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TELKOMNIKA Indonesian Journal of Electrical Engineering
Vol.12, No.1, January 2014, pp. 406 ~ 414
DOI: http://dx.doi.org/10.11591/telkomnika.v12i1.4144  406
Received June 26, 2013; Revised August 27, 2013; Accepted September 19, 2013
Design on the Time-domain Airborne Electromagnetic
Weak Signal Data Acquisition System
Xiao-ling Zhong, Yong Guo*, Han-chuan Dong
College of Information Science and Technology
Chengdu University of Technology, Chengdu, China, 610059
*corresponding author, e-mail: guoy@cdut.edu.cn
Abstract
According to principle of transient electromagnetic method as well as its signal characteristics,
this paper designed and implemented a time-domain airborne electromagnetic weak signal data
acquisition system. With the use of the floating-point amplification technology, the system amplifies the
weak transient electromagnetic signal dynamically. CPLD and DSP were used as the decoding control
circuit and the main controller for processing the sampled data, respectively. The transient electromagnetic
signal acquisition system, which was designed with a dynamic range up to 144dB and a sampling rate up
to 100 kHz, meets the requirements of the high sampling rate with high precision and it has been applied in
the time-domain fixed-wing airborne electromagnetic mineral exploration.
Keywords: DSP, CPLD, ATEM, Floating-point Amplifier, Data Acquisition
Copyright © 2014 Institute of Advanced Engineering and Science. All rights reserved.
1. Introduction
At present, China is implementing land resources survey and geological security
projects based on mineral development, and China is also making efforts to identify the status of
land resources as soon as possible. During the Eleventh Five-Year Plan period, China has
launched a research and development project for geological prospecting using high-precision
airborne geophysical technology and equipment. The project, “Fixed-wing Time-domain
Airborne Electromagnetic Exploration Systems Research and Development”, undertaken by
IGGE,is an important topic in State High-Tech Development Plan (863 Program) project
“Airborne Geophysical Exploration Technology Systems”.
According to the principle of transient electromagnetic method, for the Time-domain
Airborne Electromagnetic (ATEM) weak signal, this paper presents researches and designs of a
data acquisition system based on DSP. The transient electromagnetic is a geophysical
exploration method, with high sensitivity in resistivity change, fewer limitations in ground
conditions, good probing depth. It is widely used in many areas, including as metal mineral
exploration, drilling and aviation and marine activities.The time-domain airborne electromagnetic
method, a branch of the airborne electromagnetic methods, combines aviation with geophysical
technologyby using aircrafts as delivery platforms to load geophysical equipment and complete
the data acquisition of geophysical information. Aero Geophysical Survey is one of the important
means of completing national geological survey projects with deep exploration depth. Large
area survey can be facilitated at low cost and high efficiency, which plays an important role in
the national economy development Error! Reference source not found..
2. ATEM System
2.1. Principle of Transient Electromagnetic Method
The transient electromagnetic method, also known as Time-domain Electromagnetic
Method (TEM), is based on fundamental electromagnetic induction principles shown in Figure 1.
A transmitting coil is firstly put on the ground or in the air. By changing the current flowing
throught, a constantly varying electromagnetic field (named as “primary field”) can be generated
in the space surrounding the coil, producing an induced current in the rock and mineral beneath.
The varying current induced will also produce a varying electrmagnetic field (named as
“secondary field”) in the space around the ore body. The receiving coil is then used to obtain the
 ISSN: 2302-4046 TELKOMNIKA
TELKOMNIKA Vol. 12, No. 1, January 2014: 406 – 414
407
information of the secondary field, including resistivity, conductivity and other physical
characteristics. Further analysis based on the information obtained will help us to investigate the
distribution of the underground mine sources [2].
Figure 1. The schematic diagram showing the basic principles of the transient electromagnetic
method
In order to improve the sensitivity of resistivity characterisation, reduce the limitation of
ground conditions, deepen the probing depth and get better synchronization between
transmitters and receivers, the transient electromagnetic method has recently become one of
the most important exploration method in geophysical exploration field. It has been rapidly
applied in metal mineral exploration, water resource survey, environment protection, aviation
and marine activities Error! Reference source not found..
