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<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0"><?xmltex \makeatother\@nolinetrue\makeatletter?>
  <front>
    <journal-meta><journal-id journal-id-type="publisher">GI</journal-id><journal-title-group>
    <journal-title>Geoscientific Instrumentation, Methods and Data Systems</journal-title>
    <abbrev-journal-title abbrev-type="publisher">GI</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Geosci. Instrum. Method. Data Syst.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2193-0864</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/gi-7-253-2018</article-id><title-group><article-title>Development of high-precision distributed wireless<?xmltex \hack{\break}?> microseismic acquisition
stations</article-title><alt-title>Development of high-precision distributed wireless microseismic acquisition
stations</alt-title>
      </title-group><?xmltex \runningtitle{Development of high-precision distributed wireless microseismic acquisition
stations}?><?xmltex \runningauthor{S.~Qiao et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Qiao</surname><given-names>Shuaiqing</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8981-0258</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Duan</surname><given-names>Hongmei</given-names></name>
          <email>duanhm@cugb.edu.cn</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zhang</surname><given-names>Qisheng</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6012-7308</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Zhang</surname><given-names>Qimao</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Li</surname><given-names>Shuhan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Liu</surname><given-names>Shenghui</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Liu</surname><given-names>Shiyang</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Wang</surname><given-names>Yongqing</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Yan</surname><given-names>Shichu</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Li</surname><given-names>Wenhao</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Guo</surname><given-names>Feng</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>School of Geophysics and Information Technology
(Beijing), China University of Geosciences, Beijing, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Institute of Electronics, Chinese Academy of Sciences, Beijing, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Hongmei Duan (duanhm@cugb.edu.cn)</corresp></author-notes><pub-date><day>27</day><month>September</month><year>2018</year></pub-date>
      
      <volume>7</volume>
      <issue>3</issue>
      <fpage>253</fpage><lpage>263</lpage>
      <history>
        <date date-type="received"><day>16</day><month>April</month><year>2018</year></date>
           <date date-type="rev-request"><day>14</day><month>June</month><year>2018</year></date>
           <date date-type="rev-recd"><day>23</day><month>August</month><year>2018</year></date>
           <date date-type="accepted"><day>27</day><month>August</month><year>2018</year></date>
      </history>
      <permissions>
        
