<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">ENG</journal-id><journal-title-group><journal-title>Engineering</journal-title></journal-title-group><issn pub-type="epub">1947-3931</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/eng.2014.67040</article-id><article-id pub-id-type="publisher-id">ENG-46715</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>ENGINEERING</subject></subj-group></article-categories><title-group><article-title>A Quick Classification Method of the Power Quality Disturbances</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yi</surname><given-names>Yi Tang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hao</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Information and Electrical Engineering, China University of Mining &amp; Technology, Xuzhou, China</addr-line></aff><aff id="aff2"><addr-line>NARI Group Corporation (State Grid Electric Power Research Institute), Nanjing, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>tangyi@cumt.edu.cn(YYT)</email>;<email>ditfft@126.com(HL)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>11</day><month>06</month><year>2014</year></pub-date><volume>06</volume><issue>07</issue><fpage>374</fpage><lpage>384</lpage><history><date date-type="received"><day>3</day>	<month>November</month>	<year>2013</year></date><date date-type="rev-recd"><day>5</day>	<month>April</month>	<year>2014</year>	</date><date date-type="accepted"><day>20</day>	<month>April</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
	This
paper introduces a quick classification method of the power quality
disturbances. Based on analyzing the characteristics of different electrical
disturbance signals in time domain, four distinctive features are extracted
from electrical signals for classifying different power quality disturbances
and then an automatic classifier is proposed. Using the proposed classification
method,a PQ monitor of the classifying
power quality disturbances is developed based on the TMS320F2812DSP
micro-processor. Semi-physical simulation, lab experiment and field measurement
results have verified that this proposed method can classify single or complex
disturbance signals effectively.
</p></abstract><kwd-group><kwd>Power Quality</kwd><kwd> Disturbance Classification</kwd><kwd> Noise</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>To detect and improve power quality, we first need to monitor and analyze the power quality disturbances. There have been many methods presented, such as Fourier transform [<xref ref-type="bibr" rid="scirp.46715-ref1">1</xref>] , wavelet transform [<xref ref-type="bibr" rid="scirp.46715-ref2">2</xref>] -[<xref ref-type="bibr" rid="scirp.46715-ref4">4</xref>] , S transform and so on. The Fourier transform is suitable to analyze stationary signals, and has a good effect on stationary disturbance like harmonics; the wavelet transform has advantage of analyzing singularity and nonstationary signals [<xref ref-type="bibr" rid="scirp.46715-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.46715-ref6">6</xref>] ; S transform is the inheritance and development of short-time Fourier transform and wavelet transform. So it has the advantages of the both [<xref ref-type="bibr" rid="scirp.46715-ref7">7</xref>] -[<xref ref-type="bibr" rid="scirp.46715-ref11">11</xref>] . And it analyzes signal features more comprehensively and it has been a hot research tool of power quality disturbance classification. They are all the time frequency transform methods. This paper presents a method based on the time domain analysis of the power quality disturbance signals and it has some advantages compared to the time frequency transform methods. It will be discussed in details in Section 4.</p></sec><sec id="s2"><title>2. The Analysis of Power Quality Disturbances in Time Domain</title><p>The general single-phase voltage signal can be expressed as the superposition of the fundamental wave voltage and the disturbance signals:</p><disp-formula id="scirp.46715-formula1928"><label>(1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\e322ec37-0ec5-49cc-9dc9-a301aeb0dfb9.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\2e05fda6-7ade-42ef-bd53-464c5b66ea77.png" xlink:type="simple"/></inline-formula> is the RMS (root mean square) voltage with the system fundamental frequency; <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\b7d9f2dc-20f7-45a2-a69f-d14575aa74ff.png" xlink:type="simple"/></inline-formula>is the system fundamental angular frequency; <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\aaf77a59-2931-495d-ae30-c65f596db838.png" xlink:type="simple"/></inline-formula>is the initial phase angle; <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\fcc45fda-e651-409a-8bdd-394eefa9d505.png" xlink:type="simple"/></inline-formula>is the h<sub>th</sub> harmonic RMS voltage; <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\f6c988bc-af21-4876-b738-eb672d6d429c.png" xlink:type="simple"/></inline-formula>is the h<sub>th</sub> harmonic initial phase angle; <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\1fbe93b9-9bae-47c6-aa2e-e2ca4f0a87d4.png" xlink:type="simple"/></inline-formula>is the angular frequency between harmonic waveforms and not an integer multiple of the system fundamental frequency, for example, the frequencies of interharmonics and oscillatory transients; <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\93285301-4310-4762-ba9b-baee89381a83.png" xlink:type="simple"/></inline-formula>is the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\63f88a2c-d629-438a-a4e0-ed54902d22ef.png" xlink:type="simple"/></inline-formula> RMS voltage with <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\b7dfd3e2-041e-4f1a-a59f-3ac697c7d592.png" xlink:type="simple"/></inline-formula> angular frequency; <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\19a17bf7-f81e-4b3f-a233-7f5399055732.png" xlink:type="simple"/></inline-formula>is the initial phase angle of the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\595e4b16-8ba5-42f7-abed-6fed090a7a31.png" xlink:type="simple"/></inline-formula> angular frequency voltage; <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\e9ad786d-f5b3-4bc7-a44f-872b4c7333df.png" xlink:type="simple"/></inline-formula>is the oscillatory transient attenuation constant. When<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\865cc8dc-d3a4-4625-8995-fa986dc3e4db.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\a99f1c81-76df-4769-b72f-c24a73dd4a3f.png" xlink:type="simple"/></inline-formula>is the interharmonic RMS voltage and when<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\1b3593d9-dd17-468c-9bfc-7ff67bb6bd75.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\1dcaf232-8e96-4b03-9bc9-b2eb89e2cd32.png" xlink:type="simple"/></inline-formula>is the oscillatory transients RMS voltage; <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\4abd5c9e-bcb0-4463-925b-15efab92160e.png" xlink:type="simple"/></inline-formula>is the starting time; l(t) is the unit step function. <xref ref-type="table" rid="table1">Table 1</xref> shows that characteristics of the disturbances which IEEE classified [<xref ref-type="bibr" rid="scirp.46715-ref12">12</xref>] . All the simulation parameters in this paper are chosen from <xref ref-type="table" rid="table1">Table 1</xref> randomly.