海洋瞬变电磁探测发射技术研究
详细信息    本馆镜像全文|  推荐本文 |  |   获取CNKI官网全文
摘要
海洋对于人类的生存和发展极其重要,海底大部分资源有待查明和开发,近年来,在海底探测的应用逐渐由地震方法独立展开到海洋可控源电磁法(CSEM)与地震方法联合进行,并使得海洋CSEM成为国际热点,目前海洋底CSEM探测主要针对深海环境下的油气资源,而在浅海,对于解决海洋工程问题的海底电磁探测技术有待进一步研究。本文针对浅海环境下的海底工程探测问题,借鉴陆地电磁探测方法的成功经验,研究瞬变电磁时间域CSEM方法用于浅海底低阻目标探测的基础理论、方法及发射关键技术。首先,为研究发射系统参数对测量结果的影响,给出了相应的电磁响应计算公式;其次,根据电磁响应计算公式,通过数值计算,分析海洋瞬变电磁方法在不同水深环境下的时间域或频率域电磁响应,仿真了发射源主要参数发射磁矩、发射频率、关断时间和天线高度对电磁响应的影响;研究了发射天线参数对海底CSEM探测的影响以及接收系统频带宽度对浅层分辨率的影响;最后,根据仿真研究及分析计算的结果,采用分段控制思想,设计了满足海底CSEM探测的发射系统及发射天线,选取了接收系统接收频带宽度及接收线圈,组成海洋瞬变电磁探测系统,实验结果验证了海洋瞬变电磁探测发射系统的有效性及可用性。
The oceans are very important to the existence and development of the human being, and most of the sources in the ocean floor are to be explored and exploited. The shell of the ocean is covered by sea water with different depth. The geophysical methods are essential means for the exploring and study of ocean floor. Seismic method is one of the main methods in geophysics, which utilizes the different propagation characteristics of elastic wave in different earth media, and it has perfect imaging effect to the stratum and structure of ocean floor. But in the conditions of salt-dome and volcanic rock, the result of seismic prospecting is not good because of the absorption and diffusion of elastic waves. Other physical properties should be used to explore the inner structure of the area. Among all kinds of physical properties, the conductivity is most commonly adopted. Electromagnetic (EM) methods utilize the difference of conductivity to explore the change of inner structure of seafloor. Consequently, marine electromagnetic method is another main marine geophysical method. Marine electromagnetic method has good applicability and wide range of exploration depth. In beach and shallow sea, seafloor electromagnetic detection technology can meet the requirement of geological environment investigation in marine constructions, for example, constructing offshore drilling platform, laying cable and pipes, building seafloor tunnel, warehouse and cross-sea bridges. In recent years, the application of marine controlled-source electromagnetic method (CSEM) to the seafloor detection has been an international hot topic. By far, seafloor CSEM detection mainly aims at the oil and gas resources in the deep sea, while in shallow sea, the seafloor electromagnetic technology to resolve the problem of marine engineering needs to be further studied.
     This paper adopts the high resolution electromagnetic detection technology to seek new techniques and equipments for seafloor engineering in offshore and detecting mine resources in beach and shallow sea. With the successful experience of electromagnetic detection on land, the theory base and key transmitting technology of time-domain CSEM with Transient Electromagnetic (TEM) applied to target detection in the shallow sea is studied. First, the electromagnetic response formulas are derived for the analysis of the impact of transmitting parameters on measurement results. Then, according to the electromagnetic response formulas, the time-domain electromagnetic responses of TEM in different water depth are computed and analyzed through numerical calculation. The impact of main transmitting parameters, including magnetic moment, frequency, off-time and antenna height, on the electromagnetic response is simulated. The impact of transmitting antenna parameters on the seafloor CSEM exploration and the impact of receiver bandwidth on the resolution of shallow seafloor are both studied. Finally, according to the results of simulation and analysis, the transmitter system which can meet the requirement of seafloor CSEM exploration is development; the transmitting antenna is designed; the receiver coil with appropriate bandwidth is selected. All the works are supported by a project from the 863 program. Along with the receiver system developed by the project, the seafloor CSEM detection system is formed, and the performance of the transmitter system is tested by experiments.