        
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018.html">This article is available from https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018.html</self-uri><self-uri xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018.pdf">The full text article is available as a PDF file from https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018.pdf</self-uri>
      <abstract>
    <p id="d1e180">In recent years, owing to the shortage of oil and gas resources
and increasing difficulty in mining, traditional (wired) microseismic
monitoring equipment has been unable to meet the needs of energy
exploitation. Therefore, it is necessary to develop new high-precision
seismic exploration and data acquisition systems. In this study, we combined
advanced acquisition systems with wireless technology to develop a new
wireless microseismic acquisition system. The hardware circuit of the
acquisition system mainly includes a data acquisition board and a main
control board. High-precision analog-to-digital conversion and digital
filtering technologies are used to provide data with high signal-to-noise
ratios, resolution, and fidelity to the acquisition stations. Key
technologies were integrated into the ARM (Advanced RISC Machines)
of the main control board: reliable
GPS technology was employed to realize synchronous acquisitions among various
acquisition stations, and WIFI technology was used to achieve wireless data
communication between acquisition stations and the central station, thus
improving the data transmission speed and accuracy. After conducting a series
of evaluation tests, it was found that the system was stable, convenient to
use, and had high data accuracy, therefore providing significant support for
the solution to problems encountered in current oil and gas exploration
processes, such as the complicated environment and inconvenient construction.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \hack{\newpage}?>
<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e192">From a global view point, 50 % dependence on imported petroleum can be
regarded as a economic security warning. However, in 2017, China's foreign dependence
exceeded 67.4 %, which poses a threat to the energy and economic security
of the country (Mazza et al., 2012; CNPC Research Institute of Economics and
Technology, 2017). Therefore, the exploration of domestic oil and gas
resources in China should be enhanced to contribute to the stability and
sustainable development of the country, and also to build a more prosperous
society (Wood and Gettrust, 2002). With the development of oil and gas
exploration technologies, China has entered the difficult stage of oil and
gas exploration, namely the exploration of the pre-Cenozoic marine residual
basin (Wu et al., 2011). This involves the search for oil and gas resources
in complex geological areas, such as buried hills and their internal
structures, and geological formations on high and steep hillsides. In addition
to the increase in depth of detection, surface and underground conditions
will become more complex. Consequently, there will be new requirements and
challenges for seismographs, therefore resulting in an urgent need to develop
a novel high-accuracy seismic data acquisition system suitable for China's
conditions (Li and Liu, 2013). In recent years, as the country has placed
more emphasis on the research and development of geophysical instruments, the
number of research units engaged in studies on seismic data acquisition and
recording systems has continuously increased.</p>
      <p id="d1e195">The most powerful and widely used geophysical method for oil and gas
exploration is reflection seismology (Morandi and Ceragioli, 2002). As the
main equipment for seismic<?pagebreak page254?> exploration, the acquisition station is the core
of resource exploration and energy acquisition, with the collection of raw
data with high signal-to-noise ratio (SNR), resolution, and fidelity being the
most crucial aspects (Mazza et al., 2012; Mrmureanu and Ionescu, 2011). A
distributed wireless microseismic acquisition station preprocesses and
amplifies the analog signals collected by the detector and converts them into
digital signals with a strong anti-interference ability. The development of
seismic instruments has relied heavily on the continuous development of
seismic data acquisition methods. Since the advent of digital computers over
half a century ago, people have increasingly emphasized the use of numbers to
accurately quantify various physical quantities and to transfer information.
As a result, digital technologies have been developed in many fields, thus
driving the rapid development of microelectronics and computer technologies.
Digitization has been proposed in geophysical exploration since the 1960s,
with digital seismographs being one of the first examples (Guo and Liu,
2009). A renowned electronic device manufacturer in the USA, Texas
Instruments (TI), developed the DFSIV and DFSV digital seismographs. The
French manufacturer SERCEL also introduced the SN328 and SN338 digital
seismographs, which used seven-stage instantaneous floating-point amplifiers
(Huang and Yu, 1994).</p>
      <p id="d1e198">The design concept of the centralized instruments DFSV and SN338 limited the
increase in channel numbers, and the traveling distances of the seismic wave analog
signals sensed by the detectors along the bulky common depth point (CDP)
cables were also too long, exceeding 3 km in some cases. In addition, the
distance of signal transmission along the cable varied among different
channels, and the signals were severely adulterated by induction (Huang and
Yu, 1994). The SN388, 408UL, 428XL, and 508XT systems subsequently introduced
by SERCEL offered enhanced processing power, integration level, and stability,
but still had shortcomings in terms of gain, cost, and human–machine
interaction (Liu, 2015).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p id="d1e203">Structural block diagram of the hybrid acquisition system based on
the ADS1274 high-precision seismic electrical method.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f01.png"/>

      </fig>

      <p id="d1e213">With the dramatic increase in the number of seismic acquisition channels and
exploration in remote regions, the production efficiency of cable systems has
been reduced. In regions that are difficult to access and where the
environment is vulnerable, cable systems should be supplemented or replaced
by wireless systems. At present, the goal of seismograph research and
development is to establish high-resolution, high-precision, and synchronous data
acquisition, as well as real-time, high-speed, and low-power data transmission
(Zhang et al., 2013). Therefore, the development of a new wireless microseismic
digital acquisition system on the basis of traditional seismic instruments is
of great significance.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p id="d1e218">Operational block diagram of the single channel of the acquisition
board.</p></caption>
        <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f02.png"/>

      </fig>

</sec>
<sec id="Ch1.S2">
  <title>Hardware circuit</title>
<sec id="Ch1.S2.SS1">
  <title>Acquisition circuit design</title>
      <p id="d1e238">The acquisition board is the front-end circuit of the main control board and
is responsible for processing the analog electrical signals collected by
detectors (or electrodes) and converting them into digital signals to be
processed. Figure 1 shows the structural block diagram of the simulation
board of the acquisition station.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p id="d1e243">Schematic of the single channel of the acquisition board.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f03.png"/>

        </fig>

      <p id="d1e252">The front end of the three channels of the ADS1274 analog-to-digital
converter (ADC) is connected to a three-component seismometer, and can
simultaneously acquire the <inline-formula><mml:math id="M1" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M2" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M3" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> components of the seismic wave.
Three analog signals (the seismic wave signal in the <inline-formula><mml:math id="M4" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M5" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M6" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula>
directions) input by the detector are first filtered and
denoised by the front-end conditioning circuit. Next, the signals are
amplified by the programmable amplifier and further filtered by a
single-ended differential circuit. They are then converted into a
differential signal, input to the ADS1274 for analog-to-digital (AD)
conversion, and finally passed to the field programmable gate array (FPGA)
circuit for digital filtering.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p id="d1e301">Block diagram of the hardware design for the main control circuit
of the wireless microseismic acquisition station.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f04.png"/>