</p><p>In Equation (1), when <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\918970ef-3408-458c-a68d-053e78af2860.png" xlink:type="simple"/></inline-formula> is stationary, equal to the rating value and</p><disp-formula id="scirp.46715-formula1929"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\310251e4-0d88-4993-a3be-fc78396cfc60.png"/></disp-formula><p>Equation (1) represents the ideal voltage. So the voltage disturbance can be divided into two categories. One is the disturbances with the change of the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\fc922081-6139-41fd-b988-496627f3d473.png" xlink:type="simple"/></inline-formula> amplitude, including voltage sag, swell, interruption, under voltage, over voltage, fluctuation, flicker and so on. The other is the additive disturbances, including harmonics, oscillatory transients, impulse voltage, interharmonics and so on. From the aspect of disturbance duration, we can also divide the disturbances into two categories. One is stationary disturbance, including voltage fluctuation and flicker, under voltage, over voltage, continuous interruption, harmonics, interharmonics and so on. The other is transient disturbances, including voltage sag, swell, instantaneous interruption, oscillatory transients, impulse voltage and so on. So the power quality disturbances can be divided into four categories by time domain features, shown in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>For voltage sag, swell and interruption has the similar characteristics, the author only takes voltage sag as the analyzing object. The other two can also be identified by the method presented in this paper.</p><p>If <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\3245522e-be73-464e-b3cc-40bfa4715dd3.png" xlink:type="simple"/></inline-formula> in Equation (1) is multiplied by<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\9e9d77ed-dc27-4f2b-b5d3-bae497bb00a4.png" xlink:type="simple"/></inline-formula>, we can get:</p><disp-formula id="scirp.46715-formula1930"><label>(2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\fe3e906f-79cd-4c11-a269-ddb0eca69c32.png"/></disp-formula><table-wrap id="table1"  position="float"><object-id pub-id-type="pii">Table 1</object-id><label>Table 1</label><caption><p>. Typical characteristics of power system disturbances</p></caption><table><thead><tr><th align="center" valign="middle" >Disturbances</th><th align="center" valign="middle" >Typical spectral content</th><th align="center" valign="middle" >Typical duration</th><th align="center" valign="middle" >Typical voltage magnitude</th></tr></thead><tbody><tr><td align="center" valign="middle" >Voltage sag</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.5 cycles - 1 min</td><td align="center" valign="middle" >0.1 - 0.9 pu</td></tr><tr><td align="center" valign="middle" >Fluctuation and flicker</td><td align="center" valign="middle" >&lt;25 Hz</td><td align="center" valign="middle" >Intermittent</td><td align="center" valign="middle" >0.1% - 7%</td></tr><tr><td align="center" valign="middle" >Harmonics</td><td align="center" valign="middle" >0 - 100<sup>th</sup> Hz</td><td align="center" valign="middle" >Steady state</td><td align="center" valign="middle" >0% - 20%</td></tr><tr><td align="center" valign="middle" >Oscillatory transients</td><td align="center" valign="middle" >&lt;5 kHz</td><td align="center" valign="middle" >0.3 - 50 ms</td><td align="center" valign="middle" >0 - 4 pu</td></tr><tr><td align="center" valign="middle" >Interharmonics</td><td align="center" valign="middle" >0 - 6 kHz</td><td align="center" valign="middle" >Steady state</td><td align="center" valign="middle" >0% - 2%</td></tr></tbody></table></table-wrap><table-wrap id="table2"  position="float"><object-id pub-id-type="pii">Table 2</object-id><label>Table 2</label><caption><p>. The categories of the voltage disturbance</p></caption><table><thead><tr><th align="center" valign="middle"  rowspan="2"  >Voltage amplitude disturbances</th><th align="center" valign="middle" >Stationary</th><th align="center" valign="middle" >Fluctuation and flicker, under voltage ,over voltage</th></tr></thead><tbody><tr><td align="center" valign="middle" >Transient</td><td align="center" valign="middle" >Voltage sag, swell, transient interruption</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >Additive disturbances</td><td align="center" valign="middle" >Stationary</td><td align="center" valign="middle" >Harmonics, interharmonics</td></tr><tr><td align="center" valign="middle" >Transient</td><td align="center" valign="middle" >Oscillatory transients, impulse voltage</td></tr></tbody></table></table-wrap><p>where, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\0d5b696b-3df2-4ed4-a2a4-66bf68c5986f.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\81f9f8e2-3509-432e-b0ef-ed31b62f2332.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\95395774-985b-4e2d-8f21-4bdce243f09a.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\1357f92e-221f-4d15-ac3e-895c7ac780de.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\e6ce32bf-a691-4b33-a183-b50cd1b2ac73.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\9415eba6-dd93-41a0-bcda-ef66352354a2.png" xlink:type="simple"/></inline-formula></p><p>Equation (2) consists of three parts. First is DC component<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\4a3ae25b-a99b-44c7-8768-00697693e437.png" xlink:type="simple"/></inline-formula>. Second is an AC component <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\10181b55-ec96-4d45-9c0f-7419df1bd496.png" xlink:type="simple"/></inline-formula> with an integer multiple system frequency. Third is an AC component <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\626155af-e92a-46c0-98b3-cae97995f878.png" xlink:type="simple"/></inline-formula> with a non-integer multiple system frequency. After a full cycle (0 - T) integral of the (2) we can see that<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\59e026aa-e934-4a80-beab-0274af07d4be.png" xlink:type="simple"/></inline-formula>, and some AC components still exist in<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\5afe1cbf-ac5c-49be-8851-027f64734e54.png" xlink:type="simple"/></inline-formula>. <xref ref-type="fig" rid="fig1">Figure 1</xref> is the curve of the full cycle integral of (2). In <xref ref-type="fig" rid="fig1">Figure 1</xref>(a) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(b) only contain<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\e7abd564-b50e-4596-a345-8e4f40549015.png" xlink:type="simple"/></inline-formula>. <xref ref-type="fig" rid="fig1">Figure 1</xref>(c) contains <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\b9d360cb-5720-4941-8329-76076e97a68e.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\e7a8d502-94a5-42e8-9fd6-1bc5ae4504fb.