2.2. Characteristics of Transient Electromagnetic Signal
In the electrical prospecting method, the intensity secondary field response of
underground conductors decays exponentially with a decay function Error! Reference source not
found.. The function is:
e
tK
t


/
)(e

 (1)
Where e(t) represents the intensity of the secondary field response of conductive body,
K is a time-independent constant, t is the time elapsed, and  is a time constant dependent on
the property of the conductive body.
Figure 2 is showing the characteristic curve of the TEM signal and its features are as
follows:
ISSN: 2302-4046 
Design on the Time-domain Airborne Electromagnetic Weak Signal Data... (Yong Guo)
408
Figure 2. Characteristic curve of the TEM signal
(1) Large dynamic range: signal amplitude decays from n×105µV to n×10-1µV, up to 120db of
dynamic range.
(2) Wide band: The frequency range of the TEM signal collected in this topic is 20 Hz to 25 kHz.
(3) Quick signal attenuation: Early TEM signals decay quicker and late signals decay slower.
2.3. ATEM System
Airborne Time-domain Electromagnetic Method Airborne Time-domain Electromagnetic
Method (ATEM) is an important branch of airborne electromagnetic method (AEM).Its
development is based on traditional ground electromagnetic method with the implementation of
aerial survey. Similar as the ground electromagnetic methods, ATEM has its unique
advantages, including fast speed, low cost, high efficiency, deep probing depth and etc.
Besides, its application can be extended to geophysical survey work in areas where terrestrial
method cannot be applied due to complexity, including swamps, deserts, lakes, forests and
residential areas. ATEM is an effective exploration method and it is essential for land resources
survey Error! Reference source not found..
Figure 3 is showing schematic diagram of the frequency-domain airborne
electromagnetic survey system platform developed by IGGE. The fundamental principle of the
frequency-domain airborne electromagnetic method is the same as that of the time-domain
method Error! Reference source not found.. The platform employs domestic Y12 IV aircrafts with
transmiting and receiving coils installed at both ends of the fixed wings. Cabin equipment
includes transmitters, receivers, aviation single-ray optically pumped magnetometer, aviation
spectrometer, airborne geophysical data collection system as well as GPS navigation and
positioning system.
Figure 3. Schematic diagram of the frequency-domain airborne electromagnetic survey system
ATEM can be used to investigate the magnetotelluric properties, such as conductivity,
permeability and etc. As the working platform of AEM is the aircraft, the main technical features
of the AEM system are related not only to the instrument itself, but also to the type of the aircraft
and the unique modifications made upon the airplane (Man Yan-long, 2009).
3. Floating-Point Amplification Technology
 ISSN: 2302-4046 TELKOMNIKA
TELKOMNIKA Vol. 12, No. 1, January 2014: 406 – 414
409
Floating-point amplification means the input signal can be amplified with dynamical
extent and devices based on the principle of floating-point amplification are called floating-point
amplifiers.
Figure 4 shows the schematic diagram of a floating-point amplifier which is composed
of pre-sampling circuit, the second sampling circuit, programmable amplifying circuit and
encoding circuit Error! Reference source not found..
Figure 4. Schematic diagram of a floating-point amplifier
4. System Design Program
Figure 5 shows the overall system design program. The components enclosed in the
dashed box is a floating-point amplifier circuit which is controlled by CPLD. Firstly, the TEM
signal passes through the preamplifier and a low pass filter.Then CPLD will collect the raw
signal with its internal coding circuit controlling the dynamic amplification. DSP then samples the
signal again and transmits the results, which will also be displayed on the LCD, to the host
computer.
Figure 5. Schematic diagram of the system design
5. System Hardware Design
Figure 6 is showing the block diagram of the system hardware design, which can be
further divided into two parts: DSP and CPLD. The DSP controller and CPLD controller are
marked as the gray shaded area and the external circuit includes the minimum system of this
two controllers as well as the external interfaces. The hardware circuit diagram is drawn using
Protel99 SE.
5.1. DSP Subsampling Hardware Circuit
ISSN: 2302-4046 
Design on the Time-domain Airborne Electromagnetic Weak Signal Data... (Yong Guo)
410
Figure 7 shows the DSP component of the hardware circuit diagram. It mainly contains
a DSP minimum system circuit, a data memory expansion circuit, a level-shifting circuit, a LCD
circuit, a second sampling circuit and a data transmission circuit.