        </fig>

      <p id="d1e310">The front end of the other channel of the ADS1274 is connected to an
electrode (or magnetic bar). The analog signal input by the electrode is
amplified by a preamplifier circuit and passes through a filter to eliminate
unwanted signals in order to improve the SNR. The filtered analog input
signal is<?pagebreak page255?> further amplified by the main amplifier circuit, which is
controlled by the FPGA, and passes through the ADS1274 to be converted into
a digital signal. The digital signal is then fed to the FPGA for
digitalization.</p>
      <p id="d1e313">Figure 2 shows the operational block diagram of the single channel of the
acquisition board design. The AD conversion chip used in this design is the
24 bit ADS1274 manufactured by TI. The chip has four acquisition channels
that can acquire data simultaneously. The first three channels are used to
collect seismic signals in three directions (<inline-formula><mml:math id="M7" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M8" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M9" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> components),
while the fourth channel is used to acquire electrical
signals. The processing steps are similar for the four analog channels.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p id="d1e339">Overall software architecture diagram.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f05.png"/>

        </fig>

      <p id="d1e348">Figure 3 is the schematic diagram of the single channel of the acquisition
board. The signal first enters the acquisition board through the input
protection and impedance-matching circuit. The front-end conditioning circuit
preprocesses the analog signal to reduce waveform distortion, and the
preprocessed signal is filtered using a low-pass filter to remove the
high-frequency clutter signals brought in from the detector. The filtered
signal is then subsequently amplified. In this design, a programmable gain
amplifier AD8253 is used. Through the IO port, the CPU can control its gain
to 0, 20, 40, or 60 dB so that the gain can be controlled according to the
input signal size in order to achieve a higher resolution for the acquisition
board. The amplified signal passes through the AD driver chip so that the
single-ended signal is converted into a differential signal (that is, the
input to the ADS1274 is a differential signal). The differential signal is
then input to the ADS1274 for AD conversion, and the digital signal is
output by the AD chip.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p id="d1e354">Schematic of a distributed wireless acquisition system.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f06.png"/>

        </fig>

      <p id="d1e363">The calibration signal in the schematic diagram is generated by an analog
switch chip. The IO port of the FPGA can control the switching frequency of
the chip to generate square waves with different frequencies, which can be
used to perform self-testing on the acquisition system. The reference voltage
module REF5025 generates a 2.5 V standard reference voltage for the AD chip.
The clock of the AD chip (CLK) is generated from the FPGA module on the main
control board.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p id="d1e368">Communication and interaction process of the wireless network.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f07.png"/>