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\48b757a3-69d5-4cbf-b24c-7160f982fa09.png" xlink:type="simple"/></inline-formula>. <xref ref-type="fig" rid="fig1">Figure 1</xref>(d) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(e) contain <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\02dc1eba-334d-4f6e-bbc6-96e1d0285c0a.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\0a2f33b3-01f0-4ccf-a34b-e8f136a12f01.png" xlink:type="simple"/></inline-formula>. For <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\744e36ce-f540-45d2-b81d-d82027bc7a89.png" xlink:type="simple"/></inline-formula> is the sine wave AC value of non-integer multiple system frequency, after a full cycle integral<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\ca3a4ac3-7a66-4cad-8149-3b53fa3771fa.png" xlink:type="simple"/></inline-formula>. It shows the existence of the sine wave AC disturbance of non-integer multiple system frequency. The simulation parameters of the following pictures are chosen in the range of <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The square of Equation (1) is:</p><disp-formula id="scirp.46715-formula1931"><label>(3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\8ca88130-acfb-4bff-a871-1af5cf140cf0.png"/></disp-formula><p>The expanded formula of (3) is long, but also is consists of three parts: DC component<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\0c2316dd-e205-459e-ae12-84f6781a7940.png" xlink:type="simple"/></inline-formula>, an AC component <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\20c4c28a-b6e5-4bf8-851d-d2cbc5656138.png" xlink:type="simple"/></inline-formula> with an integer multiple system frequency, an AC component <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\df232323-9cc5-4fb1-adbc-e5d7760d5656.png" xlink:type="simple"/></inline-formula> with a non-integer multiple system frequency. In it:</p><disp-formula id="scirp.46715-formula1932"><label>(4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\898536b3-d04d-424b-9dd7-233f5dfa6b6c.png"/></disp-formula><p>The curve of a full cycle integral of (3) is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>By comparing <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref>, we can find that <xref ref-type="fig" rid="fig1">Figure 1</xref>(a) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(b) are the same with <xref ref-type="fig" rid="fig2">Figure 2</xref>(a) and <xref ref-type="fig" rid="fig2">Figure 2</xref>(b) because there is no additive disturbance in the voltage sag and fluctuation and flicker. The harmonics is additive disturbance, so the U<sub>d</sub>/U<sub>N</sub> in <xref ref-type="fig" rid="fig2">Figure 2</xref>(c) is larger than U<sub>1</sub>/U<sub>N</sub> in <xref ref-type="fig" rid="fig1">Figure 1</xref>(c). And the dif-</p><p>ference between them is the amplitude of the additive disturbance<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\0bc874d1-3e59-456b-bd41-4020987e31da.png" xlink:type="simple"/></inline-formula>. The oscillatory transients and in-</p><p>terharmonics are the additive disturbances. So the U<sub>d</sub>/U<sub>N</sub> in <xref ref-type="fig" rid="fig2">Figure 2</xref>(d) and <xref ref-type="fig" rid="fig2">Figure 2</xref>(e) is larger than the U<sub>1</sub>/U<sub>N</sub> in <xref ref-type="fig" rid="fig1">Figure 1</xref>(d) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(e). And the difference is also the amplitude of additive disturbance</p><disp-formula id="scirp.46715-formula1933"><label>.</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\041cfd7b-ceb7-4652-94ca-5ef7a6376526.png"/></disp-formula><fig-group id="fig1"><caption><title>Figure 1</title><p> The curve of full cycle integral of (2). (a) Voltage sag; (b) fluctuation and flicker; (c) harmonics; (d) Oscillatory transients; (e) Interharmonics</p></caption><fig id ="fig1_1"><label>(a)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\7f79a352-7024-416e-8357-b5ee873b76ac.png"/></fig><fig id ="fig1_2"><label>(b)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\17dfc767-025e-44fe-a9de-7f2c19c51b31.png"/></fig><fig id ="fig1_3"><label>(c)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\426bfd1c-5e0c-42fb-ae5d-d42813494e20.png"/></fig><fig id ="fig1_4"><label>(d)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\ee573a0e-0fe4-469c-a227-a74ee5ff8b8f.png"/></fig><fig id ="fig1_5"><label>(e)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\53e4da29-aaf9-494a-bf74-6bce7acfdebf.png"/></fig></fig-group><fig-group id="fig2"><caption><title>Figure 2</title><p> The curve of full cycle integral of (3). (a) Voltage sag; (b) Fluctuation and flicker; (c) Harmonics; (d) Oscillatory transients; (e) Interharmonics</p></caption><fig id ="fig2_1"><label>(a)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\935e6f7c-af43-4763-aa23-2c237233fff0.png"/></fig><fig id ="fig2_2"><label>(b)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\bcdbd0a9-9092-45a7-a7ab-41c2281f8038.png"/></fig><fig id ="fig2_3"><label>(c)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\43dda645-31d8-45df-ba5d-d52b90bc94d7.png"/></fig><fig id ="fig2_4"><label>(d)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\f6dcd726-29f7-42ff-bf93-ad94842f1b14.png"/></fig><fig id ="fig2_5"><label>(e)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\7295c40e-429c-4c79-9f0b-d9a3c85a7400.png"/></fig></fig-group></sec><sec id="s3"><title>3. Basic Idea of the Classification of the Power Quality Disturbances</title><p>Though above analysis, some individual features of the power quality disturbance singles can be shown in time- domain:</p><p>1) Equation (2) has the effect of selecting system fundamental frequency. The DC component, which can be gotten by low pass filter from Equation (2), is the RMS voltage with system fundamental frequency, which is not affected by additive disturbance. And its change is equivalent to the amplitude disturbance of the RMS voltage (like voltage sag, swell, transient interrupt, under voltage, over voltage, continuous interrupt, fluctuation, flicker and so on).</p><p>2) The DC component of Equation (3) is the geometric sum of the RMS voltage with system fundamental frequency and all other additive disturbance RMS voltages. So the geometric difference of the Equation (3) and Equation (2)’s DC component is exactly equivalent to the amplitude of the additive disturbance (like harmonics, oscillatory transients, impulse voltage and interharmonics).</p><p>3) <xref ref-type="fig" rid="fig1">Figure 1</xref>(d) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(e)’s curves contain <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\67351a05-3227-48d5-8891-c90e98490d09.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\deffb362-f59a-4d2e-8962-267142e7b13f.png" xlink:type="simple"/></inline-formula>.The component <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\b48a5a9a-ab94-4fa4-8758-5770fc9fda37.png" xlink:type="simple"/></inline-formula> exists usually because of the existence of the interharmonics and the oscillatory transients which are non-integer system fundamental frequency sine wave signal. <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\6860a6b7-1927-4a36-8b63-13a1ae2f1cef.png" xlink:type="simple"/></inline-formula>indicates the existence of the interharmonics or oscillatory transients.