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<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" article-type="research-article" dtd-version="1.4" xml:lang="en">
  <front>
    <journal-meta>
      <journal-id journal-id-type="publisher-id">jtts</journal-id>
      <journal-title-group>
        <journal-title>Journal of Transportation Technologies</journal-title>
      </journal-title-group>
      <issn pub-type="epub">2160-0481</issn>
      <issn pub-type="ppub">2160-0473</issn>
      <publisher>
        <publisher-name>Scientific Research Publishing</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.4236/jtts.2026.161003</article-id>
      <article-id pub-id-type="publisher-id">jtts-147831</article-id>
      <article-categories>
        <subj-group>
          <subject>Article</subject>
        </subj-group>
        <subj-group>
          <subject>Engineering</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>Development of a Platform for Real-Time, Non-Disruptive Monitoring and Early Fault Detection of Critical High Voltage Transformers and Switchgears in High Speed-Rail</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Zhu</surname>
            <given-names>Ming</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Fan</surname>
            <given-names>Jiawei</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Jiang</surname>
            <given-names>Yingtao</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Teng</surname>
            <given-names>Hualiang</given-names>
          </name>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
      </contrib-group>
      <aff id="aff1"><label>1</label> Department of Electrical and Computer Engineering, University of Nevada Las Vegas, Las Vegas, USA </aff>
      <aff id="aff2"><label>2</label> Department of Civil and Environmental Engineering and Construction, University of Nevada Las Vegas, Las Vegas, USA </aff>
      <author-notes>
        <fn fn-type="conflict" id="fn-conflict">
          <p>The authors declare no conflicts of interest regarding the publication of this paper.</p>
        </fn>
      </author-notes>
      <pub-date pub-type="epub">
        <day>26</day>
        <month>11</month>
        <year>2025</year>
      </pub-date>
      <pub-date pub-type="collection">
        <month>11</month>
        <year>2025</year>
      </pub-date>
      <volume>16</volume>
      <issue>01</issue>
      <fpage>38</fpage>
      <lpage>53</lpage>
      <history>
        <date date-type="received">
          <day>08</day>
          <month>10</month>
          <year>2025</year>
        </date>
        <date date-type="accepted">
          <day>05</day>
          <month>12</month>
          <year>2025</year>
        </date>
        <date date-type="published">
          <day>08</day>
          <month>12</month>
          <year>2025</year>
        </date>
      </history>
      <permissions>
        <copyright-statement>© 2026 by the authors and Scientific Research Publishing Inc.</copyright-statement>
        <copyright-year>2026</copyright-year>
        <license license-type="open-access">
          <license-p> This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license ( <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 content-type="doi" xlink:href="https://doi.org/10.4236/jtts.2026.161003">https://doi.org/10.4236/jtts.2026.161003</self-uri>
      <abstract>
        <p>Partial discharge (PD) incidents in high-speed rail systems, such as transformers and switchgears, arise from insulation defects under electric stress, leading to potential flashovers, breakdowns, downtime, and safety risks. PD emits radio frequency (RF) signals, enabling the development of a non-invasive, real-time PD detection and monitoring platform. This system uses an RF antenna and a high-speed data acquisition system to scan a frequency range (100 MHz to 2.5 GHz) with intermediate frequency modulation for precise detection and analysis. PD events exceeding a preset power threshold are recorded, capturing both signal data and spectrum snapshots. Real-time data is streamed to a cloud server, accessible via a smartphone app, allowing remote monitoring and quick responses by maintenance teams. Laboratory tests confirm the system’s effectiveness in accurately capturing PD signals, enhancing high-speed rail infrastructure reliability and safety.</p>