5.2. CPLD Floating Point Zoom Hardware Circuit
Floating-point amplification circuit is controlled by CPLD chip EPM7128 and the
controlling circuit block diagram is shown in Figure 8. It mainly contains a EPM7128 minimum
system circuit, a low-pass filter circuit, a pre-sampling circuit, a programmable amplifier circuit
and a FIFO (First Input First Output) memory circuit.
Figure 6. Block diagram of system hardware design
Figure 7. DSP component of hardware circuit diagram
 ISSN: 2302-4046 TELKOMNIKA
TELKOMNIKA Vol. 12, No. 1, January 2014: 406 – 414
411
Figure 8. Diagram of a CPLD floating point amplifier circuit
5.3. Physical Map of System Hardware
Figure 9 shows the physical map of the system, in which the floating point amplifier
circuit board is fixed onto the DSP subsampling circuit board.
Figure 9. The physical map of the system
6. System Software Design
6.1. The Design of Sampling Circuit Software
The design process of the system software is shown in Figure 10. Once the system is
turned on, the main program will initialize the DSP hardware system, including disabling the
watchdog, setting the system clock and the peripheral clock, turning off the interrupts and
peripheral interrupt, initializing the PIE control registers and enabling the PIE vector table. CPLD
controls the floating-point amplification and processes the pre-sampling of transient
electromagnetic signal. DSP will samples the signals again, processes the results and restores
the original signal before transmitting the final results to the host computer and LCD for display
purpose.
ISSN: 2302-4046 
Design on the Time-domain Airborne Electromagnetic Weak Signal Data... (Yong Guo)
412
Figure 10. Software design flow chart
6.2. The Design of Data Collection Software
In order to get the characteristic curve of the secondary field as shown in Figure 2, the
system also needs specialized data collection software to receive the data collected from the
slave machine. The collection software should be able to readand save data, playback the data
stored in the hard disk, display the data and collect the waveform simultaneously. The data
collection software on the host computer is written in LabVIEW. LabVIEW is a program
development environment developed by American National Instruments which uses the graphic
visualization language, G-language, for programming. LabVIEW is widely used in the control of
instrumentation, measurement, data processing and display areasError! Reference source not
found.. Figure 11 shows the interface of the data collection software.
Figure 11. Interface of the data collection software
 ISSN: 2302-4046 TELKOMNIKA
TELKOMNIKA Vol. 12, No. 1, January 2014: 406 – 414
413
7. Test Results
Figure 12 shows the decay curve of the transient electromagnetic secondary field signal
in system field testing. System uses a 25 Hz bipolar combination wave as the excitation source,
a sampling frequency of 100 kHz will collect data of 500 points in 5 ms. As indicated by the
acquisition curve, the induced electromotive force decays from the initial 500 mV to about 0 mV
in the end. The data acquisition system collects the approximated decay curve of the secondary
field signal, showing the attenuation of the secondary field information with time.
Figure 12. The attenuation curve of secondary field signal
8. Conclusion
In this paper, we made an in-depth study in the development of weak signal data
acquisition system based on DSP, on the basis of the efforts made in the transient
electromagnetic method by predecessors. The system increases the dynamic amplification
range to 144 dB using floating point amplifier technology, and it has a sampling rate of 100 kHz,
which meets the requirements for high sampling rate and precision. The field test proved that
the system was able to capture the weak transient electromagnetic signal. The research work
has some practical values and application prospect, and the system has been applied in the
time-domain fixed-wing airborne electromagnetic mineral exploration.
Acknowledgements
This work was supported by the Cultivating programme of Middle-aged backbone
teachers of Chendu university of technology, Cultivating programme of excellent innovation
team of Chendu university of technology, and "863" National High Technology Research and
Development Program (2006AA06A206) .
References
[1] Xiong Sheng Qing. The think about developing Chinese Aero Geophysical Survey Technology.
Chinese Geology. 2009; 36 (06): 1366.
[2] Dang RuiRong, Zhao WenTao, Ren ZhiPing. Transient receiving system based on floating point zoom
technology. Petroleum Instruments. 2010; 24(1): 76-77.
[3] Munkholm MS, Auken E. Electromagnetic noise contamination on Transient Electromagnetic sound-i-
ngs in culturally disturbed environments. Journal of Environment and Engineering Geophysics. 1996;
2(1).
[4] Wang Zhong, Huang Yue, Lin Jun. Development of high-speed and high dynamic range transient
electromagnetic receiver. Journal of Scientific Instrument. 2006; 27(04): 416.