     The main study work and achievements of this paper include:
     1. According to the principles of TEM time domain seafloor CSEM detection technology, it derived the frequency and time domain electromagnetic response equations of 1D marine geoelectrical model. By the simplification of them, it obtained the time domain induced voltage analysis formulas of homogeneous seafloor in the conditions of infinite depth and finite depth, respectively. Utilizing these formulas, we can simulate the time-domain and frequency domain electromagnetic responses of magnetic resources in different water depth, thus found theoretical basis for the analysis of the influence of transmitter parameters on the detecting results.
     2. Through the simulation of marine CSEM using TEM, it studied the impact of transmitter parameters on the electromagnetic response. The results show that, in shallow seafloor detection which requires measurement at early delay time, transmitting coil of small radius should be adopted. The upper limit of transmitting frequency is mainly determined by the biggest delay time required in sea floor detection and the admitted impact degree of the rise edge on the measured field. The slope time has impact on seafloor detection. The longer slope time predicates that the earliest time that can be measured is later, which leads to weaker electromagnetic anomaly and lower S/N. Consequently, when we detect the shallow seafloor, especially the thin resistive layer, small slope time should be carried out to obtain large electromagnetic anomaly. However, since the electromagnetic anomaly due to shallow medium will exist for a certain time, we can still find the shallow target according to the electromagnetic anomaly at late delay time besides poor anomaly when the slope time is a little big. In spite of that, the slope time shouldn’t be too big, or the anomaly due to shallow target may be lost. The impact of the antenna height on the measurement result is mainly presented in the early delay time. The higher the height, the later delay time is required for seafloor resistivity resolution. Because the electromagnetic response at late delay time is small and the antenna height has negative impact on the anomaly, we should let antenna height as small as possible in seafloor detection if the condition permits. The simulation results supply the design of seafloor transmitter systems with theoretical guidance and basis.
     3. It analyzed the influence of the magnitude of transmitting current and the number of windings of the transmitter coil on the off-time of the transmitter system, when multiple-winding small coil is deployed as transmitter coil, and developed multiple-winding small transmitter coil. It also studied the impact of the receiving coil bandwidth on the resolution, so as to provide theoretical guidance for the development of receiver system and the selection of receiver coil.
     4. It studied the characteristic and demands of the transmitter system of marine TEM detection, according to which, the driving circuits of switching device are designated using independent components to supply short off-time driving signal with negative bias voltage characteristic to transmitting bridge. In view of the characters of the transmitting current in different stages, including current rising, flat top, current descending and reverse current overshooting, a piecewise control idea is presented. Independent controlling circuits and controlling voltages are used in each stage, and the currents in different stages are controlled deploying different controlling strategies, so as to form a ladder current output pulse. And this resolves the contradiction between gradual rising and descending edges and the flat top current of the pulse in traditional magnetic source EM transmitter, and reduces the rising and descending time of transmitting current effectively. It developed a recording unit of the transmitting current wave to completely record the wave, which provides the foundation to the elimination of the following first field. To increase the overall electromagnetic compatibility, guarantee the system to work robustly, and avoid the influence of the circuits each other, it implemented a multi-output of transformer using the enwinding manner of stranded wire and double winding and a multiplexed double ended push-pull switch power supply.
     5. Indoor simulation experiments, outdoor detection experiments on land seafloor detection experiments of marine TEM detection are carried out. Though these experiments, the form of observation device, survey manner and work parameters of the transmitter system are determined. By the indoor simulation experiments, it verified the detection efficiency of devices of small size central loop, small size coincident loop and small size dipole-dipole devices, respectively. The results show that all of them can detect the low conductivity anomaly. Compared to each other, the dipole-dipole device is the best, while the coincident loop device is the worst. Through the man made anomaly detection experiments on the land, it compared the detection effectivity of the device with considerable larger size central loop and that with small size one. The results show that, for the detection of shallow layer, the device with small size is better than that with large size. The results from the seafloor detection experiments indicate that, the detection ability of the small size coincident loop device is weak. On the other hand, though the dipole-dipole device is better, the polar distance of it is susceptible to the environment underwater, and the shapes of the cross curves are odd and complex, which is not suitable for the data processing and explanation afterward. Consequently, we select the small size central loop as the observation device in the seafloor detection experiments, and we detected two unknown oil pipelines successfully, which verified the effectivity of the marine TEM detection methods and system.