      </abstract>
      <kwd-group kwd-group-type="author-generated" xml:lang="en">
        <kwd>Partial Discharge</kwd>
        <kwd>Real-Time Monitoring</kwd>
        <kwd>Robust Detection</kwd>
        <kwd>Radio Frequency</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
      <title>1. Introduction</title>
      <p>High-speed rail (HSR) has revolutionized transportation since 1960 by providing rapid, efficient, and reliable services that connect major cities and regions [<xref ref-type="bibr" rid="B1">1</xref>]. Extensive HSR networks have been developed in numerous countries, including Japan, France, Germany, China [<xref ref-type="bibr" rid="B2">2</xref>], and the undergoing California High-Speed Rail (CAHSR) project from Sacramento/San Francisco Bay Area to the Greater Los Angeles/San Deigo [<xref ref-type="bibr" rid="B3">3</xref>], showcasing significant advancements in speed, safety, and passenger comfort.</p>
      <p>The efficient and reliable operation of high-speed rail systems relies heavily on sophisticated high-voltage electrical facilities, such as transformers and switchgears, to ensure the seamless transmission and distribution of electrical power for train operations [<xref ref-type="bibr" rid="B4">4</xref>]-[<xref ref-type="bibr" rid="B6">6</xref>]. However, these high-voltage assets are susceptible to partial discharge (PD), which occurs when the electric field intensity exceeds the dielectric strength of the insulating material, causing localized discharges that do not completely bridge the insulation. These discharges typically result from defects such as voids, cracks, or contaminants within the insulation, which can arise during manufacturing, installation, or due to aging and environmental factors [<xref ref-type="bibr" rid="B7">7</xref>]. The occurrence of PD in high-voltage transformers and switchgears can have severe consequences, such as generating heat and chemical byproducts that degrade the insulating material over time. This degradation leads to erosion, cracks and carbonization, progressively weakening the insulation’s ability to withstand high voltages (<xref ref-type="fig" rid="fig1">Figure 1</xref>). Such phenomenon may significantly undermine the performance and longevity of transformers and switchgears, resulting in costly repairs, down time and/or fire hazards [<xref ref-type="bibr" rid="B8">8</xref>][<xref ref-type="bibr" rid="B9">9</xref>]. According to the research [<xref ref-type="bibr" rid="B10">10</xref>][<xref ref-type="bibr" rid="B11">11</xref>], 85% of high-voltage facility failures and asset damages are due to the PD activities (<xref ref-type="fig" rid="fig2">Figure 2</xref>).</p>
      <fig id="fig1">
        <label>Figure 1</label>
        <graphic xlink:href="https://html.scirp.org/file/3501028-rId13.jpeg?20251208015047" />
      </fig>
      <p><bold>Figure 1</bold><bold>.</bold> Causes of PD in switchgears and transformers.</p>
      <p>To mitigate the risks associated with PD, it is crucial to implement effective monitoring and maintenance strategies. There are multiple approaches to detect PD, such as electromagnetic method [<xref ref-type="bibr" rid="B12">12</xref>]-[<xref ref-type="bibr" rid="B14">14</xref>], electrical method [<xref ref-type="bibr" rid="B15">15</xref>]-[<xref ref-type="bibr" rid="B18">18</xref>], chemical [<xref ref-type="bibr" rid="B19">19</xref>]-[<xref ref-type="bibr" rid="B22">22</xref>], acoustic [<xref ref-type="bibr" rid="B23">23</xref>]-[<xref ref-type="bibr" rid="B25">25</xref>], optical [<xref ref-type="bibr" rid="B26">26</xref>][<xref ref-type="bibr" rid="B27">27</xref>] and combinations of these methods [<xref ref-type="bibr" rid="B28">28</xref>]-[<xref ref-type="bibr" rid="B31">31</xref>]. However, electrical and chemical methods require contact with the equipment, which may bring interference of normal railway operations; whereas acoustic and optical methods may be disrupted by the environmental noises that may affect the detection accuracy.</p>
