CN103576205B - Air-ground transient electromagnetic exploration method based on composite magnetic source technology - Google Patents
Air-ground transient electromagnetic exploration method based on composite magnetic source technology Download PDFInfo
- Publication number
- CN103576205B CN103576205B CN201310574207.5A CN201310574207A CN103576205B CN 103576205 B CN103576205 B CN 103576205B CN 201310574207 A CN201310574207 A CN 201310574207A CN 103576205 B CN103576205 B CN 103576205B
- Authority
- CN
- China
- Prior art keywords
- source
- combination
- ground
- forcing
- sources
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
- 230000001052 transient effect Effects 0.000 title claims abstract description 31
- 238000000034 method Methods 0.000 title claims abstract description 24
- 239000002131 composite material Substances 0.000 title claims abstract 6
- 238000005259 measurement Methods 0.000 claims description 38
- 230000000737 periodic effect Effects 0.000 claims description 2
- 238000002372 labelling Methods 0.000 claims 3
- 230000000638 stimulation Effects 0.000 claims 1
- 230000007704 transition Effects 0.000 claims 1
- 230000005284 excitation Effects 0.000 description 35
- 238000009826 distribution Methods 0.000 description 18
- 238000010586 diagram Methods 0.000 description 9
- 238000013480 data collection Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 238000001514 detection method Methods 0.000 description 2
- 238000004088 simulation Methods 0.000 description 2
- 230000002411 adverse Effects 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Geophysics And Detection Of Objects (AREA)
Abstract
Description
技术领域technical field
本发明涉及一种基于组合源发射-无人机接收的地空瞬变电磁勘查方法,属于地球物理电磁勘探方法范畴。The invention relates to a ground-air transient electromagnetic prospecting method based on combined source emission and UAV reception, belonging to the category of geophysical electromagnetic prospecting methods.
背景技术:Background technique:
瞬变电磁法是一种传统的找矿找水电磁勘探方法,采用在地面上布置发射回线,供以电流脉冲信号,接收线圈也布置在地面上,接收垂直感生电动势瞬变信号。然后根据观测数据反演解释地下电性构造以达到地质勘探的目的。该方法在地形复杂、地面物探难以施工区域,工作效率较低,甚至无法进行工作。于是,人们想到应用航空瞬变电磁勘查技术来实现大面积、长距离地物探工作。航空瞬变电磁方法有以固定翼为平台的和以直升机为平台的两种方法,前者作业速度快,发射磁矩大、勘探深度相对较大,后者空间分辨率高,勘探深度相对较小。该种方法由于需机载发射机、接收机、主机和供电电源等设备,因此航空瞬变电磁勘探深度很有限,固定翼航空瞬变电磁的勘探深度一般在400~800米,直升机航空瞬变电磁的勘探深度一般在300米左右。从上可以看出,现有瞬变电磁勘查法均无法实现复杂区域的高效、高分辨率、大面积和大深度勘探。The transient electromagnetic method is a traditional electromagnetic prospecting method for ore and water exploration. The transmitting loop is arranged on the ground to supply the current pulse signal, and the receiving coil is also arranged on the ground to receive the vertically induced electromotive force transient signal. Then, according to the observation data, the underground electrical structure is inverted and interpreted to achieve the purpose of geological exploration. This method has low work efficiency and even cannot work in areas with complex terrain and difficult ground geophysical prospecting. Therefore, people thought of applying airborne transient electromagnetic survey technology to realize large-area and long-distance geophysical prospecting work. There are two methods of aviation transient electromagnetic methods, which use fixed-wing as the platform and helicopter as the platform. The former has fast operation speed, large emission magnetic moment, and relatively large exploration depth. The latter has high spatial resolution and relatively small exploration depth. . Since this method requires airborne transmitters, receivers, hosts, power supplies and other equipment, the exploration depth of aviation transient electromagnetics is very limited. The exploration depth of fixed-wing aviation transient electromagnetics is generally 400-800 meters. Electromagnetic exploration depth is generally about 300 meters. It can be seen from the above that none of the existing transient electromagnetic survey methods can achieve high-efficiency, high-resolution, large-area and deep-depth exploration in complex areas.