     The main innovations of this paper include the followings:
     1. It derived the frequency and time domain electromagnetic response equations of 1D marine geoelectrical model and the time domain induced voltage analysis formulas of homogeneous seafloor in the conditions of infinite depth and finite depth. All these provide the theoretical foundation and mathematical model for the analysis of the influence of transmitter parameters on the detecting results.
     2. It presented a piecewise control idea which means providing independent control according to the characteristics of each stage, so it implements piecewise control over the complete output transmitting current wave. As a result, it effectively reduced the time of rising and descending edges. It developed a transmitter system of for marine TEM detection, which can be applied to seafloor engineering exploration.
     3. Based on the results of simulation and model experiments, it determined the form of the transmitting device suitable for marine TEM detection, and successfully applied the TEM detection methods deployed on land to seafloor.
     The achievements of this paper build the theoretical guidance for the application of CSEM to the investigation of seafloor engineering environment in our country, and provide theoretical basis, measuring methods and instruments for the TEM detection applied to the investigation of seafloor engineering environments.
引文
[1]何继善,鲍力知.海洋可控源电磁法研究现状何进展[J],地球物理学进展, 1999, 14(1):7-39.
    [2]王琦,朱而勤.海洋沉积学[M].北京:科学出版社,1989.
    [3]严似松.海洋工程导论[M].上海:上海交通大学出版社,1987.
    [4]金庆焕.南海地质与油气资源[M].北京:地质出版社,1989.
    [5]吕炳全,孙志国.海洋环境与地质[M].上海:同济大学出版社,1997.
    [6]许东禹,刘锡清,张训华,等.中国近海地质[M].北京:中国地质出版社,1997.
    [7]蒋邦远.实用近区磁源瞬变电磁法勘探[M].北京:地质出版社,1998.
    [8]米萨克N.纳比吉安主编,赵经祥等译,勘察地球物理电磁法(第一卷)[M].北京:地质出版社,1992.
    [9] Steven Constable and Leonard J. Srnka. An introduction to marine controlled-source electromagnetic methods for hydrocarbon exploration[J], GEOPHYSICS, 2007, 72(2):WA3–WA12.
    [10] David Andréis1 and Lucy MacGregor1. Controlled-source electromagnetic sounding in shallow water: Principles and applications[J], GEOPHYSICS, 2008, 73(1):F21–F32.
    [11] KURT STRACK, CENGIZ ESMERSOY, and NORMAN ALLEGAR. Introduction to This Special Section: CSEM[J], THE LEADING EDGE,2007,3:323-325.
    [12] Michael J. Tompkins and Leonard J. Srnka, Marine controlled-source electromagnetic methods—Introduction[J], GEOPHYSICS, 2007, 72(2):WA1–WA2.
    [13]邓明,候胜利,王广福等.中国海底地球物理探测仪器的新进展[J],勘探地球物理进展, 2004, 27(4):241-245.
    [14]金翔龙,初凤友.大洋海底矿产资源研究现状及其发展趋势[J],东海海洋2003, 21(1):1-4.
    [15]江怀友,潘继平,邵奎龙,等.世界海洋油气资源勘探现状[J].中国石油企业,2008(03):77-79.
    [16]康竹林.中国沿海大陆架油气勘探开发现状及前景[J].海洋地质动态,1998(10):1-4.
    [17]常城,舒先林.中国海洋油气开发的战略分析[J].石油化工技术经济,2007,23(2):1-6.