      <p>On the other hand, since PD usually emits a radio frequency (RF) signal in a range between 300 and 1500 MHz, we can employ one or multiple ultra-high-frequency (UHF) antenna(s) to scan and detect RF signals in the air within this spectrum. However, continuously and losslessly monitoring PD signals that span over a wide frequency range of up to 1500 MHz usually requires a minimum sampling rate of 3GHz (<italic>i.e.</italic>, <inline-formula><mml:math><mml:mrow><mml:mtext> 3 </mml:mtext><mml:mo> × </mml:mo><mml:msup><mml:mrow><mml:mn> 10 </mml:mn></mml:mrow><mml:mn> 9 </mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> samples per second) of the data acquisition </p>
      <fig id="fig2">
        <label>Figure 2</label>
        <graphic xlink:href="https://html.scirp.org/file/3501028-rId16.jpeg?20251208015046" />
      </fig>
      <p><bold>Figure 2</bold><bold>.</bold> Damages caused by PD hazards. (a) Inner surface burn; (b) Burn through the shield; (c) Contact damage; (d) Explosion of the pillar insulator.</p>
      <p>system (DAS), proposing an excessive hardware challenge in processing this huge amount of data. Developing such high-speed customized DAS is often costly and takes a long time to align all hardware to work effectively and reliably. In addition, a single UHF antenna may not suffice the demand to constantly capture PD signals of such broadband, and employing multiple antennas will bring extra complexity to the circuit.</p>
      <p>To resolve such challenges, we propose to use a single antenna to iteratively scan the spectrum from 100 MHz to 2500 MHz with intermediate frequency (IF) modulation [<xref ref-type="bibr" rid="B32">32</xref>][<xref ref-type="bibr" rid="B33">33</xref>]. In this way, the system only has one input and is flexible to various scanning spectrums by adjusting the IF modulation frequencies. One drawback of this method is that the band-limited antenna can only scan a small range of RF spectrum at a time while leaving other spectrum unattended, causing the possibility of missing the PD. Nevertheless, as long as the PD events are repetitive and with proper configuration of the scanning rate, the system will catch PD occurrence confidently.</p>
      <p>The organization of this paper is as follows. The development of the proposed PD detection and cloud-based monitoring is described in Section 2, and the system evaluations are illustrated in Section 3. The conclusion is drawn in Section 4.</p>
    </sec>
    <sec id="sec2">
      <title>2. Development of a Non-Disruptive Real-Time PD Detection and Monitoring System</title>
      <p>This chapter introduces the developed hardware and software platform for PD signal capturing, detection and recording, as well as the cloud-based remote access on the smartphone (<xref ref-type="fig" rid="fig3">Figure 3</xref>). The PD signal data acquisition system only consists of an antenna with a passing bandwidth of 800 MHz centered at 136 MHz, a Tektronix RSA 306B real-time RF spectrum analyzer [<xref ref-type="bibr" rid="B34">34</xref>], and a computer (or other high-performance embedded system) with USB-3 interface. Key specifications of the RSA 306B are listed in <bold>Table 1</bold>.</p>
      <fig id="fig3">
        <label>Figure 3</label>
        <graphic xlink:href="https://html.scirp.org/file/3501028-rId17.jpeg?20251208015047" />
      </fig>
      <p><bold>Figure 3</bold><bold>.</bold> IoT-cloud-based remote accessible real-time PD monitoring system diagram.</p>
      <p><bold>Table 1</bold><bold>.</bold> Key specification of tektronix RSA 306b real-time RF analyzer.</p>
      <table-wrap id="tbl1">
        <label>Table 1</label>
        <table>
          <tbody>
            <tr>
              <td>Detection Frequency</td>
              <td>9 K - 6.2 GHz</td>
            </tr>
            <tr>
              <td>Sampling Frequency</td>
              <td>112 MSa/s</td>
            </tr>
            <tr>
              <td>IF Bandwidth</td>
              <td>Max. 40 MHz</td>
            </tr>
            <tr>
              <td>ADC bit-width</td>
              <td>14-bit</td>
            </tr>
            <tr>
              <td>Amplitude Accuracy</td>
              <td>About 1 dB</td>
            </tr>
            <tr>
              <td>Max DC Level</td>
              <td>±40 Vdc</td>
            </tr>
            <tr>
              <td>Average Noise</td>
              <td>≤−130 dB</td>
            </tr>
          </tbody>
        </table>
      </table-wrap>
      <sec id="sec2dot1">
        <title>2.1. PD Data Acquisition Process</title>