[5] Meng Qing Min. Study on layered inversion and application of frequency domain airborne
electromagnetic method. BeiJing: China University of Geosciences; 2005.
[6] Li JunFeng, Liu Kai Fei, Liu Ying Ying. Primary magnetic automatic compensation technology of
frequency domain airborne electromagnetic system. Geophysical and Geochemical Exploration.
2009; 33(10): 536-540.
[7] Qin RuiJie, Li Wen Quan, Lin Jun. A novel instantaneous floating point amplifier. Air Measurement
Technology. 1997; (17): 27.
ISSN: 2302-4046 
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414
[8] Dong Han Chuan, Guo Yong, Li Wen Jie. The application of LabVIEW serial communication in data
acquisition. Microcomputer and Applications. 2011; 12(10): 63-64.
[9] Li Wen Jie, Meng Qing Min, Li Jun Feng. The review and prospect of frequency domain airborne
electromagnetic method Instrument System Development. Geophysical and Geochemical Exploration
of Computing Technology. 2007; 29(s1): 21-22.
[10] Li Fei, Meng Qing Min, Ding Zhi Qiang. Some important issues of Y-12 airborne geophysical
integrated station in the wild flight. Geology and Prospecting. 2011; 47(3): 423-425.
[11] Xue Guo Qiang, Li Xiu, Di Qing Yun. Research progress of forward and inverse problems for transient
electromagnetic method. Advances in Geophysics. 2008; 23(4): 1165.
[12] Jeffrey Travis, Jim Kring. LabVIEW University Practical Guide. BeiJing: Publishing House of
Electronics Industry. 2008.
[13] Li Wen Jie. Study of frequency domain airborne electromagnetic data processing technology. BeiJing:
China University of Geosciences; 2008.
[14] Li Jun Feng. Study of fixed-wing frequency domain airborne electromagnetic measurement system
technology. BeiJing: China University of Geosciences; 2009.
[15] Yuan Gui Qin, Xiong Sheng Qing, Meng QingMin. Research on geophysical exploration technology
and application. Geology Journal. 2011; (85): 1744-1748.
[16] Li Jin Ming. Geoelectric Field and Electrical Prospecting. BeiJing: Geological Publishing House. 2005.

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Design on the Time-domain Airborne Electromagnetic Weak Signal Data Acquisition System

  • 1. TELKOMNIKA Indonesian Journal of Electrical Engineering Vol.12, No.1, January 2014, pp. 406 ~ 414 DOI: http://dx.doi.org/10.11591/telkomnika.v12i1.4144  406 Received June 26, 2013; Revised August 27, 2013; Accepted September 19, 2013 Design on the Time-domain Airborne Electromagnetic Weak Signal Data Acquisition System Xiao-ling Zhong, Yong Guo*, Han-chuan Dong College of Information Science and Technology Chengdu University of Technology, Chengdu, China, 610059 *corresponding author, e-mail: guoy@cdut.edu.cn Abstract According to principle of transient electromagnetic method as well as its signal characteristics, this paper designed and implemented a time-domain airborne electromagnetic weak signal data acquisition system. With the use of the floating-point amplification technology, the system amplifies the weak transient electromagnetic signal dynamically. CPLD and DSP were used as the decoding control circuit and the main controller for processing the sampled data, respectively. The transient electromagnetic signal acquisition system, which was designed with a dynamic range up to 144dB and a sampling rate up to 100 kHz, meets the requirements of the high sampling rate with high precision and it has been applied in the time-domain fixed-wing airborne electromagnetic mineral exploration. Keywords: DSP, CPLD, ATEM, Floating-point Amplifier, Data Acquisition Copyright © 2014 Institute of Advanced Engineering and Science. All rights reserved. 1. Introduction At present, China is implementing land resources survey and geological security projects based on mineral development, and China is also making efforts to identify the status of land resources as soon as possible. During the Eleventh Five-Year Plan period, China has launched a research and development project for geological prospecting using high-precision airborne geophysical technology and equipment. The project, “Fixed-wing Time-domain Airborne Electromagnetic Exploration Systems Research and Development”, undertaken by IGGE,is an important topic in State High-Tech Development Plan (863 Program) project “Airborne Geophysical Exploration Technology Systems”. According to the principle of transient electromagnetic method, for the Time-domain Airborne Electromagnetic (ATEM) weak signal, this paper presents researches and designs of a data