    [18]胡茂炎.天然气水合物新世纪一种重要的接替资源[J].探矿工程,2002,(4):1-2.
    [19]雷怀彦,王先彬,房玄,等.天然气水合物研究现状与未来挑战[J].沉积学报,1999,17(3):493-498.
    [20]郭玉松. TEM法在工程勘察中的研究与应用[J].工程勘察,199(81):70-72.
    [21]林君.电磁探测技术在工程与环境中的应用现状[J].物探与化探,2000,24(3):167-177.
    [22]朱德兵.工程地球物理方法技术研究现状综述[J].地球物理学进展,2002,17(1):163-170.
    [23]张保祥,刘春华,汪家权.瞬变电磁法在地下水勘查中的应用[J].水利水电科技进展,2002,22(4):23-29.
    [24]张运霞,韩自豪,周建雄,等.瞬变电磁法在煤层水探测中的应用[J].中国煤田地质,2005,17(6):45-47.
    [25]王东坡,曾孝箴,薛林福,等.海洋阵列大地电磁测深法在辽东湾滩海深部地质构造研究中的应用[J].石油与天然气地质,2000,21(4):293-299.
    [26]罗维斌.伪随机海洋可控源多道电磁测深法研究[D].长沙,中南大学,2007.
    [27] Kurt Strack and Norman Allegar, KMS Technologies, Svein Ellingsrud , Electromagnetic Geoservices. Marine time domain CSEM: an emerging technology[C], SEG Las Vegas 2008 Annual Meeting 653-656.
    [28] R.N.EdWards and A.D.Chave, A Transient Electric Dipole-Dipole Method for Mapping the Conductivity of the Sea Floor[J], Geophysics, 1986, 51(4):984-987.
    [29] R.N. Edwards, L.K.Law, J.M.Delaurier, On Measuring the Electrical Conductivity of the Oceanic Crust by a Modified Magnetometric Resistivity Method[J], Journal of Geophysical Research, 1981, 86(B12):11609-11615.
    [30] L MacGregor. Imaging sub-basalt sediments using marine electromagnetic sounding[C]. AAPG Hedberg Conference, September 2002, Stavanger, Norway.
    [31] S Constable. Marine electromagnetic methods—A new tool for offshore exploration[J]. The Leading Edge, 2006:438-444.
    [32] P A Wolfgram, R N Edwards, L K Law, et al. Polymetallic sulfide exploration on the deep sea floor: The feasibilly of the MINI-MOSES experiment[J]. Geophysics, 1986, 51(9):1808-1818.
    [33] M J Tompkins, L J Srnka. Marine controlled-source electromagnetic methods—Introduction[J]. Geophysics, 2007, 72(2): WA1-WA2.
    [34] N Edwards, Marine controlled source electromagnetic principles, methodologies, future commercial applications[J]. Surveys in Geophysics, 2005, 26:675-700.
    [35] E S Um, D L Alumbaugh. On the physics of the marine controlled-source electromagnetic method[J]. Geophysics, 2007, 72(2):WA13-WA26.
    [36] T Eidesmo, S Ellingsrud, L M MacGregor,et al. Sea Bed Logging (SBL), a new method for remote and direct identification of hydrocarborn filled layers in deepwater areas[J]. First Break, 2002, 20:144-152.
    [37] D Andreis, L MacGregor. Controlled-source electromagnetic sounding in shallow water: Principles and applications[J]. Geophysics, 2008, 73(1):F21-F32.
    [38] P R Bannister. Determination of the electrical conductivity of the sea bed in shallow waters[J]. Geophysics, 1968, 33(6):995-1003.
    [39] R N Edwards, L K Law, J M Delaurier. On measuring the electrical conductivity of the oceanic crust by a modified magnetometric resistvivity method[J]. J. Geophys. Res., 1981, 86:11609-11615.
    [40] P D Aversana. Marine CSEM in shallow water: acquisition and interpretation strategies[C]. SEG/New Orleans 2006 Annual Meeting, 2006, P724-728.