</p><p>So, the next 4 features (F<sub>1</sub> - F<sub>4</sub>) can be used to classify power quality single disturbances and the mixed disturbances can be considered as the “superposition” of the single disturbances. The calculating flow chart of the 4 features is shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p>1) <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\53318889-0e0d-4e3d-9b3f-81b54e336ab6.png" xlink:type="simple"/></inline-formula>is taken as a feature after Equation (2) is filtered by a low pass. Because of the (2)’s effect of frequency selection, F<sub>1</sub> is the system fundamental wave voltage amplitude variation value which is not affected by additive disturbance. It reflects the extent of the fundamental wave amplitude change. So the information of system fundamental RMS voltage change can be known from the extent of the F<sub>1</sub> change. Then it can be used to identify whether there are the voltage sag, swell, instantaneous interruption, under voltage, over voltage, continuous interruption, fluctuation and flicker in electrical singles (shown in <xref ref-type="table" rid="table3">Table 3</xref>).</p><p>2)<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\5aae8847-33d6-46f9-8a1f-2a1338bfd619.png" xlink:type="simple"/></inline-formula>. N is the total sample points during the analysis period of time <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\6feba13c-f873-4c4f-8638-71f8eacacedf.png" xlink:type="simple"/></inline-formula></p><p>(for F<sub>2</sub> is used to detect stationary additive disturbances, the analysis period of time can be enlarged. This paper takes<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\5c6eb01d-91ff-4164-9ab7-de6f931f42a3.png" xlink:type="simple"/></inline-formula>, 100 cycles). <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\2f763e46-50f5-4487-b4d4-41957350ede9.png" xlink:type="simple"/></inline-formula>is the RMS value of the additive disturbance during the analysis period of time<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\fae21f9b-bdb5-48b9-b95a-111980bc27f7.png" xlink:type="simple"/></inline-formula>. If<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\4be5402b-ecc7-4877-98a4-b992d7642e77.png" xlink:type="simple"/></inline-formula>, the additive disturbance must exist. If <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\73a456d5-fcf8-40d4-9887-3b095e4a6a7f.png" xlink:type="simple"/></inline-formula> is stationary, the disturbance must be harmonics and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\1785053e-4f0f-4ae0-ac95-ed5d23350eab.png" xlink:type="simple"/></inline-formula> is equivalent to THD. <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\0dfded7c-a085-4a6a-b092-8f6e4b1b9738.png" xlink:type="simple"/></inline-formula>can be the threshold value of the harmonics and interharmonics.</p><p>3) If<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\98b4967d-2878-48da-b385-71737e1b47d1.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\b3898338-80ef-4659-9d7d-574c4b92cf59.png" xlink:type="simple"/></inline-formula>means the average increment of the<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\c27ff1b1-e9e7-439a-801b-5ce581ef7ec6.png" xlink:type="simple"/></inline-formula>. It can be used to</p><p>classify the additive disturbances harmonics and interharmonics. If interharmonics exist in Equation (2), the curve of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\a7342c38-02f4-406c-a3e1-e5a0146c399a.png" xlink:type="simple"/></inline-formula> will contain AC component of non-integer system fundamental frequency (shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>(c)</p><fig id="fig3"><label>Figure 3</label><caption><p> The flow chart of calculating classification features</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\6463c7fe-a6dc-4126-8d82-63339316f952.png"/></fig><table-wrap id="table3"  position="float"><object-id pub-id-type="pii">Table 3</object-id><label>Table 3</label><caption><p>. Amplitude change disturbance classifications with F<sub>1</sub></p></caption><table><thead><tr><th align="center" valign="middle" >c</th><th align="center" valign="middle" >F<sub>1</sub> = 1.1 - 1.2 pu, duration &gt; 1 min</th></tr></thead><tbody><tr><td align="center" valign="middle" >Under voltage</td><td align="center" valign="middle" >F<sub>1</sub> = 0.8 - 0.9 pu, duration &gt; 1 min</td></tr><tr><td align="center" valign="middle" >Voltage interruption</td><td align="center" valign="middle" >F<sub>1</sub> &lt; 0.1 pu, duration: 10 ms - 3 s instantaneous interruption;  3 - 60 s temporary interruption; &gt;60 s power off</td></tr><tr><td align="center" valign="middle" >Voltage sag</td><td align="center" valign="middle" >F<sub>1</sub> = 0.1 - 0.9 pu, duration 10 ms - 1 min</td></tr><tr><td align="center" valign="middle" >Voltage swell</td><td align="center" valign="middle" >F<sub>1</sub> = 1.1 - 1.8 pu, duration 10 ms - 1 min</td></tr><tr><td align="center" valign="middle" >Fluctuation and flicker</td><td align="center" valign="middle" >F<sub>1</sub> is voltage fluctuation in 0.9 - 1.1 pu randomly</td></tr></tbody></table></table-wrap><p>and <xref ref-type="fig" rid="fig1">Figure 1</xref>(e)). Then value of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\a735d590-3a82-485d-a754-d88ca3d23ebe.png" xlink:type="simple"/></inline-formula> is much larger than that when only harmonics exist. The MATLAB simulation shows that when<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\2d2e790c-9df8-4b34-9ffe-816477117663.png" xlink:type="simple"/></inline-formula>, interharmonics exist; when<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\279c5230-4f53-4a45-bcb5-012e61929ee9.png" xlink:type="simple"/></inline-formula>, only interharmonics exist; when<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\9db41022-a932-4b08-993c-1ff98037714a.png" xlink:type="simple"/></inline-formula>, both harmonics and interharmonics exist.</p><p>4)<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\15a8b035-127d-4f7e-93c9-f1e337508d34.