitude of the free decay signal, ω 0 is the local Larmor frequency, M 0 is the proton magnetic moment, I is the emission current, γ is the proton magnetic gyro ratio, and n is the water content at point r , q is the transmitted pulse distance, B is the component of the external magnetic field perpendicular to the geomagnetic field.

所述自由衰减信号的初始振幅的计算方法为:利用有限元法求取外加磁场的分布;采用直立六面体剖分、线性插值获得总体矩阵,然后求解左端包含电性分布信息、右端包含源项信息的方程组即可求得磁场值分布;通过半空间场值来反算源项的方法形成右端项,然后根据有限元法计算的磁场值即可获得模型的核磁共振响应。The calculation method of the initial amplitude of the free attenuation signal is: use the finite element method to obtain the distribution of the external magnetic field; use the upright hexahedron subdivision and linear interpolation to obtain the overall matrix, and then solve the left end containing electrical distribution information and the right end containing source item information The distribution of magnetic field values can be obtained by the equations; the right-hand term is formed by back-calculating the source term through the half-space field value, and then the NMR response of the model can be obtained according to the magnetic field value calculated by the finite element method.

所述S2步骤中,瞬变电磁方法中,信号接收装置是由多匝导线绕成的线圈或探头,接收到的是二次磁场随时间的变化率,依据等效导电平面理论有:In the S2 step, in the transient electromagnetic method, the signal receiving device is a coil or a probe wound by a multi-turn wire, and what is received is the rate of change of the secondary magnetic field with time, according to the equivalent conductive plane theory:

其中,S为纵向电导,K为与发射接收有关的常数,I为发射电流,a为发射回线半径,F为一个与时间和电导都有关的函数;Among them, S is the longitudinal conductance, K is a constant related to transmission and reception, I is the transmission current, a is the radius of the transmission loop, and F is a function related to both time and conductance;

F的表达式为:The expression of F is:

式中,h为薄板深度,t为接收时刻;In the formula, h is the depth of the thin plate, and t is the receiving time;

纵向电导S可依下式求取:The longitudinal conductance S can be calculated according to the following formula:

所述(6)式是关于纵向电导S的非线性方程,求解该方程即得纵向电导S;Described (6) formula is about the non-linear equation of longitudinal conductance S, solves this equation and obtains longitudinal conductance S;

以上所述仅是本发明的优选实施方式,应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以作出若干改进和润饰,这些改进和润饰也应视为本发明的保护范围。The above is only a preferred embodiment of the present invention, it should be pointed out that for those of ordinary skill in the art, without departing from the principle of the present invention, some improvements and modifications can also be made, and these improvements and modifications should also be It is regarded as the protection scope of the present invention.

Claims (5)

1. A transient electromagnetic and nuclear magnetic resonance integrated detection method based on a new emission waveform is characterized by comprising the following steps:
s1: emitting a new waveform which simultaneously meets the excitation conditions of transient electromagnetism and nuclear magnetic resonance, and then simultaneously observing the transient electromagnetism and the nuclear magnetic resonance;
s2: acquiring underground electrical distribution by using a transient electromagnetic detection technology, and performing nuclear magnetic resonance inversion on the basis to obtain the water content distribution of underground water;
s3: according to a set research scale, a research space is discretized into grid units, and physical properties in each grid are uniformly distributed to obtain a calculation formula of the nuclear magnetic resonance initial amplitude:
wherein N is the number of subdivision units, KjInitial amplitude, n, generated for water contained in the jth celljIs the water content of the jth cell;
under multiple pulse interval excitation, the above formula (1) can be expressed in a matrix form:
Kn=E (2)
wherein,Kijthe initial amplitude generated by the water quantity in the jth unit under the excitation of the ith pulse distance;
solving the linear equation set (2) to obtain the water content value of each unit;
in the step S1:
s11: the new waveform is as follows: rising edge of trapezoidal wave is 0-t1Cosine wave t of segment and Larmor frequency1~t2And falling edge t of trapezoidal wave2~t3A combination of segments; direct current component I05 to 50A, cosine wave amplitude I10.5-5A, duration delta t1I.e. t2-t1100-1000 ms, and a turn-off time Deltat2I.e. t3-t210-500 us;
s12: and simultaneously exciting transient electromagnetism and nuclear magnetic resonance response through the new waveform, and simultaneously acquiring data of the transient electromagnetism and the nuclear magnetic resonance through one-time observation.
2. The method of claim 1, wherein the step of inverting nuclear magnetic resonance in step S2 is:
s21, in the external magnetic field perpendicular to the direction of the geomagnetic field, the interaction between the macroscopic magnetic moment and the external magnetic field generates a moment, so that the macroscopic magnetic moment is not parallel to the geomagnetic field any more, but generates a pulling chamfer angle with the geomagnetic field;
s22, after the external magnetic field is removed, the macroscopic magnetic moment is enabled to act with the earth magnetic field so that the macroscopic magnetic moment is gradually restored to the state before the magnetic field is applied, and in the process, a free attenuation signal equal to Larmor frequency is released;
and S23, deducing the distribution and the water content of the underground water-containing body according to the initial amplitude of the free attenuation signal.
3. The method of claim 2, wherein the initial amplitude of the free fading signal is formulated as:
in the formula, E0For freely attenuating the initial amplitude, ω, of the signal0Is the local Larmor frequency, M0Is proton magnetic moment, I is emission current, gamma is proton magnetic rotation ratio, n is water content at r point, q is emission pulse distance, BIs the component of the applied magnetic field perpendicular to the geomagnetic field.
4. The method of claim 3, wherein the initial amplitude of the free fading signal is calculated by: the distribution of the external magnetic field is obtained by utilizing a finite element method; obtaining an overall matrix by adopting vertical hexahedron subdivision and linear interpolation, and then solving an equation set with the left end containing electrical distribution information and the right end containing source item information to obtain magnetic field value distribution; and forming a right-end term by a method of back-calculating a source term through a half-space field value, and then obtaining the nuclear magnetic resonance response of the model according to the magnetic field value calculated by a finite element method.
5. The method of claim 1, wherein in the step S2, in the transient electromagnetic method, the signal receiving device is a coil or a probe formed by winding a plurality of turns of wire, and the rate of change of the secondary magnetic field with time is received, and according to the equivalent conducting plane theory:
wherein S is the longitudinal conductance, K is a constant related to transmission and reception, I is the transmission current, a is the transmission loop radius, F is a function related to both time and conductance, and the expression of F is:
wherein h is the sheet depth, and t is the receiving time;
the longitudinal conductance S can be calculated as follows:
equation (6) is a nonlinear equation about the longitudinal conductance S, and solving the equation results in the longitudinal conductance S;
according to the definition of the longitudinal conductance, there is a resistivity value ρτ(h) dh/dS, corresponding to depths:
wherein, mu0=4π×10-7The magnetic permeability constant is vacuum;
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