    [41] R N Edwards. On the resource evaluation of marine gas hydrate deposits using sea-floor transient electric dipole-dipole methods[J]. Geophysics, 1997, 62(1):63-74.
    [42] T Eidesmo, S Ellingsrud, S E Johansen, et al. Long-offset techniques head advances in marine electromagnetic surveying[J]. Oil & Gas Journal, 2005(Nov):P34-41.
    [43] J Chen, G M Hoversten, D Vasco,et al. A Bayesian model for gas saturation estimation using marine seismic AVA and CSEM data[J] Geophysics, 2007, 72(2):WA85-WA95.
    [44] J Hesthammer, M Boulaenko. The offshore EM challenge[J]. First Break, 2005, 23(Nov):59-66.
    [45] G M Hoversten, F Cassassuce, E Gasperikova,et al. Direct reservior parameter estimation using joint inversion of marine seismic AVA and CSEM data[J]. Geophysics, 2006, 71(3):C1-C13.
    [46] Z Hou, Y Rubin, G M Hoversten, et al. Reservoir-parameter identification using minimum relative entropy-based Bayesian inversion of seismic AVA and marine CSEM data[J]. Geophysics, 2006, 71(6):O77-O88.
    [47] S E Johansen, H E F Amundsen, T Rosten, et al. Subsurface hydrocarbons detected by electromagnetic sounding[J]. First Break, 2005, 23(March):31-36.
    [48] C K Choo, M Rosenquist, E Rollett,et al. Detecting hydrocarbon reservoir with seabed loggingTM in deepwater sabah, Malaysia[C]. SEG/New Orleans 2006 Annual Meeting, P714-718.
    [49] M Darnet, M C K Choo, R E Plessix,et al. Detecting hydrocarbon reservoirs from CSEM data in complex settings: Application to deepwater Sabah, Malaysia[J]. Geophysics, 2007, 72(2):WA97-WA103.
    [50] B Farrelly, C Ringstad, S E Johnstad, et al. Remote characterization of hydrocarbon filled reservoirs at the Troll Field by Sea Bed Logging[C]. EAGE Fall Research Workshop, Rhodes,Greece, 19th-23rd September 2004.
    [51] D Smit, S Saleh, J Voon,et al. Recent controlled source EM results show positive impact on exploration at Shell[C]. SEG/New Orleans 2006 Annual Meeting, P3536-3541.
    [52] K A Weitemeyer, S C Constable, K W Key, et al. First results from a marine controlled-source electromagnetic survey to detect gas hydrates offshore Oregon[J]. Geophysics Research Letters, 2006, 33(L03304).
    [53] A Gribenko, M Zhdanov. Rigorous 3D inversion of marine CSEM data based on the integral equation method[J]. Geophysics, 2007, 72(2):WA73-WA84.
    [54] P Weidelt. Guided waves in marine CSEM[J]. Geophys. J. Int., 2007, 171:153-176.
    [55] J I Nordskag, L Amundsen. Asymptotic airwave modeling for marinecontrolled-source electromagnetic surveying[J]. Geophysics, 2007, 72(6):F249-F255.
    [56] L Amundsen, L Loseth, R Mittet,et al. Decomposition of electromagnetic fields into upgoing and downgoing compoments[J]. Geophysics, 2006, 71(5):G211-G233.
    [57] S Constable, C J Weiss. Mapping thin resistors and hydrocarbons with marine EM methods: Insights from 1D modeling[J]. Geophysics, 2006, 71(2):G43-G51.
    [58] C J Weiss, S Constable. Mapping thin resistors and hydrocarbons with marine EM methods, Part II--Modeling and analysis in 3D [J]. Geophysics, 2006, 71(6):G321-G332.
    [59] K Weitemeyer, S Constable, K Key. Marine EM techniques for gas-hydrate detection and hazard mitigation [J]. The Leading Edge, 2006(May):629-632.
    [60]渤海找到亿吨级大油田(海讯)[J].中国海洋平台,1999(04):44.