发明内容Contents of the invention
本发明的目的在于提供一种基于组合磁性源技术的地空瞬变电磁勘查方法,该方法能实现在地表环境复杂区域进行高效、高分辨率、大面积和大深度的勘探。The object of the present invention is to provide a ground-space transient electromagnetic prospecting method based on combined magnetic source technology, which can realize high-efficiency, high-resolution, large-area and deep-depth prospecting in areas with complex surface environments.
本发明提供的基于组合磁性源技术的地空瞬变电磁勘查方法,包括在地面上布置发射周期性双极性电流脉冲信号的磁性源,用线圈接收感生电动势瞬变信号,所述磁性源为4、6或8个,间隔均匀的分布在以勘探目标区域为中心的地面上的一个圆周上,各磁性源可视为垂直磁偶极子源;接收线圈载于无人机上,无人机在勘查目标区域上方飞行,采集各种组合源激励下的感生电动势瞬变响应数据,所述组合源是指由对称分布的几个或全部磁性源构成的激励源。The ground-space transient electromagnetic survey method based on the combined magnetic source technology provided by the present invention includes arranging a magnetic source on the ground that emits a periodic bipolar current pulse signal, and using a coil to receive an induced electromotive force transient signal. The magnetic source There are 4, 6 or 8, and they are evenly spaced on a circle on the ground centered on the exploration target area, and each magnetic source can be regarded as a vertical magnetic dipole source; the receiving coil is carried on the UAV, and no one The aircraft flies above the survey target area to collect the induced electromotive force transient response data under the excitation of various combined sources. The combined source refers to the excitation source composed of several or all magnetic sources symmetrically distributed.
上述无人机在勘查区域上方沿相互平行的路线按首尾相连的往返方式飞行,一种组合源测量完毕后,换另一种组合源激励信号,重新往返飞行进行新的组合激励源信号下的飞行测量,直至各种组合源全部测量为止。The above-mentioned unmanned aerial vehicle flies along the parallel route above the survey area in an end-to-end round-trip manner. After the measurement of one combined source is completed, the excitation signal of another combined source is changed, and the round-trip flight is carried out under the new combined excitation source signal. Measure on the fly until all combined sources are measured.
上述磁性源为4个,设各个源的标记依次为A、B、C、D,第一次进行标记为A、C的组合源激励下的飞行测量;第二次进行标记为B、D的组合源激励下的飞行测量;第三次进行标记为A、B、C、D的组合源激励下的飞行测量,最终得到三种组合源的测量数据。The above-mentioned magnetic sources are 4, assuming that the labels of each source are A, B, C, D in turn, the first flight measurement under the excitation of the combined source labeled A and C is carried out; The flight measurement under the excitation of the combined source; the third flight measurement under the excitation of the combined source marked as A, B, C, and D is carried out, and finally the measurement data of the three combined sources are obtained.
上述磁性源为6个,设各个源的标记依次为A、B、C、D、E、F,第一次进行标记为A、C、E的组合源激励下的飞行测量;第二次进行标记为B、D、F的组合源激励下的飞行测量;第三次进行标记为A、B、C、D、E、F的组合源激励下的飞行测量,最终得到三种组合源的测量数据。The above-mentioned magnetic sources are 6, and the labels of each source are set as A, B, C, D, E, F in turn, and the flight measurement under the excitation of the combined source marked as A, C, E is carried out for the first time; The flight measurement under the excitation of the combined source marked as B, D, F; the third flight measurement under the excitation of the combined source marked as A, B, C, D, E, F, and finally the measurement of the three combined sources data.
上述磁性源为8个,设各个源的标记依次为A、B、C、D、E、F、G、H,第一次进行标记为A、C、E、G的组合源激励下的飞行测量;第二次进行标记为B、D、F、H的组合源激励下的飞行测量;第三次进行标记为A、B、C、D、E、F、G、H的组合源激励下的飞行测量,最终得到三种组合源的测量数据。The above-mentioned magnetic sources are 8, assuming that the labels of each source are A, B, C, D, E, F, G, and H in turn, and the first flight under the excitation of the combined sources labeled A, C, E, and G is carried out. Measurements; second in-flight measurement under combined source excitation marked B, D, F, H; third time under combined source excitation marked A, B, C, D, E, F, G, H Finally, the measurement data of the three combined sources are obtained.