acquisition system based on DSP. The transient electromagnetic is a geophysical exploration method, with high sensitivity in resistivity change, fewer limitations in ground conditions, good probing depth. It is widely used in many areas, including as metal mineral exploration, drilling and aviation and marine activities.The time-domain airborne electromagnetic method, a branch of the airborne electromagnetic methods, combines aviation with geophysical technologyby using aircrafts as delivery platforms to load geophysical equipment and complete the data acquisition of geophysical information. Aero Geophysical Survey is one of the important means of completing national geological survey projects with deep exploration depth. Large area survey can be facilitated at low cost and high efficiency, which plays an important role in the national economy development Error! Reference source not found.. 2. ATEM System 2.1. Principle of Transient Electromagnetic Method The transient electromagnetic method, also known as Time-domain Electromagnetic Method (TEM), is based on fundamental electromagnetic induction principles shown in Figure 1. A transmitting coil is firstly put on the ground or in the air. By changing the current flowing throught, a constantly varying electromagnetic field (named as “primary field”) can be generated in the space surrounding the coil, producing an induced current in the rock and mineral beneath. The varying current induced will also produce a varying electrmagnetic field (named as “secondary field”) in the space around the ore body. The receiving coil is then used to obtain the
  • 2.  ISSN: 2302-4046 TELKOMNIKA TELKOMNIKA Vol. 12, No. 1, January 2014: 406 – 414 407 information of the secondary field, including resistivity, conductivity and other physical characteristics. Further analysis based on the information obtained will help us to investigate the distribution of the underground mine sources [2]. Figure 1. The schematic diagram showing the basic principles of the transient electromagnetic method In order to improve the sensitivity of resistivity characterisation, reduce the limitation of ground conditions, deepen the probing depth and get better synchronization between transmitters and receivers, the transient electromagnetic method has recently become one of the most important exploration method in geophysical exploration field. It has been rapidly applied in metal mineral exploration, water resource survey, environment protection, aviation and marine activities Error! Reference source not found.. 2.2. Characteristics of Transient Electromagnetic Signal In the electrical prospecting method, the intensity secondary field response of underground conductors decays exponentially with a decay function Error! Reference source not found.. The function is: e tK t   / )(e   (1) Where e(t) represents the intensity of the secondary field response of conductive body, K is a time-independent constant, t is the time elapsed, and  is a time constant dependent on the property of the conductive body. Figure 2 is showing the characteristic curve of the TEM signal and its features are as follows:
  • 3. ISSN: 2302-4046  Design on the Time-domain Airborne Electromagnetic Weak Signal Data... (Yong Guo) 408 Figure 2. Characteristic curve of the TEM signal (1) Large dynamic range: signal amplitude decays from n×105µV to n×10-1µV, up to 120db of dynamic range. (2) Wide band: The frequency range of the TEM signal collected in this topic is 20 Hz to 25 kHz. (3) Quick signal attenuation: Early TEM signals decay quicker and late signals decay slower. 2.3. ATEM System Airborne Time-domain Electromagnetic Method Airborne Time-domain Electromagnetic Method (ATEM) is an important branch of airborne electromagnetic method (AEM).Its development is based on traditional ground electromagnetic method with the implementation of aerial survey. Similar as the ground electromagnetic methods, ATEM has its unique advantages, including fast speed, low cost, high efficiency, deep probing depth and etc. Besides, its application can be extended to geophysical survey work in areas where terrestrial method cannot be applied due to complexity, including swamps, deserts, lakes, forests and residential areas. ATEM is an effective exploration method and it is essential for land resources survey Error! Reference source not found.. Figure 3 is showing schematic diagram of the frequency-domain airborne electromagnetic survey system platform developed by