        <p>During each PD sampling process, the RF antenna contactlessly senses the PD signals in the air and conveys them to the RSA 306B, which sets up an intermediate frequency (IF) carrier signal to shift the ultra-high frequency PD signals to a lower spectrum (<italic>i.e.</italic>, IF modulation). The modulated signal will then be sampled, quantified and digitized by high-speed analog-to-digital converter (ADC), and the data stream will be transmitted to the computer via USB-3 connection (<xref ref-type="fig" rid="fig4">Figure 4</xref>). Here, we call the data within one sample duration (<italic>i.e.</italic>, 10 milliseconds in this study) a data or sample frame. The computer reads the data frame via Tektronix application programing interface (API) [<xref ref-type="bibr" rid="B35">35</xref>], and calculates the data in both time domain in-phase/quadrature (I/Q) stream form (<italic>i.e.</italic>, quadrature modulation) (<xref ref-type="fig" rid="fig5">Figure 5</xref>) [<xref ref-type="bibr" rid="B36">36</xref>] and spectrum form (<xref ref-type="fig" rid="fig6">Figure 6</xref>) using Fourier Transform, Equation (1). The power is calculated as Equation (2).</p>
        <disp-formula id="FD1">
          <label>(1)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:mi>X</mml:mi>
              <mml:mrow>
                <mml:mo>[</mml:mo>
                <mml:mi>k</mml:mi>
                <mml:mo>]</mml:mo>
              </mml:mrow>
              <mml:mo>=</mml:mo>
              <mml:munderover>
                <mml:mstyle mathsize="140%" displaystyle="true">
                  <mml:mo>∑</mml:mo>
                </mml:mstyle>
                <mml:mrow>
                  <mml:mi>n</mml:mi>
                  <mml:mo>=</mml:mo>
                  <mml:mn>0</mml:mn>
                </mml:mrow>
                <mml:mrow>
                  <mml:mi>N</mml:mi>
                  <mml:mo>−</mml:mo>
                  <mml:mn>1</mml:mn>
                </mml:mrow>
              </mml:munderover>
              <mml:mi>x</mml:mi>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mi>n</mml:mi>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:msup>
                <mml:mi>e</mml:mi>
                <mml:mrow>
                  <mml:mo>−</mml:mo>
                  <mml:mrow>
                    <mml:mrow>
                      <mml:mi>j</mml:mi>
                      <mml:mn>2</mml:mn>
                      <mml:mi>π</mml:mi>
                      <mml:mi>k</mml:mi>
                      <mml:mi>n</mml:mi>
                    </mml:mrow>
                    <mml:mo>/</mml:mo>
                    <mml:mi>N</mml:mi>
                  </mml:mrow>
                </mml:mrow>
              </mml:msup>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <disp-formula id="FD2">
          <label>(2)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:mi>P</mml:mi>
              <mml:mi>o</mml:mi>
              <mml:mi>w</mml:mi>
              <mml:mi>e</mml:mi>
              <mml:mi>r</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mn>10</mml:mn>
              <mml:mi>log</mml:mi>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mfrac>
                    <mml:mrow>
                      <mml:msup>
                        <mml:mi>I</mml:mi>
                        <mml:mn>2</mml:mn>
                      </mml:msup>
                      <mml:mo>+</mml:mo>
                      <mml:msup>
                        <mml:mi>Q</mml:mi>
                        <mml:mn>2</mml:mn>
                      </mml:msup>
                    </mml:mrow>
                    <mml:mrow>
                      <mml:mn>1</mml:mn>
                      <mml:mi>m</mml:mi>
                      <mml:mi>W</mml:mi>
                    </mml:mrow>
                  </mml:mfrac>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <fig id="fig4">
          <label>Figure 4</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId22.jpeg?20251208015049" />
        </fig>
        <p><bold>Figure 4</bold><bold>.</bold> Signal capturing, modulation and sampling in RSA 306B.</p>
        <fig id="fig5">
          <label>Figure 5</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId23.jpeg?20251208015049" />
        </fig>
        <p><bold>Figure 5</bold><bold>.</bold> I/Q modulation for data in time domain [<xref ref-type="bibr" rid="B36">36</xref>].</p>
        <fig id="fig6">