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\e47737ca-9af2-4b84-9186-885c6837c6f9.png" xlink:type="simple"/></inline-formula>is the maximum differential value of<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\02737211-8c44-4250-81e0-e54f69c18282.png" xlink:type="simple"/></inline-formula>. The characteristic</p><p>that the amplitude of instantaneous disturbance changes fast determines <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\df95be26-166f-4f26-82c7-169632c36471.png" xlink:type="simple"/></inline-formula> a large number. But to stationary disturbance, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\84976fa7-942d-460c-8370-96ecaa836434.png" xlink:type="simple"/></inline-formula>is small or even zero. The value of F<sub>4</sub> can determine the instantaneous disturbances exist or not. The MATLAB simulation shows that the threshold can be 15. If<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\d40d72a7-8437-403c-9344-83a7be9c42dc.png" xlink:type="simple"/></inline-formula>, the instantaneous disturbance exists; if<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\2224d3c8-b9b7-433e-93a6-f7ce9f096ff0.png" xlink:type="simple"/></inline-formula>, no instantaneous disturbance exists. For instance, when <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\3c989940-91a2-4f7b-b598-f7343f1a3cdd.png" xlink:type="simple"/></inline-formula> shows amplitude disturbance exists, if<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\ac6e4fd4-a057-4bea-a029-7bf79882ccf5.png" xlink:type="simple"/></inline-formula>, the disturbance should be instantaneous amplitude disturbance such as the voltage sag, swell, instantaneous interruption, and if<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\6eb25142-47b9-4440-932f-2c17db36fd6b.png" xlink:type="simple"/></inline-formula>, the disturbance should be stationary amplitude disturbance such as under voltage, over voltage, fluctuation and flicker and when <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\1d3e9124-d795-44b6-a26d-0152e69a4a76.png" xlink:type="simple"/></inline-formula> shows no amplitude disturbance exists, if<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\5eaf31ec-9b7b-408c-9901-f896485918de.png" xlink:type="simple"/></inline-formula>, the disturbance must be the additive instantaneous disturbance such as oscillatory transient.</p><table-wrap id="table4"  position="float"><object-id pub-id-type="pii">Table 1</object-id><label>Table 4 shows the simulation value of 5 single disturbances and 4 mixed disturbances</label><caption><p>. Figure 4 is the flow chart of the automate classification of the disturbances</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink"  xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\446e4eba-0b80-4297-ba8f-edab911a5129.png"/></table-wrap></sec><sec id="s4"><title>4. Discussion</title><p>Comparing with the other power quality disturbance classification methods using some kinds of transforms, the method presented by this paper has advantages as follows:</p><p>1) The single disturbance can be identified by one feature or the combination of some features. That means if one feature or some features satisfied some conditions, a disturbance or mixed disturbances can be sure. Then the disturbance classification will not be probable, but be definitive and the correct rate of the disturbance classification would be very high. And it makes the classification simpler. For example, as shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>, if</p><fig id="fig4"><label>Figure 4</label><caption><p> The flow chart of the automate classification. A: Har- monics + Interharmonics; B: Harmonics; C: Interharmonics; D: No stationary additive disturbance; E:<img src="htmlimages\6-8102085x\752a4585-0df5-47eb-873b-8d8a4c90756a.png" width="191.000003814697" height="34.2499995231628" />?; F: Identify the amplitude disturbances by<img src="htmlimages\6-8102085x\60f04146-2a2c-40ae-a97e-8e8144f34060.png" width="26.5000009536743" height="34.2499995231628" />; G: No amplitude dis- turbance; H:<img src="htmlimages\6-8102085x\c854a9bd-0879-429a-9ca0-dc0ac1144160.png" width="71.7500019073486" height="34.2499995231628" />?; I: Osillatory transients</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\99a7c50b-7c64-4c0c-9ed7-8bedf7f6cceb.png"/></fig><table-wrap id="table5"  position="float"><object-id pub-id-type="pii">Table 5</object-id><label>Table 4</label><caption><p>. The simulation value of the features</p></caption><table><thead><tr><th align="center" valign="middle" >The disturbances</th><th align="center" valign="middle" >The disturbance parameters</th><th align="center" valign="middle" >F<sub>2</sub></th><th align="center" valign="middle" >F<sub>3</sub></th><th align="center" valign="middle" >F<sub>4</sub></th></tr></thead><tbody><tr><td align="center" valign="middle" >Fluctuation and flicker</td><td align="center" valign="middle" >Amplitude: 0.95 - 1.05</td><td align="center" valign="middle" >0.68</td><td align="center" valign="middle" >0. 91</td><td align="center" valign="middle" >1.96</td></tr><tr><td align="center" valign="middle" >Voltage sag</td><td align="center" valign="middle" >Sag amplitude: 0.5 pu</td><td align="center" valign="middle" >0.49</td><td align="center" valign="middle" >0. 40</td><td align="center" valign="middle" >38.66</td></tr><tr><td align="center" valign="middle" >Harmonics</td><td align="center" valign="middle" ><sup>*</sup>5<sup>th</sup> 4%; 7<sup>th</sup> 3%</td><td align="center" valign="middle" >5.0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >Oscillatory transients</td><td align="center" valign="middle" >M<sub>s</sub> = 0.8 pu, f<sub>s</sub> = 1025 Hz; U<sub>s</sub> = 0.1</td><td align="center" valign="middle" >0.49</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" >59.95</td></tr><tr><td align="center" valign="middle" >Interharmonics</td><td align="center" valign="middle" >f = 125 Hz, amplitude 2%</td><td align="center" valign="middle" >1.99</td><td align="center" valign="middle" >1.27</td><td align="center" valign="middle" >1.78</td></tr><tr><td align="center" valign="middle" >Voltage sag and harmonics</td><td align="center" valign="middle" >0.5 pu, 5<sup>th</sup> 4%; 7<sup>th</sup> 3%</td><td align="center" valign="middle" >5.41</td><td align="center" valign="middle" >0. 40</td><td align="center" valign="middle" >39.45</td></tr><tr><td align="center" valign="middle" >Fluctuation and harmonics</td><td align="center" valign="middle" >Amplitude: 0.95 - 1.05; 5<sup>th</sup> 4%; 7<sup>th</sup> 3%</td><td align="center" valign="middle" >5.05</td><td align="center" valign="middle" >0. 91</td><td align="center" valign="middle" >1.31</td></tr><tr><td align="center" valign="middle" >Harmonics and oscillatory transients</td><td align="center" valign="middle" >5<sup>th</sup> 4%; 7<sup>th</sup> 3%, γ<sub>s</sub> = 0.1, U<sub>s</sub> = 0.8 pu, f<sub>s</sub> = 1025 Hz</td><td align="center" valign="middle" >5.34</td><td align="center" valign="middle" >0. 22</td><td align="center" valign="middle" >59.92</td></tr><tr><td align="center" valign="middle" >Harmonics and interharmonics</td><td align="center" valign="middle" >5<sup>th</sup> 4%; 7<sup>th</sup> 3%; f<sub>s</sub> = 125 Hz, U<sub>s</sub> = 2%</td><td align="center" valign="middle" >5.37</td><td align="center" valign="middle" >1.27</td><td align="center" valign="middle" >1.73</td></tr></tbody></table></table-wrap><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\dd4c23bb-d98e-4c02-892a-6b42c6e96402.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\e2a56d46-28e5-46fd-a8df-8ac9b010b128.png" xlink:type="simple"/></inline-formula>, only harmonics exist; if<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\2a7fd699-7ad2-46d1-92f8-7c495b6b5b87.