本发明采用在地面上布置多个磁性源,发射脉冲电流信号,在空中用无人机携带接收线圈测量三分量感生电动势响应信号,无人机在空中可以高效地飞行测量。由于勘探区域在多个磁性源的中心区域,因此各个磁性源可视为垂直磁偶极子,同时由于多个磁性源布置在地面上,因此观测数据的强度相对较大、信噪比也相对较高。传统的地面瞬变电磁方法中,要做面积性勘探的话,如果采用移动源的方法,如中心回线或重叠回线法,需要在地面网状测点上逐点采集,地形起伏或地表环境恶劣的话,不但工作量大,而且工作效率低甚至无法开展工作;如果采用定回线装置的话,测点的偏移距较大时,用一个激励源的定回线源瞬变电磁响应幅度较小。另外,如果有局部不均匀体位于发射源附近或其下方,如同地面CSAMT方法的场源复印效应等类似,外侧观测区域的响应数据会受到局部不均匀体的影响。用传统的一个激励源进行勘探时,近源的不均匀体会影响很大的一片区域,对地下异常的圈定造成非常不利的影响。采用组合源激励技术,在勘探目标区域周围的一个大的近似圆周上布置激励源,不但会增加勘探区域的响应信号强度,增加勘探深度,同时减弱局部不均匀体对整个区域的响应数据造成的影响。组合源激励技术还有一个优势是,可以获得不同组合源的多次采集数据,从而获得关于地下异常体的多角度观测信息,降低反演多解性的影响。因此本发明方法可以克服大面积区域勘探所面临的诸多困难,实现复杂区域的高效、高分辨率、大面积和大深度的勘探。In the present invention, a plurality of magnetic sources are arranged on the ground to emit pulsed current signals, and a receiving coil is used to measure the three-component induced electromotive force response signal in the air, and the drone can fly and measure efficiently in the air. Since the exploration area is in the central area of multiple magnetic sources, each magnetic source can be regarded as a vertical magnetic dipole. At the same time, since multiple magnetic sources are arranged on the ground, the intensity of the observation data is relatively large, and the signal-to-noise ratio is also relatively high. higher. In the traditional ground transient electromagnetic method, if you want to do area exploration, if you use the method of moving source, such as the center loop or overlapping loop method, you need to collect point by point on the ground network measuring points, terrain fluctuations or surface environment If it is bad, not only the workload is heavy, but also the work efficiency is low and even the work cannot be carried out; if the fixed loop device is used, when the offset distance of the measuring point is large, the transient electromagnetic response amplitude of the fixed loop source with an excitation source is relatively small. Small. In addition, if there is a local inhomogeneity located near or below the emission source, similar to the field source copying effect of the ground CSAMT method, the response data in the outer observation area will be affected by the local inhomogeneity. When a traditional excitation source is used for exploration, the inhomogeneity near the source will affect a large area, which will have a very adverse effect on the delineation of underground anomalies. Using combined source excitation technology, the excitation source is arranged on a large approximate circle around the exploration target area, which will not only increase the response signal strength of the exploration area, increase the exploration depth, but also weaken the influence of local inhomogeneous bodies on the response data of the entire area. influences. Another advantage of the combined source excitation technology is that multiple acquisition data of different combined sources can be obtained, so as to obtain multi-angle observation information about underground anomalies and reduce the influence of inversion multi-solution. Therefore, the method of the present invention can overcome many difficulties faced in the exploration of large areas, and realize the exploration of complex areas with high efficiency, high resolution, large area and large depth.
下面以一个简单的三层介质模型的组合源-无人机地空瞬变电磁响应为例进行仿真计算,来进一步解释本发明的具体效果。The following uses a simple three-layer medium model combined source-UAV ground-air transient electromagnetic response as an example to perform simulation calculations to further explain the specific effects of the present invention.