    [61]徐嘉信.中国海上油气田开发特点及其前景[J].中国海洋平台,1994,(z1):8-28.
    [62]陈建文,吴志强.天然气水合物的地球物理识别技术[J].海洋地质动态,2004,20(6):1-5.
    [63]杨建文,R N Edwards.用于海底电导率填图的可控源时域电磁法[J].中国有色金属学报,1998,8(4):705-713.
    [64]王一新,王家林,王家映,等.瞬变电磁系统探测海底电导率的研究[J].地球物理学报,1998,41(6):841-847。
    [65]邓明,沈高山,余平,等.基于麦克斯韦理论的海底大地电磁探测技术[J].海洋技术,2003,22(2):44-47.
    [66]邓明,李哲,魏文博,等.带远参考测量方式的海底大地电磁同步采集技术[J].地质与勘探,2003,39(5):77-80.
    [67]邓明,魏文博,谭捍东,等.海底大地电磁数据采集器[J].地球物理学报,2003,46(2):217-223.
    [68]邓明,魏文博,邓靖武,等.海底天然大地电磁场的探测[J].测控技术,2003,22(1):5-8.
    [69]丁建荣,王勇,于鹏,等.浅海电磁道分离同步采集的大地电磁测深观测试验[J].石油地球物理勘探,2006,41(1):107-110.
    [70]刘长胜.海底可控源电磁探测数值模拟与实验研究[D].长春,吉林大学,2009.
    [71] C J Weiss. The fallacy of the“shallow-water problem”in marine CSEM exploration[J]. Geophysics, 2007, 72(6):A93-A97.
    [72] P D Aversana. Marine CSEM data interpretation: Pitfalls and possible solutions[J]. The Leading Edge, June 2007:686-691.
    [73] P J Summerfield, L S Gale, X Lu, et al. Marine CSEM Acquisition Challenges, SEG Expanded Abstracts [J]. 2005, 24(538).
    [74]李桐林,林君,刘福春,等.国内外海洋大地电磁测深的发展综述[J].国外地质勘探技术,1998(4):1-10.
    [75]李慧.海洋瞬变响应理论计算及浅海底瞬变电磁探测技术研究[D].长春,吉林大学,2007.
    [76] K Baba. Electrical structure in marine tectonic settings[J]. Surveys in Geophysics, 2005, 26:701-731.
    [77] A A Kaufman, G V Keller. Frequency and transient soundings [M]. New York: Elsevier Science Publishers, 1983.
    [78] L O Loseth, H M Pedersen, B Ursin, et al. Low-frequency electromagnetic fields in applied geophysics: Waves or diffusion[J]. Geophysics, 2006, 71(4):W29-W40.
    [79] N B Christensen, K Dodds. 1D inversion and resolution analysis of marine CSEM data[J]. Geophysics, 2007, 72(2):WA27-WA38.
    [80] A P Raiche, R G Gallagher. Apparent resistivity and diffusion velocity [J]. Geophysics, 1985, 50(10):1628-1633.
    [81] M N Nabighian. Quasi-static transient response of a conducting half-space—An approximate representation [J]. Geophysics, 1979, 44:1700-1705.
    [82] J E Reid, J C Macnae. Comments on the electromagnetic“somke ring”concept [J]. Geophysics, 1998, 63(6):1908-1913.
    [83] T Wang. The electromagnetic smoke ring in a transversely isotropic medium [J]. Geophysics, 2002, 67(6):1779-1789.
    [84] R N Edwards, D C Nobes, E G Trevino. Offshore electrical exploration of sedimentary basins: The effects of anisotropy in horizontally isotropic, layered media[J]. Geophysics, 1984, 49(5):566-576.
    [85] Y Li, S Constable. 2D marine controlled-source electromagnetic modeling: Part 2-- The effect of bathymetry [J]. Geophysics, 2007, 72(2):WA63-WA71.
    [86] Cheesman, S. J., R. N. Edwards, and A. D. Chave, On the theory of sea-floor conductivity mapping using transient electromagnetic systems[J], Geophysics, 1987, 52(2):204-217.