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\2a1c4701-4fe6-4401-b40d-9b54a9a1010a.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\69d52b18-9c70-498c-a109-87a233f5fd62.png" xlink:type="simple"/></inline-formula>, only interharmonics exist; if<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\1ebadb8e-d7bc-4277-9096-47b0bb93e478.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\35fcc216-be0b-4de3-a63c-eb6799690243.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\7b48d026-a1df-40b5-ad89-bb838a7c37c1.png" xlink:type="simple"/></inline-formula>, both harmonics and interharmonics exist.</p><p>2) The features extracted from one disturbance won’t change a lot for the existence of the other disturbance. This is shown clearly in <xref ref-type="table" rid="table4">Table 4</xref>. For example, when the voltage sag and harmonics both exist, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\85e00390-5f53-473e-b1d4-6ccbcad56e1f.png" xlink:type="simple"/></inline-formula>which is used to identify voltage sag won’t change for the existence of harmonics. And <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\b5546fb0-a9bf-47c2-b321-2be038f5e858.png" xlink:type="simple"/></inline-formula> (only harmonics exist,<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\818c8e73-6350-4159-8dac-90aa9e6ec7f3.png" xlink:type="simple"/></inline-formula>), which is used to identify harmonics changes a little by the existence of voltage sag (harmonics + voltage sag,<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\91d0e618-9d1d-4fde-a924-694757ef6b00.png" xlink:type="simple"/></inline-formula>). When the oscillatory transients exist in harmonics, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\98b6c54b-1f89-4589-b18f-efd93adb2831.png" xlink:type="simple"/></inline-formula>increases a little (from 5.0 to 5.23). The harmonics and interharmonics are both additive disturbances, so <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\68ebca7d-e314-4f20-bf11-cfcac519df8f.png" xlink:type="simple"/></inline-formula> is the approximate geometric</p><p>summation of their amplitude (<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\8e2c4dcf-803e-480a-b231-cf2b1a85d343.png" xlink:type="simple"/></inline-formula>, the simulation result in <xref ref-type="table" rid="table4">Table 4</xref> is 5.37). For another ex-</p><p>ample, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\61c2790f-e33d-4b26-9496-78cbe867d0f8.png" xlink:type="simple"/></inline-formula>which is used to identify transient voltage sag <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\c28e73c5-557d-4f90-9035-201531577d67.png" xlink:type="simple"/></inline-formula> and oscillatory transients <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\17703a32-68f1-4a63-95ff-b009a8a80ff1.png" xlink:type="simple"/></inline-formula> will not change a lot for the existence of harmonics (voltage sag + harmonics,<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\4d1c5bcf-3761-40e7-a016-fcf1055f0b52.png" xlink:type="simple"/></inline-formula>; oscillotary + harmonics,<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\c39e4c8e-e1b0-4b63-bacc-cb9425f74a7d.png" xlink:type="simple"/></inline-formula>). This characteristic of the features is the key of the classifying the mixed disturbances. For the idea of this paper considers the mixed disturbances as the “superposition” of the single disturbances. For the characteristics above, all single or mixed disturbances can be classified correctly by simple classifying program, and the classifying results won’t conflict and are definitive.</p><p>3) The classifying features have clear physical meanings. So it profits the evaluation of the power quality disturbance. The physical meaning of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\5a53924e-394d-4468-a3cd-3c35cbdd60ee.png" xlink:type="simple"/></inline-formula> is the per unit value of the system fundamental RMS voltage, so the amplitude of all the voltage amplitude disturbances can be gained from<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\621613e5-7517-46a0-9114-7c8fbd896b2f.png" xlink:type="simple"/></inline-formula>. And the starting time <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\cc14869f-0a38-4c67-837a-51300e003200.png" xlink:type="simple"/></inline-formula> and the ending time <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\5ca26607-7869-4e57-8fb4-0606a239e3b1.png" xlink:type="simple"/></inline-formula> of the transient amplitude disturbance can also be gained from <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\cec6ce26-b9fb-4611-bdf2-a00ea8937919.png" xlink:type="simple"/></inline-formula> (shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>). The physical meaning of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\a3e687e5-5f79-4c63-9630-9ebf879358c2.png" xlink:type="simple"/></inline-formula> is the content of the additive disturbances. So <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\b1e6a93c-2204-46fc-983a-7b465681132f.png" xlink:type="simple"/></inline-formula> gives the content of the harmonics and interharmonics accurately. The oscillatory amplitude and the attenuation constant of the oscillatory transients can be gained by fitted method from <xref ref-type="fig" rid="fig2">Figure 2</xref>(d).</p><p>4) The calculating time is much less, and profits to be used in real-time power quality disturbance classification.</p><p>5) The features extracted are low-pass filtered or the full cycle integral values, so it has good ability of noise proof.</p></sec><sec id="s5"><title>5. Verifications</title><p>Using the proposed power quality disturbance classification method, a PQ monitor is developed based on the TMS320F2812 DSP micro-processor. Semi-physical simulation, lab experiment and field measurement results have verified the proposed method.</p><sec id="s5_1"><title>5.1. Semi-Physical Simulation Results</title><p>The authors use D space semi-physical experiment platform as the disturbance signal generator. The PQ monitor samples the signals generated by D space, identifies disturbances and evaluates their parameters. <xref ref-type="table" rid="table5">Table 5</xref> shows that it identifies the disturbance types correctly and evaluates their parameters accurately.