设三层模型的层电阻率为100、20和100欧姆米,层厚度均为300米。地面上铺设的各个磁性源均为参数相同的垂直磁偶极子(Vertical MagneticDipole,VMD)源,磁矩为1Am2,置于地面一个圆周上的不同的点上。接收线圈为1m2,其高度为100米。设发射信号为阶跃脉冲,测量断电后32个时刻点的感生电动势瞬变响应。Assume that the layer resistivity of the three-layer model is 100, 20 and 100 ohm-meters, and the layer thickness is 300 meters. Each magnetic source laid on the ground is a vertical magnetic dipole (Vertical Magnetic Dipole, VMD) source with the same parameters, the magnetic moment is 1Am 2 , and they are placed at different points on a circle on the ground. The receiving coil is 1 m 2 and its height is 100 m. Assuming that the transmitting signal is a step pulse, the transient response of the induced electromotive force at 32 time points after power-off is measured.
比较五种组合发射源分布时的响应结果,第一种是1个垂直磁偶极子发射源位于(-2000,0,0)m处,第二种也是1个VMD发射源,位于(2000,0,0)m处,第三种是2个VMD发射源分别位于(-2000,0,0)m和(2000,0,0)m处,第四种是4个VMD发射源分别位于(-2000,0,0)m、(2000,0,0)m、(0,-2000,0)m、(0,2000,0)m处,第五种是8个VMD发射源,它们的位置分别在以地面坐标原点为中心、半径为2000m的圆周上八个点,其中第一源位于(2000,0,0)m处,其它源的位置与原点的连线同x正方向夹角分别为45度、90度、135度、180度、225度、270度和315度。Comparing the response results of the distribution of five combined emitters, the first one is a vertical magnetic dipole emitter located at (-2000,0,0)m, the second is also a VMD emitter located at (2000 ,0,0)m, the third type is that 2 VMD emission sources are located at (-2000,0,0)m and (2000,0,0)m respectively, the fourth type is that 4 VMD emission sources are located at (-2000,0,0)m, (2000,0,0)m, (0,-2000,0)m, (0,2000,0)m, the fifth type is 8 VMD emission sources, they The positions of the eight points on the circle with the origin of the ground coordinates as the center and a radius of 2000m, among which the first source is located at (2000,0,0)m, and the positions of the other sources and the origin are in the same positive x direction The angles are 45 degrees, 90 degrees, 135 degrees, 180 degrees, 225 degrees, 270 degrees and 315 degrees.
图1~图5是断电后4.32ms时五种组合源激励下飞行面(z=-100m)上三个分量响应的分布图。观察各图可知,只用一个激励源时,响应的分布具有方向性,距离激励源越远,响应的幅度也越小。当运用组合源激励时,勘探目标区域逐渐变得均匀,组合源中对称分布的激励源个数越多,中央区域响应分布也越均匀,响应幅度也越大,对勘探地下构造也越有利。图6是五种组合源下勘探区域中心的飞行面上空对应点(0,0,-100)m的z分量瞬变曲线对比图。从图中可以看出,一个源时,无论布置在勘探区域左或右的位置,响应是一致的,多个组合源时,瞬变响应形态一致,源的个数越多,响应的幅值越大。Figures 1 to 5 are the distribution diagrams of the three component responses on the flight surface (z=-100m) under the excitation of five combined sources at 4.32ms after power failure. Observing each figure, it can be known that when only one excitation source is used, the distribution of the response has directionality, and the farther away from the excitation source, the smaller the response amplitude. When combined source excitation is used, the exploration target area gradually becomes uniform. The more symmetrically distributed excitation sources in the combined source, the more uniform the response distribution in the central area and the larger the response range, which is more beneficial to the exploration of underground structures. Fig. 6 is a comparative diagram of the z-component transient curves of corresponding points (0, 0, -100) m above the flight surface at the center of the exploration area under five combined sources. It can be seen from the figure that when there is one source, the response is consistent regardless of whether it is arranged on the left or right of the exploration area; when multiple sources are combined, the transient response form is consistent. bigger.
图7是三个时刻点y=0m飞行测线上的z分量响应剖面曲线,可以看出,传统的地面单个源激励时,各个瞬时的剖面响应曲线是向远源方向单调衰减的。而采用本发明的对称组合源激励时,各个瞬时剖面曲线中央部分变得相对平缓,利于探测。Figure 7 shows the z-component response profile curves on the flight survey line at three time points y=0m. It can be seen that when the traditional ground single source is excited, the profile response curves at each instant decay monotonously toward the far source. However, when the symmetrical combination source of the present invention is used for excitation, the central part of each instantaneous profile curve becomes relatively smooth, which is convenient for detection.