    [87]陈明生.电偶源瞬变电磁测深研究(一)--基本原理[J].煤田地质与勘探.1999.27(1):55-59.
    [88]陈明生.电偶源瞬变电磁测深研究(二)--_瞬变电磁场的求解方法[J].煤田地质与勘探.1999.27(2):54-57.
    [89] F N Kong. Hankel transform filters for dipole antenna radiation in a conductive medium[J]. Geophysical Prospecting, 2007, 55:83-89.
    [90] Edwards, R. N., Two-dimensional modeling of a towed in-line electric dipole-dipole sea-floor electromagnetic system: The optimum time delay or frequency for target resolution[J], Geophysics, 1988, 53(6):846-853.
    [91] R.N.EdWards and S.J.Cheesman,Two-Dimensionsl Modeling of a Towed Transient Magnetic Dipole-Dipole Sea Floor EM System[J],Journal of Geophysics,1987(61):110-121.
    [92] B R Spies. Depth of investigation in electromagnetic sounding methods [J]. Geophysics, 1989, 54(7):872-888.
    [93]李实,李创社,张鹏飞,包松清,宋建平.高性能瞬变电磁仪的研制及应用[J].北京:物探与化探.2002,24(1):76-80.
    [94]李实,宋建平,李创社.瞬变电磁仪中几种干扰的消除方法[J].西安:西安交通大学学报.2001,35(4):373-381.
    [95]李实,李创社,张鹏飞,包松清,宋建平.高性能瞬变电磁仪的研制及应用[J].北京:物探与化探.2002,24(1):76-80.
    [96]周逢道,林君等.浅海底瞬变电磁探测系统关断沿影响因素研究[J].电波科学学报,2006,21(4):532-535.
    [97]周逢道,林君等.浅海底瞬变电磁探测接收天线的频率特性对探测结果的影响[J].地球物理学进展,2006,21(4):1342-1345.
    [98] Hoy Lee.A High-Bandwidth Induction Sensor Coil[J],The Institute of Physics, 1982, 15:1017-1019.
    [99] Macnae, J. C., Y. Lamontagne, and G. F. West, Noise processing techniques for time-domain EM systems[J], Geophysics, 1984,49(7):934-948.
    [100] Rune Mittet and Tor Schaug-Pettersen. Shaping optimal transmitter waveforms for marine CSEM surveys[J], GEOPHYSICS, 2008,73(3):F97–F104.
    [101]刘国栋.电磁法及电法仪器的新进展和应用[J].石油地球物理勘探,2004,39(增刊):46-51.
    [102]周国华.基于DSP的瞬变电磁探测系统设计与实现[D].长春,吉林大学,2006.
    [103]徐立忠.基于ATEM-Ⅱ的改进型电磁法发射系统设计与实现[D].长春,吉林大学,2008.
    [104]周国华,林君,周逢道等.浅海底瞬变电磁探测发射系统研究[J].电力电子技术,2006,40(5):58-61.
    [105]王静.ATTEM发射机发射电流下降沿记录关键技术研究[D].长春:吉林大学,2004.
    [106]周逢道,林君,周国华等.瞬变电磁探测发射电流波形记录单元设计[J],吉林大学学报(工学版),2009, 39 (02):0541-0545.
    [107] Zhou Fengdao,LinJun,Liu Changsheng.Study on work parameters of seafloor towed survey using transient electromagnetic systems[C]. PIERS 2007 Beijing China.
    [108] P F Lezaeta, A D Chave, R L Evans. Correction of shallow-water electromagnetic data for noise induced by instrument motion[J]. Geophysics, 2005, 70(5):G127-G133.

© 2004-2018 中国地质图书馆版权所有 京ICP备05064691号 京公网安备11010802017129号

地址:北京市海淀区学院路29号 邮编:100083

电话:办公室:(+86 10)66554848;文献借阅、咨询服务、科技查新:66554700