        </fig>

</sec>
<?pagebreak page256?><sec id="Ch1.S2.SS2">
  <title>Acquisition station master control circuit design</title>
      <p id="d1e383">Figure 4 is a diagram of the hardware design for the main control circuit of
the wireless microseismic acquisition station. The embedded control software
in the seismic data acquisition system runs on the main control circuit,
which is the core of the distributed wireless microseismic acquisition
station. The OMAP3730 processor and the Linux 2.6.37 operating system are
adopted in the core control processor. OMAP3730 is a dual-core processor
integrating ARM (Advanced RISC Machines) and DSP (digital signal processing)
processors, and can perform signal acquisition control and real-time data
storage. The embedded operating system Linux 2.6.37 runs on the processor and
is responsible for task scheduling. A high-speed memory management controller
chip is used as the data storage medium, while power-up management, power
supply management, LED driving, and keypad management are performed through
the general-purpose input/output (GPIO) port of the OMAP3730 processor. The
FPGA section is used to accomplish multiple tasks that cannot be performed by
general-purpose processors; these are (1) control of scheduling and execution
of all time-related tasks, including the generation of the sampling and
real-time clocks, scheduling of related strategies, etc.; (2) acquisition and
control of voltage, current, temperature, and other sensor data;
(3) acquisition system control and data<?pagebreak page257?> buffering; (4) wired data
communication; and (5) decoding and time synchronization of GPS information.</p>
      <p id="d1e386">The main control board is the core control processing unit of the
acquisition station. The design combines the high-performance
industrial-grade control system board OMAP3730 and the XC3S2000 FPGA to
achieve the following functions.
<list list-type="order"><list-item>
      <p id="d1e391">system monitoring function: monitoring of power supply voltage, electric
current, system temperature, and other boards</p></list-item><list-item>
      <p id="d1e395">communication management: USB and serial communications</p></list-item><list-item>
      <p id="d1e399">data storage function: storage in SDHC card</p></list-item><list-item>
      <p id="d1e403">acquisition system control and configuration, and data processing
functions</p></list-item><list-item>
      <p id="d1e407">time scheduling management functions: synchronization of real-time clock
and GPS time, with FPGA being responsible for time-based scheduling control
management</p></list-item><list-item>
      <p id="d1e411">control of human–computer interaction board</p></list-item><list-item>
      <p id="d1e415">storage status indication function</p></list-item><list-item>
      <p id="d1e419">communication status indication function</p></list-item><list-item>
      <p id="d1e423">data preprocessing function</p></list-item><list-item>
      <p id="d1e427">other auxiliary functions</p></list-item></list></p>
      <p id="d1e430">The OMAP3730 core control system board circuit integrates the general-purpose
memory controller (GPMC) bus, SD card, serial communication, USB, GPIO, and
other functional interfaces to simplify the system design. As one USB
interface integrated in the OMAP3730 core control system cannot meet the
system implementation requirements, we decided to expand the USB interface to
communicate with the WIFI module. A high-speed USB 2.0 PHY chip, USB 3320,
was used, and the industrial-grade SDIO (secure digital input and output)
wireless module RS9110 was used for the WIFI module. RS9110 is a WIFI module
that supports 802.11n b g<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and has high-performance wireless
transmission capabilities. The clock module provides the acquisition system
with accurate clock frequencies, GPS, and other information. The clock module
communicates with the master-control FPGA through UART (universal
asynchronous receiver/transmitter) and SPI (serial peripheral interface). The
master-control FPGA reads the GPS status information through UART and
calculates and adjusts the digital-to-analog output voltage through the
continuous count of pulses per second (PPS), so that the frequency of the
constant-temperature crystal oscillator is more accurate.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><caption><p id="d1e447">Equivalent input noise waveform of the acquisition board.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f08.png"/>

        </fig>

<?xmltex \hack{\newpage}?>
</sec>
</sec>
<?pagebreak page258?><sec id="Ch1.S3">
  <title>Overall design of the software</title>
<sec id="Ch1.S3.SS1">
  <title>Summary of software requirement</title>
      <p id="d1e470">The software designed in this study adopts the traditional software
development life cycle method, and also the top-down and stepwise refinement
structural software design approach.</p>
      <p id="d1e473">The main functions to be achieved by the software are as follows:
disk management, equipment calibration, CRC data verification, data
acquisition and storage, real-time data transmission over the network,
peripheral acquisition equipment management, GPS information analysis,
keypad management, LED status management, wireless network configuration,
and large-line network management.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Software architecture of the distributed wireless microseismic
acquisition station</title>
      <p id="d1e482">The embedded control software runs on the Linux 2.6.37 system platform. The
primary library of the system provides a basic platform for device hardware
control functions. Regardless of whether the users are in threads or
processes, any user can directly call the system-related interface functions
to perform the corresponding tasks. The primary library mainly includes the
following: time management interfaces, device management interfaces, disk
management interfaces, wireless network management interfaces, network
management interfaces, upgrade interfaces, and serial port management
interfaces. System calls are an important part of the system and depend on
the underlying operating system and the GNU C Library.</p>
      <p id="d1e485">The core business layer consists of five submodules and a main task as shown
in Fig. 5, with each component being a separate thread.
<list list-type="order"><list-item>
      <p id="d1e490">main thread: responsible for the data acquisition, instrument
calibration, and data deletion processes;</p></list-item><list-item>
      <p id="d1e494">system status thread: responsible for monitoring the system status,
including disk capacity, voltage, current, temperature, synchronization
status, etc., and handling of response status;</p></list-item><list-item>
      <p id="d1e498">GPS decoding thread: responsible for decoding GPS information;</p></list-item><list-item>
      <p id="d1e502">network communication thread: includes communication with notebooks
through wireless network management and communication with large-line
transmission systems through large-line network management;</p></list-item><list-item>
      <p id="d1e506">key event management thread: receives the user's key operations and takes
corresponding action according to the operations;</p></list-item><list-item>
      <p id="d1e510">LED lamp management thread: indicates the current status of the system
through different statuses of the LED lamp.</p></list-item></list></p>
      <p id="d1e513">The core communication interface module is an interface for communication
between different threads to establish a message communication mechanism
among threads.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p id="d1e518">Harmonic distortion test chart.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f09.png"/>