从上述的模拟结果可知,对称分布的组合源可以克服单源的远源衰减问题,增强数据的信噪比,降低反演的多解性影响,提高解释结果的可靠性。另外,采用多源组合的多次测量技术,可以获得多角度的探测信息,对局部目标体的分辨能力也更强。From the above simulation results, it can be seen that the combined source with symmetrical distribution can overcome the problem of far-source attenuation of single source, enhance the signal-to-noise ratio of data, reduce the influence of multiple solutions in inversion, and improve the reliability of interpretation results. In addition, the multi-measurement technology of multi-source combination can obtain multi-angle detection information, and the ability to distinguish local targets is also stronger.
下面结合附图和实施例对本发明作进一步说明。The present invention will be further described below in conjunction with drawings and embodiments.
附图说明Description of drawings
图1是第一种激励源(一个左源)接收高度面上4.32ms时的三分量响应分布,其中图a~c分别是x,y,z分量感生电动势响应的分布图。Figure 1 is the three-component response distribution of the first excitation source (a left source) at 4.32ms on the receiving height plane, where Figures a~c are the distribution diagrams of the induced electromotive force responses of the x, y, and z components respectively.
图2是第二种激励源(一个右源)接收高度面上4.32ms时的三分量响应分布,其中图a~c分别是x,y,z分量感生电动势响应的分布图。Figure 2 is the three-component response distribution of the second excitation source (a right source) at 4.32ms on the receiving height plane, where Figures a~c are the distribution diagrams of the induced electromotive force responses of the x, y, and z components respectively.
图3是第三种激励源(左右两个源)接收高度面上4.32ms时的三分量响应分布,其中图a~c分别是x,y,z分量感生电动势响应的分布图。Figure 3 is the three-component response distribution of the third excitation source (left and right sources) at 4.32ms on the receiving height plane, where Figures a~c are the distribution diagrams of the induced electromotive force responses of the x, y, and z components respectively.
图4是第四种激励源(上下左右四个源)接收高度面上4.32ms时的三分量响应分布,其中图a~c分别是x,y,z分量感生电动势响应的分布图。Figure 4 is the three-component response distribution of the fourth excitation source (up, down, left, and right) at 4.32 ms on the receiving height plane, where Figures a to c are the distributions of the x, y, and z component induced electromotive force responses.
图5是第五种激励源(圆周上等间隔分布8个源)接收高度面上4.32ms时的三分量响应分布,其中图a~c分别是x,y,z分量感生电动势响应的分布图。Figure 5 is the distribution of the three-component response at 4.32 ms on the receiving height plane of the fifth excitation source (8 sources equally spaced on the circumference), where Figures a to c are the distributions of the induced electromotive force responses of the x, y, and z components respectively picture.
图6是五种发射源下,(0,0,-100)m处的Vz分量瞬变响应曲线对比图。Figure 6 is a comparison chart of Vz component transient response curves at (0, 0, -100) m under five emission sources.
图7是三个时刻点y=0m飞行测线上的z分量响应剖面曲线。Figure 7 is the z-component response profile curves on the flight survey line at three time points y=0m.
图8是4个磁性源在地面的分布图。Figure 8 is a distribution diagram of four magnetic sources on the ground.
图9是无人机飞行路线示意图。Figure 9 is a schematic diagram of the flight path of the drone.
图10是6个磁性源在地面的分布图。Figure 10 is a distribution diagram of six magnetic sources on the ground.
图11是8个磁性源在地面的分布图。Figure 11 is a distribution diagram of 8 magnetic sources on the ground.
具体实施方式detailed description
本发明实施时,首先需确定磁性源所在圆周的半径大小、磁性源采用的个数、发射脉冲波形、采样时间序列、飞行高度、航线等,然后再进行数据采集,下面分别以4个源、6个源和8个源进行说明。During the implementation of the present invention, at first it is necessary to determine the radius of the circle where the magnetic source is located, the number that the magnetic source adopts, the emission pulse waveform, the sampling time sequence, the flight height, the flight route, etc., and then carry out data collection. Below, respectively use 4 sources, 6 sources and 8 sources for illustration.