IGGE. The fundamental principle of the frequency-domain airborne electromagnetic method is the same as that of the time-domain method Error! Reference source not found.. The platform employs domestic Y12 IV aircrafts with transmiting and receiving coils installed at both ends of the fixed wings. Cabin equipment includes transmitters, receivers, aviation single-ray optically pumped magnetometer, aviation spectrometer, airborne geophysical data collection system as well as GPS navigation and positioning system. Figure 3. Schematic diagram of the frequency-domain airborne electromagnetic survey system ATEM can be used to investigate the magnetotelluric properties, such as conductivity, permeability and etc. As the working platform of AEM is the aircraft, the main technical features of the AEM system are related not only to the instrument itself, but also to the type of the aircraft and the unique modifications made upon the airplane (Man Yan-long, 2009). 3. Floating-Point Amplification Technology
  • 4.  ISSN: 2302-4046 TELKOMNIKA TELKOMNIKA Vol. 12, No. 1, January 2014: 406 – 414 409 Floating-point amplification means the input signal can be amplified with dynamical extent and devices based on the principle of floating-point amplification are called floating-point amplifiers. Figure 4 shows the schematic diagram of a floating-point amplifier which is composed of pre-sampling circuit, the second sampling circuit, programmable amplifying circuit and encoding circuit Error! Reference source not found.. Figure 4. Schematic diagram of a floating-point amplifier 4. System Design Program Figure 5 shows the overall system design program. The components enclosed in the dashed box is a floating-point amplifier circuit which is controlled by CPLD. Firstly, the TEM signal passes through the preamplifier and a low pass filter.Then CPLD will collect the raw signal with its internal coding circuit controlling the dynamic amplification. DSP then samples the signal again and transmits the results, which will also be displayed on the LCD, to the host computer. Figure 5. Schematic diagram of the system design 5. System Hardware Design Figure 6 is showing the block diagram of the system hardware design, which can be further divided into two parts: DSP and CPLD. The DSP controller and CPLD controller are marked as the gray shaded area and the external circuit includes the minimum system of this two controllers as well as the external interfaces. The hardware circuit diagram is drawn using Protel99 SE. 5.1. DSP Subsampling Hardware Circuit
  • 5. ISSN: 2302-4046  Design on the Time-domain Airborne Electromagnetic Weak Signal Data... (Yong Guo) 410 Figure 7 shows the DSP component of the hardware circuit diagram. It mainly contains a DSP minimum system circuit, a data memory expansion circuit, a level-shifting circuit, a LCD circuit, a second sampling circuit and a data transmission circuit. 5.2. CPLD Floating Point Zoom Hardware Circuit Floating-point amplification circuit is controlled by CPLD chip EPM7128 and the controlling circuit block diagram is shown in Figure 8. It mainly contains a EPM7128 minimum system circuit, a low-pass filter circuit, a pre-sampling circuit, a programmable amplifier circuit and a FIFO (First Input First Output) memory circuit. Figure 6. Block diagram of system hardware design Figure 7. DSP component of hardware circuit diagram
  • 6.  ISSN: 2302-4046 TELKOMNIKA TELKOMNIKA Vol. 12, No. 1, January 2014: 406 – 414 411 Figure 8. Diagram of a CPLD floating point amplifier circuit 5.3. Physical Map of System Hardware Figure 9 shows the physical map of the system, in which the floating point amplifier circuit board is fixed onto the DSP subsampling circuit board. Figure 9. The physical map of the system 6. System Software Design 6.1. The Design of Sampling Circuit Software The design process of the system software is shown in Figure 10. Once the system is turned on, the main program will initialize the DSP hardware system, including disabling the watchdog, setting the system clock and the peripheral clock, turning off the interrupts and peripheral interrupt, initializing the PIE control registers and enabling the PIE vector table. CPLD controls the floating-point amplification and processes the pre-sampling of transient electromagnetic signal. DSP will samples the signals again, processes the results and restores the original signal before transmitting the final results to the host computer and LCD for display purpose.