          <label>Figure 6</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId24.jpeg?20251208015049" />
        </fig>
        <p><bold>Figure 6</bold><bold>.</bold> RSA API and data flow in computer [<xref ref-type="bibr" rid="B36">36</xref>].</p>
        <p>If the system detects any signal power exceeding a pre-set threshold (<italic>i.e.</italic>, −50 dB in this study) during each sample frame, the I/Q data and spectrum information of that frame will be recorded in .r3f and siq format (<xref ref-type="fig" rid="fig7">Figure 7</xref>), which can be further decoded to the time sequence .csv files. The fundamental functions of data acquisition are fulfilled by C/C++ based on RSA 306B API, and a python interface is implemented on top of the C/C++ code and RSA API for the simplicity of user interaction and process control.</p>
        <fig id="fig7">
          <label>Figure 7</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId25.jpeg?20251208015049" />
        </fig>
        <p><bold>Figure 7</bold><bold>.</bold> r3f and .siq file for data storage [<xref ref-type="bibr" rid="B36">36</xref>].</p>
        <p>As the RSA has the sampling rate of 112 MHz and its signal sampling bandwidth of 40 MHz, for each complete PD scanning process, the system will iteratively set RSA’s IF modulation carrier frequency from 100 MHz to 2500 MHz (<italic>i.e.</italic>, one iteration), with an incremental step of 40 MHz, to cover the PD signal frequency of interest (<xref ref-type="fig" rid="fig8">Figure 8</xref>). In the end of each iteration (<italic>i.e.</italic>, 61 samples in 60 iterations of 600 milli-seconds), the system will stitch the power-spectrum diagram of each sample frame for a complete diagram, and remove I/Q data that does not include any PD signals. If any PD signals are captured, the corresponding I/Q data and power-spectrum diagrams will be kept and named according to the timestamp and detected PD frequency. In this way, users can easily observe and trace back the records of PD occurrences, and the system storage can be more efficiently utilized.</p>
      </sec>
      <sec id="sec2dot2">
        <title>2.2. Remote Access to Continuous Real-Time PD Monitoring</title>
        <p>With the expansion of widely spread high-speed rail network, internet of things (IoT) technology should be added to local PD detection and monitoring system at each switchgear/transformer station for the remote accessibility and potentially instant responsiveness to any alert messages it may generate. To achieve this goal, the google cloud service (e.g., Google Drive, Firebase, etc.) is employed and a </p>
        <fig id="fig8">
          <label>Figure 8</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId26.jpeg?20251208015050" />
        </fig>
        <p><bold>Figure 8</bold><bold>.</bold> (a) Iterative sampling and spectrum analysis; (b) Iterative scanning to cover the entire PD spectrum.</p>
        <p>smartphone application (APP) is developed. The local PD DAS will exploit Rclone [<xref ref-type="bibr" rid="B37">37</xref>] to set up a new cloud storage node, and continuously synchronize the newly detected PD I/Q data and full power-spectrum diagram to the cloud storage at the end of each PD scanning iteration. On the other hand, when the user activates the APP, it will periodically request data synchronization with the cloud server via Google drive API, so that the user can see the updated PD monitoring on their fingertips. In addition, whenever the cloud receives new files, it sends out a notification email to alert the user for newly detected PD events.</p>
      </sec>
    </sec>
    <sec id="sec3">
      <title>3. System Evaluations</title>
      <sec id="sec3dot1">
        <title>3.1. Lab Environment and Hardware Setup</title>
        <p>In this section, the system evaluation results are presented. The system has been tested under the lab environment (<xref ref-type="fig" rid="fig9">Figure 9</xref>), by applying a configurable arbitrary waveform generator (AWG) with a broad bandwidth of 2GHz [<xref ref-type="bibr" rid="B38">38</xref>]. The AWG output is connected with a 50 Ω resistive load, which is parallel connected with a 2 G bandwidth oscilloscope [<xref ref-type="bibr" rid="B39">39</xref>] with spectrum analyzer to measure the actual signal waveform, amplitude and frequency that is applied onto the resistor. When the AWG signal passes through the resistor, the circuit generates RF signals as a simulation of PD signals within 100 - 2500 MHz range. Numerical test scenarios have been proceeded, and here we illustrate two representative cases, single-signal and dual-signal detection, to validate the functionalities.</p>