        </fig>

      <p id="d1e528">Under the core business layer, the system management module for the
electromagnetic data acquisition system mainly includes a time management
module, a device driver module, a disk management module, wireless network
configuration, and serial port configuration.</p>
</sec>
</sec>
<?pagebreak page259?><sec id="Ch1.S4">
  <title>Wireless microseismic acquisition station communication</title>
      <p id="d1e539">The field work mode of the distributed wireless acquisition system is shown
in Fig. 6. A relay access point (AP) is placed in a certain area as a relay
point to connect with a certain number of wireless seismic acquisition
stations for wireless data transmission. Multiple relay APs are used to cover
all wireless acquisition stations in the construction area. The central
station AP connects with each relay AP through the omnidirectional coverage
antenna to issue commands and collect real-time data.</p>
      <p id="d1e542">The communication and interaction process of the wireless network is shown in
Fig. 7.</p>
</sec>
<sec id="Ch1.S5">
  <title>Acquisition station performance test</title>
<sec id="Ch1.S5.SS1">
  <title>Noise test</title>
      <p id="d1e556">The equivalent input noise refers to the output of the seismic acquisition
station when the input end of the station is connected to the standard
resistance. The measurement result is converted into the root mean square
(RMS) voltage value, usually expressed in microvolts. The equivalent input
noise is mainly composed of ADC quantization noise and the thermal noise of
the components, and is directly superimposed on the input seismic signal
during operation. Therefore, it determines the capability of the instrument
to distinguish weak signals, wherein lower equivalent input noise is more
desirable.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><caption><p id="d1e562">Equivalent input noise test results.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Preamplifier</oasis:entry>
         <oasis:entry colname="col2">Equivalent input</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">gain</oasis:entry>
         <oasis:entry colname="col2">noise (<inline-formula><mml:math id="M11" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>V)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">6.06</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">0.91</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">0.51</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1000</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">0.30</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?pagebreak page260?><p id="d1e673">When the equivalent input noise is tested, the analog signal input terminal
must be connected with a terminal test resistor. In the present design, a
resistor of 1 k<inline-formula><mml:math id="M16" display="inline"><mml:mi mathvariant="normal">Ω</mml:mi></mml:math></inline-formula> resistance was used. During the test, the sampling
rate of the ADS1274 was set to 1000 SPS (samples per second), and data corresponding to preamp
gains of <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1000</mml:mn></mml:mrow></mml:math></inline-formula> were
respectively collected. Data from 8192 sample points were collected for
processing and analysis.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><caption><p id="d1e726">Test chart of the acquisition station synchronization.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gi.copernicus.org/articles/7/253/2018/gi-7-253-2018-f10.png"/>