实施例1Example 1
磁性源为4个,均为参数相同的垂直磁偶极子源,设各个源的标记依次为A、B、C、D,如图8所示,第一次进行标记为A、C的组合源激励下的飞行测量;第二次进行标记为B、D的组合源激励下的飞行测量;第三次进行标记为A、B、C、D的组合源激励下的飞行测量,最终得到三种组合源的测量数据。There are 4 magnetic sources, all of which are vertical magnetic dipole sources with the same parameters. Let the labels of each source be A, B, C, and D in turn, as shown in Figure 8. The combination of labels A and C is performed for the first time The flight measurement under the source excitation; the second flight measurement under the combined source excitation marked as B and D; the third time the flight measurement under the combined source excitation marked as A, B, C, D, and finally three Measurement data from a combination of sources.
无人机携带三分量接收线圈,在勘探目标区域上空沿图9所示的路线飞行,为便于说明,将路线以1、2、3、4标明,测量时无人机先飞行路线1,然后反方向飞行路线2,再沿路线3返回,如此类推,将全部路线飞行完毕,即完成一种组合源的测量。然后,沿原路线返回进行下一种组合源的飞行测量,直至全部组合源全部测量为止。The UAV carries a three-component receiving coil and flies along the route shown in Figure 9 over the survey target area. Fly route 2 in the opposite direction, and then return along route 3, and so on, after flying all the routes, the measurement of a combined source is completed. Then, go back along the original route to carry out the flight measurement of the next combination source until all the combination sources are measured.
数据采集完毕后,按地空瞬变电磁的工作流程进行资料处理、反演解释等工作。After the data collection is completed, data processing, inversion interpretation and other work are carried out according to the workflow of ground-space transient electromagnetic.
实施例2Example 2
磁性源为6个,均为参数相同的垂直磁偶极子源,设各个源的标记依次为A、B、C、D、E、F,如图10所示,第一次进行标记为A、C、E的组合源激励下的飞行测量;第二次进行标记为B、D、F的组合源激励下的飞行测量;第三次进行标记为A、B、C、D、E、F的组合源激励下的飞行测量,最终得到三种组合源的测量数据。There are 6 magnetic sources, all of which are vertical magnetic dipole sources with the same parameters. Let the labels of each source be A, B, C, D, E, and F in turn, as shown in Figure 10. The first time the label is A The flight measurement under the combined source excitation of , C, E; the second flight measurement under the combined source excitation marked as B, D, F; the third time is marked as A, B, C, D, E, F Finally, the measurement data of the three combined sources are obtained.
无人机的飞行路线与实施例1相同。数据采集完毕后,按地空瞬变电磁的工作流程进行资料处理、反演解释等工作。The flight route of the unmanned aerial vehicle is identical with embodiment 1. After the data collection is completed, data processing, inversion interpretation and other work are carried out according to the workflow of ground-space transient electromagnetic.
实施例3Example 3
磁性源为8个,均为参数相同的垂直磁偶极子源,设各个源的标记依次为A、B、C、D、E、F、G、H,如图11所示,第一次进行标记为A、C、E、G的组合源激励下的飞行测量;第二次进行标记为B、D、F、H的组合源激励下的飞行测量;第三次进行全部8个组合源激励下的飞行测量,最终得到三种组合源的测量数据。There are 8 magnetic sources, all of which are vertical magnetic dipole sources with the same parameters, and the marks of each source are A, B, C, D, E, F, G, H in turn, as shown in Figure 11, the first Take the in-flight measurements excited by the combined sources marked A, C, E, G; the second time make the in-flight measurements excited by the combined sources marked B, D, F, H; the third time make all 8 combined sources The flight measurement under the excitation finally obtains the measurement data of the three combined sources.
无人机的飞行路线与实施例1相同。数据采集完毕后,按地空瞬变电磁的工作流程进行资料处理、反演解释等工作。The flight route of the unmanned aerial vehicle is identical with embodiment 1. After the data collection is completed, data processing, inversion interpretation and other work are carried out according to the workflow of ground-space transient electromagnetic.