  • 7. ISSN: 2302-4046  Design on the Time-domain Airborne Electromagnetic Weak Signal Data... (Yong Guo) 412 Figure 10. Software design flow chart 6.2. The Design of Data Collection Software In order to get the characteristic curve of the secondary field as shown in Figure 2, the system also needs specialized data collection software to receive the data collected from the slave machine. The collection software should be able to readand save data, playback the data stored in the hard disk, display the data and collect the waveform simultaneously. The data collection software on the host computer is written in LabVIEW. LabVIEW is a program development environment developed by American National Instruments which uses the graphic visualization language, G-language, for programming. LabVIEW is widely used in the control of instrumentation, measurement, data processing and display areasError! Reference source not found.. Figure 11 shows the interface of the data collection software. Figure 11. Interface of the data collection software
  • 8.  ISSN: 2302-4046 TELKOMNIKA TELKOMNIKA Vol. 12, No. 1, January 2014: 406 – 414 413 7. Test Results Figure 12 shows the decay curve of the transient electromagnetic secondary field signal in system field testing. System uses a 25 Hz bipolar combination wave as the excitation source, a sampling frequency of 100 kHz will collect data of 500 points in 5 ms. As indicated by the acquisition curve, the induced electromotive force decays from the initial 500 mV to about 0 mV in the end. The data acquisition system collects the approximated decay curve of the secondary field signal, showing the attenuation of the secondary field information with time. Figure 12. The attenuation curve of secondary field signal 8. Conclusion In this paper, we made an in-depth study in the development of weak signal data acquisition system based on DSP, on the basis of the efforts made in the transient electromagnetic method by predecessors. The system increases the dynamic amplification range to 144 dB using floating point amplifier technology, and it has a sampling rate of 100 kHz, which meets the requirements for high sampling rate and precision. The field test proved that the system was able to capture the weak transient electromagnetic signal. The research work has some practical values and application prospect, and the system has been applied in the time-domain fixed-wing airborne electromagnetic mineral exploration. Acknowledgements This work was supported by the Cultivating programme of Middle-aged backbone teachers of Chendu university of technology, Cultivating programme of excellent innovation team of Chendu university of technology, and "863" National High Technology Research and Development Program (2006AA06A206) . References [1] Xiong Sheng Qing. The think about developing Chinese Aero Geophysical Survey Technology. Chinese Geology. 2009; 36 (06): 1366. [2] Dang RuiRong, Zhao WenTao, Ren ZhiPing. Transient receiving system based on floating point zoom technology. Petroleum Instruments. 2010; 24(1): 76-77. [3] Munkholm MS, Auken E. Electromagnetic noise contamination on Transient Electromagnetic sound-i- ngs in culturally disturbed environments. Journal of Environment and Engineering Geophysics. 1996; 2(1). [4] Wang Zhong, Huang Yue, Lin Jun. Development of high-speed and high dynamic range transient electromagnetic receiver. Journal of Scientific Instrument. 2006; 27(04): 416. [5] Meng Qing Min. Study on layered inversion and application of frequency domain airborne electromagnetic method. BeiJing: China University of Geosciences; 2005. [6] Li JunFeng, Liu Kai Fei, Liu Ying Ying. Primary magnetic automatic compensation technology of frequency domain airborne electromagnetic system. Geophysical and Geochemical Exploration. 2009; 33(10): 536-540. [7] Qin RuiJie, Li Wen Quan, Lin Jun. A novel instantaneous floating point amplifier. Air Measurement Technology. 1997; (17): 27.
  • 9. ISSN: 2302-4046  Design on the Time-domain Airborne Electromagnetic Weak Signal Data... (Yong Guo) 414 [8] Dong Han Chuan, Guo Yong, Li Wen Jie. The application of LabVIEW serial communication in data acquisition. Microcomputer and Applications. 2011; 12(10): 63-64. [9] Li Wen Jie, Meng Qing Min, Li Jun Feng. The review and prospect of frequency domain airborne electromagnetic method Instrument System Development. Geophysical and Geochemical Exploration of Computing Technology. 2007; 29(s1): 21-22. [10] Li Fei, Meng Qing Min, Ding Zhi Qiang. Some important issues of Y-12 airborne geophysical integrated station in the wild flight. Geology and Prospecting. 2011; 47(3): 423-425. [11] Xue Guo Qiang, Li Xiu, Di Qing Yun. Research progress of forward and inverse problems for transient electromagnetic method. Advances in Geophysics. 2008; 23(4): 1165. [12] Jeffrey Travis, Jim Kring. LabVIEW University Practical Guide. BeiJing: Publishing House of Electronics Industry. 2008. [13] Li Wen Jie. Study of frequency domain airborne electromagnetic data processing technology. BeiJing: China University of Geosciences; 2008. [14] Li Jun Feng. Study of fixed-wing frequency domain airborne electromagnetic measurement system technology. BeiJing: China University of Geosciences; 2009. [15] Yuan Gui Qin, Xiong Sheng Qing, Meng QingMin. Research on geophysical exploration technology and application. Geology Journal. 2011; (85): 1744-1748. [16] Li Jin Ming. Geoelectric Field and Electrical Prospecting. BeiJing: Geological Publishing House. 2005.