        </fig>

      <p id="d1e735">The calculation method in the equivalent input noise test is as follows.
First, the average value of amplitude <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M22" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> samples was calculated
using Eq. (1) to obtain the DC offset (dc) of the noise signal.
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M23" display="block"><mml:mrow><mml:mi mathvariant="normal">dc</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>N</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover><mml:msub><mml:mi>X</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e788">Next, the RMS after drift removal, which is the equivalent input noise of
the instrument, was then calculated as
            <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M24" display="block"><mml:mrow><mml:mi mathvariant="normal">RMS</mml:mi><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>N</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi mathvariant="normal">dc</mml:mi></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e836">Then, by analyzing the data of 8192 sampling points, the equivalent input
noise waveform was plotted, as shown in Fig. 8.</p>
      <p id="d1e839">Table 1 presents the equivalent noise output results of the preprogrammed
amplifier with different gains. According to the obtained results from the
processed data, it can be seen that when the amplification of the
programmable amplifier was 40 dB, the equivalent input noise of the
acquisition station was 0.51 <inline-formula><mml:math id="M25" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>V (approximately
0.5 <inline-formula><mml:math id="M26" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>V). Therefore, it can be concluded that the acquisition
accuracy of the acquisition station satisfied the expected requirements.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <title>Harmonic distortion test</title>
      <p id="d1e862">Harmonic distortion refers to the nonlinear distortion of the output of a
seismic instrument when a sinusoidal signal is inputted. It is usually
measured by the ratio of the amplitude of each harmonic component to the RMS
of the fundamental signal amplitude. The harmonic distortion of the
seismograph reflects the fidelity of the seismic instrument in the
acquisition and recording of seismic signals. This indicator is closely
related to the noise and instantaneous dynamic range of the instrument. If
the harmonic distortion of the instrument is excessively large, each
harmonic component of the seismic signal will be converted into noise, thus
reducing the dynamic range of the system. At the same time, if the harmonic
distortion of the instrument is excessively large, the high-order harmonics
generated by the low-frequency surface waves with strong amplitude are
likely to be mixed into the frequency band of the low-amplitude effective
signal, thereby causing interference. The harmonic distortion of seismic
instruments is therefore an important performance indicator.</p>
      <?pagebreak page261?><p id="d1e865"><?xmltex \hack{\newpage}?>Discrete Fourier transform (DFT) of length <inline-formula><mml:math id="M27" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> was performed on the signal
sequence <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mi>x</mml:mi><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> to obtain the discrete frequency spectrum <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mi>X</mml:mi><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, and to find
the maximum spectral magnitude point <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mi>X</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>|</mml:mo></mml:mrow></mml:math></inline-formula>. The corresponding discrete
frequency point <inline-formula><mml:math id="M31" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> in the spectrum diagram is the corresponding frequency
point of the fundamental wave. Assuming that each harmonic amplitude is
<inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the harmonic distortion (THD) was computed using Eq. (3), and the
fifth harmonic was obtained in the actual calculation.
            <disp-formula id="Ch1.E3" content-type="numbered"><mml:math id="M33" display="block"><mml:mrow><mml:mi mathvariant="normal">THD</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">20</mml:mn><mml:mo>×</mml:mo><mml:mi>l</mml:mi><mml:mi>g</mml:mi><mml:mfenced open="(" close=")"><mml:msqrt><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>A</mml:mi><mml:mn mathvariant="normal">3</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>A</mml:mi><mml:mn mathvariant="normal">4</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>+</mml:mo><mml:msubsup><mml:mi>A</mml:mi><mml:mi>N</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:msqrt></mml:mfenced></mml:mrow></mml:math></disp-formula>
          When the data length is a non-integer multiple of the period of the sine
wave, the energy of the fundamental wave and the harmonic wave will leak
into the adjacent frequency band, thus resulting in spectral leakage. In the
actual calculation of harmonic distortion, direct use of DFT for spectral
analysis often causes frequency spectrum leakage, so that the calculated
spectrum does not accurately reflect the frequency characteristics of the
signal. Therefore, it is usually necessary to perform window processing on
the measured signal, with a minimum energy window being most optimum.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p id="d1e1013">Acquisition station performance index comparison results.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Indicator</oasis:entry>
         <oasis:entry colname="col2">High-precision distributed wireless</oasis:entry>
         <oasis:entry colname="col3">SMARTSOLO</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">microseismic acquisition stations</oasis:entry>
         <oasis:entry colname="col3"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">ADC resolution</oasis:entry>
         <oasis:entry colname="col2">24 bits</oasis:entry>
         <oasis:entry colname="col3">24 bits</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Equivalent input noise</oasis:entry>
         <oasis:entry colname="col2">0.91 <inline-formula><mml:math id="M34" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>V@20 dB (RMS)</oasis:entry>
         <oasis:entry colname="col3">1.23 <inline-formula><mml:math id="M35" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>V@12 dB (RMS)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Channels</oasis:entry>
         <oasis:entry colname="col2">4 (three seismic channels,</oasis:entry>
         <oasis:entry colname="col3">1 (only one seismic channel)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">one electrical channel)</oasis:entry>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Data transmission</oasis:entry>
         <oasis:entry colname="col2">storage in SD card <inline-formula><mml:math id="M36" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">storage in SD card</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">wireless transmission</oasis:entry>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Maximum input signal</oasis:entry>
         <oasis:entry colname="col2">2.5 peak@0 dB</oasis:entry>
         <oasis:entry colname="col3">2.5 peak@0 dB</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Timing accuracy</oasis:entry>
         <oasis:entry colname="col2">&lt; 100 ns, GPS disciplined</oasis:entry>
         <oasis:entry colname="col3">&lt; 20 <inline-formula><mml:math id="M37" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>s, GPS disciplined</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e1193">The test result is shown in Fig. 9.</p>
</sec>
<sec id="Ch1.S5.SS3">
  <title>Synchronization test of acquisition stations</title>
      <p id="d1e1202">In seismic exploration experiments, the precise collection of seismic wave
signals and the recording of their corresponding travel time are extremely
important. This requires data to be acquired synchronously by each sensor
(Mougenot, 2013).</p>
      <p id="d1e1205">In the present design, GPS technology is the key to accomplishing synchronous
acquisition. The LEA-6T timing receiver, which can output PPS signals with a
precision of up to 15 ns, has been adopted in this design. At the same time,
it has dedicated frequency and PPS output pins, with a precision as high as
10<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p>
      <p id="d1e1220">During the test, acquisition was conducted on 32 acquisition stations
simultaneously. Figure 10 shows the acquisition<?pagebreak page262?> of 32 stations under the same
seismic source. As seen from the figure, when vibrations were emitted from
the source, the entire 32 acquisition stations collected data almost
simultaneously, which indicates good synchronization performance between
them. After the actual measurement and calculation, the synchronization
accuracy of the acquisition station is measured to reach 100 ns.</p>
</sec>
<sec id="Ch1.S5.SS4">
  <title>Acquisition station performance comparison</title>
      <p id="d1e1229">After the performance test of the acquisition station was completed, the
wireless microseismic acquisition station was compared with a new type of
seismic acquisition station on the market. The selected acquisition station
was the intelligent acquisition station displayed by the Italian
DTCC/SmartSolo<sup>®</sup> at CPS/SEG 2018 in Beijing,
24–27 April. Six aspects including equivalent input noise, timing
accuracy, and data transmission were compared. These reflect the superiority of
high-precision distributed wireless microseismic acquisition stations in some
aspects. Table 2 shows the specific performance comparison results.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e1242">In this study, a high-precision distributed wireless microseismic acquisition
system has been designed for oil and gas exploration. The system design,
which was based on the ADS1274 chip manufactured by TI, made full use of the
four channels of the chip to collect vibration signals in three directions
and one electrical signal. Furthermore, the acquisition system
uses GPS and WIFI technologies to achieve distributed wireless acquisition.
After single-station testing and multi-station joint testing of the
acquisition stations, the results show that the system's performance in
equivalent noise, harmonic distortion testing, and synchronous acquisition
was able to meet the expected requirements. As such, the acquisition system
is currently being practically applied in production operations.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability">