</p><table-wrap id="table6"  position="float"><object-id pub-id-type="pii">Table 6</object-id><label>Table 5</label><caption><p>. The experiments results</p></caption><table><thead><tr><th align="center" valign="middle" >The disturbance type</th><th align="center" valign="middle" >The experiments times</th><th align="center" valign="middle" >The correct ratio of identifying the disturbance type</th><th align="center" valign="middle" >The average error of the parameters evaluation</th></tr></thead><tbody><tr><td align="center" valign="middle" >The voltage sag</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >100%</td><td align="center" valign="middle" >2.12%</td></tr><tr><td align="center" valign="middle" >The fluctuation and flicker</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >99%</td><td align="center" valign="middle" >3.01%</td></tr><tr><td align="center" valign="middle" >The harmonics</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >98%</td><td align="center" valign="middle" >2.00%</td></tr><tr><td align="center" valign="middle" >The oscillatory transients</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >98%</td><td align="center" valign="middle" >2.45%</td></tr><tr><td align="center" valign="middle" >The interharmonics</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >97%</td><td align="center" valign="middle" >6.33%</td></tr><tr><td align="center" valign="middle" >The harmonics + The voltage sag</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >100%</td><td align="center" valign="middle" >3.58%</td></tr><tr><td align="center" valign="middle" >The harmonics + The fluctuation and flicker</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >96%</td><td align="center" valign="middle" >2.99%</td></tr><tr><td align="center" valign="middle" >The harmonics + The oscillatory transients</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >100%</td><td align="center" valign="middle" >3.07%</td></tr><tr><td align="center" valign="middle" >The fluctuation and flicker + The voltage sag</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >100%</td><td align="center" valign="middle" >4.28%</td></tr><tr><td align="center" valign="middle" >The fluctuation and flicker + The oscillatory transients</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >100%</td><td align="center" valign="middle" >4.14%</td></tr><tr><td align="center" valign="middle" >The interharmonics + The voltage sag</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >100%</td><td align="center" valign="middle" >2.78%</td></tr><tr><td align="center" valign="middle" >The interharmonics + The oscillatory transients</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >99%</td><td align="center" valign="middle" >2.99%</td></tr><tr><td align="center" valign="middle" >The interharmonics + The fluctuation and flicker</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >96%</td><td align="center" valign="middle" >3.46%</td></tr><tr><td align="center" valign="middle" >The interharmonics + The harmonics</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >97%</td><td align="center" valign="middle" >2.53%</td></tr><tr><td align="center" valign="middle" >The interharmonics + The harmonics + The voltage sag</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >99%</td><td align="center" valign="middle" >4.01%</td></tr><tr><td align="center" valign="middle" >The interharmonics + The harmonics +  The voltage sag + The fluctuation and flicker</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >98%</td><td align="center" valign="middle" >3.98%</td></tr></tbody></table></table-wrap><p>The authors give three types of disturbances: the voltage sag, the voltage sag plus harmonics, the fluctuation plus harmonics plus interharmonics plus voltage sag to present 5 single disturbances and 11 mixed disturbances.</p><p>1) The voltage sag</p><p>In the following tables the same symbols have the same meanings.</p><p><xref ref-type="table" rid="table6">Table 6</xref> doesn’t give the true or false results because the PQ monitor gives the correct results every time. <xref ref-type="table" rid="table6">Table 6</xref> shows that the PQ monitor can evaluate the voltage sag parameter very well. The relative error is a little big when the voltage sag amplitude is close to the voltage sag threshold value, but the absolute error is not big.</p><p>2) The voltage sag plus harmonics</p><p>The authors do not show the identifying results in <xref ref-type="table" rid="table7">Table 7</xref>, for all harmonics plus voltage sag are identified by the PQ monitor correctly. <xref ref-type="table" rid="table7">Table 7</xref> shows that the superposed disturbance doesn’t make the features change a lot, which means the features F<sub>2</sub> and F<sub>3</sub> are relatively independent. The identifying results and the parameters evaluation are not affected by the superposition of the disturbances.</p><p>3) The fluctuation plus harmonics plus interharmonics plus voltage sag</p><p><xref ref-type="table" rid="table8">Table 8</xref> shows that the addition of the fluctuation and flicker affects the feature F<sub>2</sub> a little, but doesn’t affect the feature F<sub>3</sub>. The big amount of harmonics may blanket the existence of interharmonics, because the identifying term of the harmonics plus interharmonics is F<sub>3</sub>/F<sub>2</sub> &gt; 0.5.</p></sec><sec id="s5_2"><title>5.2. Lab Experiment Results</title><p>A lab experiment circuit is shown as <xref ref-type="fig" rid="fig5">Figure 5</xref>. When the switch S is turned on, there is voltage sag on R<sub>1</sub>. The voltage signal u<sub>1</sub> is sampled by the PQ monitor and the oscilloscope.</p><p>U = 380 V, R<sub>1</sub> = 1 kΩ, R<sub>2</sub> = 2 kΩ, R<sub>3</sub> = 3.9 Ω. S is an AC contact. FU is a fuse. When S is turned on and the current of the FU branch is large enough, the FU will blowing out and the branch will be cut off. Then there will be a voltage sag in u<sub>1 </sub>as shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>(b).</p><p>The experiment results shown in <xref ref-type="table" rid="table9">Table 9</xref> indicate that the PQ monitor can identify disturbances correctly and evaluate the voltage sag lasting time and amplitude accurately.</p><table-wrap id="table7"  position="float"><object-id pub-id-type="pii">Table 7</object-id><label>Table 6</label><caption><p>. The experiments results of voltage sag</p></caption><table><thead><tr><th align="center" valign="middle" >t<sub>m</sub> (ms)</th><th align="center" valign="middle" >t<sub>s</sub> (ms)</th><th align="center" valign="middle" >e<sub>t</sub></th><th align="center" valign="middle" >a<sub>m</sub> (pu)</th><th align="center" valign="middle" >a<sub>s</sub> (pu)</th><th align="center" valign="middle" >e<sub>a</sub></th></tr></thead><tbody><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.112</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >0.012</td></tr><tr><td align="center" valign="middle" >53</td><td align="center" valign="middle" >60</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.211</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.011</td></tr><tr><td align="center" valign="middle" >77</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.305</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >0.005</td></tr><tr><td align="center" valign="middle" >98</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.360</td><td align="center" valign="middle" >0.35</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >116</td><td align="center" valign="middle" >120</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0.389</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.011</td></tr><tr><td align="center" valign="middle" >138</td><td align="center" valign="middle" >140</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.447</td><td align="center" valign="middle" >0.45</td><td align="center" valign="middle" >0.003</td></tr></tbody></table></table-wrap><p>t<sub>m</sub>: The voltage sag lasting time measured by the PQ monitor; t<sub>s</sub>: The setting time of the voltage sag lasting time; e<sub>t</sub>: The error between time 1 and time 2; a<sub>m</sub>: The voltage sag amplitude measured by the PQ monitor; a<sub>s</sub>: The setting amplitude of voltage sag amplitude; e<sub>a</sub>: The error between amplitude 1 and amplitude 2.