Claims (4)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201310574207.5A CN103576205B (en) | 2013-11-17 | 2013-11-17 | Air-ground transient electromagnetic exploration method based on composite magnetic source technology |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201310574207.5A CN103576205B (en) | 2013-11-17 | 2013-11-17 | Air-ground transient electromagnetic exploration method based on composite magnetic source technology |
Publications (2)
Publication Number | Publication Date |
---|---|
CN103576205A CN103576205A (en) | 2014-02-12 |
CN103576205B true CN103576205B (en) | 2016-12-07 |
Family
ID=50048368
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201310574207.5A Active CN103576205B (en) | 2013-11-17 | 2013-11-17 | Air-ground transient electromagnetic exploration method based on composite magnetic source technology |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN103576205B (en) |
Families Citing this family (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104375195B (en) * | 2013-08-15 | 2017-03-15 | 中国石油天然气集团公司 | Many source multi-component three-dimensional joint inversion methods of time-frequency electromagnetism |
CN104237956B (en) * | 2014-03-06 | 2017-07-04 | 长安大学 | The air-ground detection method of grounded source transient electromagnetic |
CN104360401B (en) * | 2014-12-10 | 2016-10-12 | 中国科学院地质与地球物理研究所 | A kind of transient electromagnetic B field descends objective body geological information method definitely |
WO2016172962A1 (en) * | 2015-04-30 | 2016-11-03 | SZ DJI Technology Co., Ltd. | System and method for landing a mobile platform via a magnetic field |
RU2676556C1 (en) * | 2017-10-10 | 2019-01-09 | Публичное акционерное общество "Газпром" | Method of pulsed ground geological exploration (options) |
CN111796328B (en) * | 2020-07-09 | 2023-08-15 | 长安大学 | A multi-source frequency domain ground-space electromagnetic detection and acquisition system and method |
CN112068211A (en) * | 2020-07-30 | 2020-12-11 | 成都理工大学 | A UAV Semi-Aeronautical Time Domain Electromagnetic Exploration System |
CN112363248B (en) * | 2020-11-24 | 2021-07-27 | 吉林大学 | A device and method for simulating field ground-to-air electromagnetic environment based on three-dimensional coil |
CN113204051B (en) * | 2021-06-10 | 2022-04-15 | 成都理工大学 | Low-rank tensor seismic data denoising method based on variational modal decomposition |
CN115128680B (en) * | 2022-06-28 | 2023-06-02 | 吉林大学 | A transient electromagnetic targeting measurement method based on multi-waveform combination of magnetic sources |
CN118091767B (en) * | 2024-04-19 | 2024-07-26 | 吉林大学 | A ground-to-space time-frequency electromagnetic synchronous pulse excitation sequence encoding method and detection method |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5610523A (en) * | 1991-05-06 | 1997-03-11 | Elliot; Peter J. | Method and apparatus of interrogating a volume of material beneath the ground including an airborne vehicle with a detector being synchronized with a generator in a ground loop |
CN102096113A (en) * | 2010-12-03 | 2011-06-15 | 吉林大学 | Time-domain ground-air electromagnetic detection system and calibration method |
CN102419453A (en) * | 2011-07-15 | 2012-04-18 | 中国科学院地质与地球物理研究所 | Transient electromagnetic ground-space detection method of long wire source |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7681831B2 (en) * | 2006-12-14 | 2010-03-23 | Geotech Airborne Limited | Suspension net for airborne surveying |
-
2013
- 2013-11-17 CN CN201310574207.5A patent/CN103576205B/en active Active
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5610523A (en) * | 1991-05-06 | 1997-03-11 | Elliot; Peter J. | Method and apparatus of interrogating a volume of material beneath the ground including an airborne vehicle with a detector being synchronized with a generator in a ground loop |
CN102096113A (en) * | 2010-12-03 | 2011-06-15 | 吉林大学 | Time-domain ground-air electromagnetic detection system and calibration method |
CN102419453A (en) * | 2011-07-15 | 2012-04-18 | 中国科学院地质与地球物理研究所 | Transient electromagnetic ground-space detection method of long wire source |
Non-Patent Citations (2)
Title |
---|
激励信号对地-空瞬变电磁响应的影响分析;关珊珊 等;《电波科学学报》;20120831;第27卷(第4期);第767页第1栏第2段倒数第3-6行,及图1、3 * |
瞬变电磁法理论与应用研究进展;薛国强 等;《地球物理学进展》;20070831;第22卷(第4期);第1199页第1栏倒数第3段第4行 * |
Also Published As