        <fig id="fig9">
          <label>Figure 9</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId27.jpeg?20251208015051" />
        </fig>
        <p><bold>Figure 9</bold><bold>.</bold> Lab test setup for PD DAS (including antenna, RSA 306B, a portable computer/embedded system), an AWG, a 50-ohm resistor (<italic>i.e.</italic>, PD stimulator), and an oscilloscope.</p>
      </sec>
      <sec id="sec3dot2">
        <title>3.2. Single RF/PD Signal Capturing</title>
        <p>We connect the 50 Ω resistor with AWG via BNC-alligator cable, and placed the PD DAS with its antenna about one foot away from the resistor. Once the PD DAS is turned on and initiated with the program to scan RF/PD signals in the air, we set up the AWG to generate a 315 MHz sine waveforms of 1V peak-to-peak. Then, the DAS captures the RF signals that exceed the preset threshold (<xref ref-type="fig" rid="fig10">Figure 10</xref>), and generates one spreadsheet (<italic>i.e.</italic>, .csv file) of signal value in time-domain (<italic>i.e.</italic>, I/Q ADC values), and a power-spectrum diagram in frequency domain (<xref ref-type="fig" rid="fig11">Figure 11(a)</xref> and <xref ref-type="fig" rid="fig11">Figure 11(b)</xref>). In the end of that particular scanning iteration, a complete power-spectrum diagram is drawn from 100 MHz to 2500 MHz (<xref ref-type="fig" rid="fig11">Figure 11(c)</xref>). Another test results of 768 MHz RF/PD signal are demonstrated in <xref ref-type="fig" rid="fig11">Figure 11(d)-(f)</xref>. One can see that although there exist some relatively low frequency noises, most less than 1 MHz and −60 dB, RF/PD signals of interest can be clearly captured without much interference. In addition, the IF modulation </p>
        <fig id="fig10">
          <label>Figure 10</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId29.jpeg?20251208015053" />
        </fig>
        <p><bold>Figure 10</bold><bold>.</bold> Capturing signals exceeding the power threshold.</p>
        <fig id="fig11">
          <label>Figure 11</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId30.jpeg?20251208015053" />
        </fig>
        <p><bold>Figure 11</bold><bold>.</bold> (a) Capturing 315 MHz RF/PD signals with ADC values in time domain; (b) Impulse at 315 MHz in frequency domain for one frame; (c) Impulse at 315 MHz in complete scanning iteration; (d) Capturing 768 MHz RF/PD signals with ADC values in time domain; (e) Impulse at 768 MHz in frequency domain for one frame; (f) Impulse at 768 MHz in complete scanning iteration.</p>
        <p>can be observed in <xref ref-type="fig" rid="fig11">Figure 11(a)</xref> and especially in <xref ref-type="fig" rid="fig11">Figure 11(d)</xref>, because of the higher IF carrier frequency.</p>
      </sec>
      <sec id="sec3dot3">
        <title>3.3. Dual/Multiple RF/PD Signal Capturing</title>
        <p>We also have run the dual RF/PD detection test to confirm that if multiple PD events occur approximately at the same time (<italic>i.e.</italic>, in one scanning iteration), the PD DAS can capture both of them. We first create a Bluetooth signal (<italic>i.e.</italic>, about 2400 MHz) by turning on two Bluetooth devices and transmitting large files from one device to the other. Meanwhile, we create another 768 MHz signal with AWG as aforementioned, and turn on the PD DAS. It is worth noting that we have to adjust the RF/PD detection threshold to −70 dB so as to catch the low-power Bluetooth signal. As depicted in <xref ref-type="fig" rid="fig12">Figure 12</xref>, one can see that the DAS can clearly capture both 768 MHz and the Bluetooth signals.</p>
        <p>The confirmation of capturing multiple RF signals of various frequency demonstrates the capability and adaptivity of detecting a variety of PD signals simultaneously. Yet, the power threshold for signal detection needs to be carefully selected as it balances the detection rate and false alarms. Meanwhile, various signal filter techniques (e.g., band-pass and band-stop filters, wavelet filtering, etc.) can be applied to distinguish the hazard PD signals from the routine RF traffic with known spectrums.</p>