      <p id="d1e1249">There are no publicly available data for this study.</p>
  </notes><notes notes-type="authorcontribution">

      <p id="d1e1255">The author worked as the hardware design and post-debugging throughout the development process, as well as the drafting of the manuscript.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e1261">The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1267">This work was supported by the Natural Science Foundation of China
(no. 41574131), the National Key Research and Development Program of China
(no. 2017YFF0105704), the National “863” Program of China (no. 2012AA06110203),
and the Fundamental Research Funds for the Central
Universities of China.
<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by:  Lev Eppelbaum<?xmltex \hack{\newline}?>
Reviewed by: Chen Guangyuan and one anonymous referee</p></ack><ref-list>
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    <!--<article-title-html>Development of high-precision distributed wireless microseismic acquisition stations</article-title-html>
<abstract-html><p>In recent years, owing to the shortage of oil and gas resources
and increasing difficulty in mining, traditional (wired) microseismic
monitoring equipment has been unable to meet the needs of energy
exploitation. Therefore, it is necessary to develop new high-precision
seismic exploration and data acquisition systems. In this study, we combined
advanced acquisition systems with wireless technology to develop a new
wireless microseismic acquisition system. The hardware circuit of the
acquisition system mainly includes a data acquisition board and a main
control board. High-precision analog-to-digital conversion and digital
filtering technologies are used to provide data with high signal-to-noise
ratios, resolution, and fidelity to the acquisition stations. Key
technologies were integrated into the ARM (Advanced RISC Machines)
of the main control board: reliable
GPS technology was employed to realize synchronous acquisitions among various
acquisition stations, and WIFI technology was used to achieve wireless data
communication between acquisition stations and the central station, thus
improving the data transmission speed and accuracy. After conducting a series
of evaluation tests, it was found that the system was stable, convenient to
use, and had high data accuracy, therefore providing significant support for
the solution to problems encountered in current oil and gas exploration
processes, such as the complicated environment and inconvenient construction.</p></abstract-html>
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