Publication number | Publication date |
---|---|
CN103576205A (en) | 2014-02-12 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN103576205B (en) | Air-ground transient electromagnetic exploration method based on composite magnetic source technology | |
US9845153B2 (en) | In-situ power charging | |
CN102736114B (en) | Equipment and method for electromagnetic and its comprehensive prospecting | |
US8008921B2 (en) | Surveying using vertical electromagnetic sources that are towed along with survey receivers | |
CN104749640B (en) | Multi-source multi-frequency ground-air electromagnetic detection emission method | |
CN106908847B (en) | A kind of air-ground nuclear magnetic resonance underground water detection system and detection method | |
CN109738958B (en) | Ocean controllable source electromagnetic detection system | |
US20140012505A1 (en) | Multi-component electromagnetic prospecting apparatus and method of use thereof | |
US11531134B2 (en) | Multi-sensor system for airborne geophysical prospecting and method | |
AU2016231570B2 (en) | Airborne platform for aircraft, comprising attitude correcting means, and associated tow hitch assembly | |
CN109814161B (en) | A kind of aerial magnetic resonance groundwater detection device and method | |
CN104020496B (en) | A kind of surface controllable source electromagnetic exploration method of mode axially in line | |
CN110471117A (en) | A kind of aviation electromagnetic detection system and method | |
CN105301663A (en) | Time-frequency electromagnetic exploration data air acquisition device and system | |
CN110703342B (en) | A full coverage anti-jamming artificial source electromagnetic detection method | |
US3020471A (en) | Method and apparatus for the detection of ore bodies | |
CN115826058A (en) | Ground-air transient electromagnetic horizontal gradient measuring method for rotor unmanned aerial vehicle | |
CN106932827A (en) | Ocean controllable source time-frequency electromagnetic data acquisition system and method | |
CN119270371A (en) | Unmanned aerial vehicle array multi-component electric field and magnetic field collaborative detection system and detection method | |
Törnqvist | Some practical results of airborne electromagnetic prospecting in Sweden | |
AU2015249137B2 (en) | Multi-Component Electromagnetic Prospecting Apparatus and Method of Use Thereof | |
CN114488315A (en) | A magnetic source ground-space transient electromagnetic three-component measurement system and measurement method | |
CN110595468A (en) | Three-component induction coil attitude measurement system and method based on deep learning | |
CN207932003U (en) | A kind of monitoring of ionizing radiation unmanned plane and monitoring of ionizing radiation UAV system | |
RU2649658C2 (en) | Method and system of aeroelectric works |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
ASS | Succession or assignment of patent right |
Owner name: XI'AN RESEARCH INSTITUTE OF CHINA COAL TECHNOLOGY Effective date: 20140123 |
|
C41 | Transfer of patent application or patent right or utility model | ||
C53 | Correction of patent for invention or patent application | ||
CB03 | Change of inventor or designer information |
Inventor after: Mao Lifeng Inventor after: Wang Xuben Inventor after: Qin Qingyan Inventor before: Mao Lifeng Inventor before: Wang Xuben |
|
COR | Change of bibliographic data |
Free format text: CORRECT: INVENTOR; FROM: MAO LIFENG WANG XUBEN TO: MAO LIFENG WANG XUBEN QIN QINGYAN |
|
TA01 | Transfer of patent application right |
Effective date of registration: 20140123 Address after: Three road 610059 Sichuan city of Chengdu province Chenghua District Erxian Qiaodong No. 1 Applicant after: Chengdu University of Technology Applicant after: Xi'an Research Institute, CCTEG Address before: Three road 610059 Sichuan city of Chengdu province Chenghua District Erxian Qiaodong No. 1 Applicant before: Chengdu University of Technology |
|
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
CB03 | Change of inventor or designer information |
Inventor after: Wang Xuben Inventor after: Mao Lifeng Inventor after: Gao Song Inventor after: Li Linlin Inventor after: Qin Qingyan Inventor before: Mao Lifeng Inventor before: Wang Xuben Inventor before: Qin Qingyan |
|
COR | Change of bibliographic data | ||
C14 | Grant of patent or utility model | ||
GR01 | Patent grant |