        <fig id="fig12">
          <label>Figure 12</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId31.jpeg?20251208015054" />
        </fig>
        <p><bold>Figure 12</bold><bold>.</bold> (a) No test signal generated (only noises); (b) Only with a 768 MHz generated by AWG; (c) Only with a Bluetooth signal at about 2400 MHz; (d) With both 768 MHz and Bluetooth signals in the air.</p>
      </sec>
      <sec id="sec3dot4">
        <title>3.4. Cloud-Cased Remote Monitoring</title>
        <p>The cloud service is established on the DAS via Google drive and Rclone, so that any files created and edited within this particular Google drive folder will be automatically synchronized in all terminals that use the same Google drive account. Once the user logs in with proper credentials (<xref ref-type="fig" rid="fig13">Figure 13(a)</xref>) on a remote device (e.g., a smartphone), one can see the updated I/Q data and spectrum diagrams (<xref ref-type="fig" rid="fig13">Figure 13(b)</xref>), and corresponding file attribute details (<xref ref-type="fig" rid="fig13">Figure 13(c)</xref>). In addition to the real-time synchronization from the local PD DAS to the cloud and granting remote accessibility, the cloud also sends a notification email to the user whenever any new PD signals are detected (<xref ref-type="fig" rid="fig13">Figure 13(d)</xref>). In that case, personnel who is in charge of monitoring the switchgears and transformers in high-speed </p>
        <fig id="fig13">
          <label>Figure 13</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId32.jpeg?20251208015055" />
        </fig>
        <fig id="fig14">
          <label>Figure 14</label>
          <graphic xlink:href="https://html.scirp.org/file/3501028-rId33.jpeg?20251208015055" />
        </fig>
        <p><bold>Figure 13</bold><bold>.</bold> (a) APP login; (b) APP access to files; (c) File attribute details; (d) Email notifications of detected PD events.</p>
        <p>rail can be alerted at early stage to minimize the potential damage and maintenance cost PD may cause.</p>
      </sec>
    </sec>
    <sec id="sec4">
      <title>4. Conclusions</title>
      <p>This study has successfully developed an advanced platform for the non-disruptive, continuous, real-time detection and monitoring of partial discharges in switchgears and transformers used within high-speed rail infrastructure. The system is designed to iteratively scan and capture PD signals within a frequency range of 100 MHz to 2500 MHz, ensuring comprehensive coverage and detection of PD activities.</p>
      <p>In addition to its robust detection capabilities, the system is seamlessly integrated with cloud services, enabling remote accessibility to real-time PD data and analysis results. This feature facilitates prompt decision-making and timely interventions by maintenance teams, significantly enhancing the overall reliability and safety of high-speed rail operations.</p>
      <p>Extensive laboratory evaluations have been conducted to assess the system’s performance. These evaluations demonstrate the system’s effectiveness and proficiency in automated real-time PD detection and long-term monitoring. The results indicate that the platform not only meets but exceeds the operational requirements, ensuring that potential faults are identified and addressed promptly before they can escalate into major issues.</p>
      <p>The successful implementation of this platform marks a significant advancement in the maintenance and monitoring of high-voltage electrical infrastructure in high-speed rail systems. By leveraging real-time data and remote monitoring capabilities, this system represents a proactive approach to infrastructure management, reducing the risk of unexpected failures and enhancing the overall efficiency and safety of high-speed rail operations.</p>
    </sec>
    <sec id="sec5">
      <title>Acknowledgements</title>
      <p>This study was conducted with the support from the USDOT Tier 1 University Transportation Center on Railroad Sustainability and Durability with the grant no. 69A3551747132.</p>
    </sec>
  </body>
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