</p><table-wrap id="table8"  position="float"><object-id pub-id-type="pii">Table 8</object-id><label>Table 7</label><caption><p>. The experiments results of harmonics plus voltage sag</p></caption><table><thead><tr><th align="center" valign="middle" >THD</th><th align="center" valign="middle" >e<sub>THD</sub></th><th align="center" valign="middle" >t<sub>m</sub> (ms)</th><th align="center" valign="middle" >e<sub>t</sub></th><th align="center" valign="middle" >a<sub>m</sub> (pu)</th><th align="center" valign="middle" >e<sub>a</sub></th><th align="center" valign="middle" >F<sub>2</sub></th><th align="center" valign="middle" >F<sub>3</sub></th></tr></thead><tbody><tr><td align="center" valign="middle" >2.08%</td><td align="center" valign="middle" >0.0018</td><td align="center" valign="middle" >38</td><td align="center" valign="middle" >3.52</td><td align="center" valign="middle" >0.102</td><td align="center" valign="middle" >0.011</td><td align="center" valign="middle" >2.08</td><td align="center" valign="middle" >0.04</td></tr><tr><td align="center" valign="middle" >3.12%</td><td align="center" valign="middle" >0.0029</td><td align="center" valign="middle" >54</td><td align="center" valign="middle" >4.76</td><td align="center" valign="middle" >0.212</td><td align="center" valign="middle" >0.011</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >4.09%</td><td align="center" valign="middle" >0.0014</td><td align="center" valign="middle" >78</td><td align="center" valign="middle" >2.60</td><td align="center" valign="middle" >0.307</td><td align="center" valign="middle" >0.005</td><td align="center" valign="middle" >4.09</td><td align="center" valign="middle" >0.02</td></tr><tr><td align="center" valign="middle" >5.06%</td><td align="center" valign="middle" >0.0010</td><td align="center" valign="middle" >98</td><td align="center" valign="middle" >1.93</td><td align="center" valign="middle" >0.361</td><td align="center" valign="middle" >0.010</td><td align="center" valign="middle" >5.06</td><td align="center" valign="middle" >0.13</td></tr><tr><td align="center" valign="middle" >5.97%</td><td align="center" valign="middle" >0.0019</td><td align="center" valign="middle" >115</td><td align="center" valign="middle" >4.77</td><td align="center" valign="middle" >0.387</td><td align="center" valign="middle" >0.010</td><td align="center" valign="middle" >5.97</td><td align="center" valign="middle" >0.05</td></tr></tbody></table></table-wrap><p>e<sub>THD</sub>: The error between the measured THD by PQ monitor and the setting THD.</p><table-wrap id="table9"  position="float"><object-id pub-id-type="pii">Table 9</object-id><label>Table 8</label><caption><p>. The experiments results of voltage fluctuation plus harmonics plus interharmonics plus voltage sag</p></caption><table><thead><tr><th align="center" valign="middle" >The disturbance parameters</th><th align="center" valign="middle" >F<sub>2</sub></th><th align="center" valign="middle" >F<sub>3</sub></th><th align="center" valign="middle" >Results</th><th align="center" valign="middle" >Remarks</th></tr></thead><tbody><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.02, frequency  6 Hz; interharmonics content 2%,frequency 125 Hz;  harmonics THD 2%; voltage sag amplitude 0.4 pu</td><td align="center" valign="middle" >4.72</td><td align="center" valign="middle" >3.75</td><td align="center" valign="middle" >Voltage Fluctuation plus  harmonics plus interharmonics  plus voltage sag</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.03, frequency 8 Hz; interharmonics content 2%,frequency 125 Hz;  harmonics THD 2%; voltage sag amplitude 0.4 pu</td><td align="center" valign="middle" >4.80</td><td align="center" valign="middle" >3.80</td><td align="center" valign="middle" >Voltage fluctuation plus  harmonics plus interharmonics  plus voltage sag</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.02, frequency  6 Hz; interharmonics content 2%,frequency 125 Hz;  harmonics THD 2%; voltage sag amplitude 0.4 pu</td><td align="center" valign="middle" >4.91</td><td align="center" valign="middle" >3.82</td><td align="center" valign="middle" >Voltage fluctuation plus  harmonics plus interharmonics  plus voltage sag</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.05, frequency 6 Hz; interharmonics content 2%,frequency 125 Hz;  harmonics THD 2%; voltage sag amplitude 0.4 pu</td><td align="center" valign="middle" >4.98</td><td align="center" valign="middle" >3.80</td><td align="center" valign="middle" >Voltage fluctuation plus  harmonics plus interharmonics  plus voltage sag</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.02, frequency  6 Hz; interharmonics content 1%,frequency 125 Hz;  harmonics THD 2%; voltage sag amplitude 0.4 pu</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >1.07</td><td align="center" valign="middle" >Voltage fluctuation plus  harmonics plus voltage sag</td><td align="center" valign="middle" >When the interharmonics  content is lower than 1%,  and the harmonics content is large, the error is a little large</td></tr><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.02, frequency  6 Hz; interharmonics content 2%,frequency 1245 Hz;  harmonics THD 2%; voltage sag amplitude 0.4 pu</td><td align="center" valign="middle" >4.21</td><td align="center" valign="middle" >3.68</td><td align="center" valign="middle" >Voltage fluctuation plus  harmonics plus interharmonics  plus voltage sag</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.02, frequency  6 Hz; interharmonics content 2%,frequency 125 Hz;  harmonics THD 3%; voltage sag amplitude 0.4 pu</td><td align="center" valign="middle" >5.25</td><td align="center" valign="middle" >3.71</td><td align="center" valign="middle" >Voltage fluctuation plus  harmonics plus interharmonics  plus voltage sag</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.02, frequency  6 Hz; interharmonics content 2%,frequency 125 Hz;  harmonics THD 5%; voltage sag amplitude 0.5 pu</td><td align="center" valign="middle" >7.27</td><td align="center" valign="middle" >3.75</td><td align="center" valign="middle" >Voltage fluctuation plus  harmonics plus interharmonics  plus voltage sag</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.02, frequency  6 Hz; interharmonics content 2%,frequency 125 Hz;  harmonics THD 2%; voltage sag amplitude 0.7 pu</td><td align="center" valign="middle" >4.05</td><td align="center" valign="middle" >3.69</td><td align="center" valign="middle" >Voltage fluctuation plus  harmonics plus interharmonics  plus voltage sag</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Fluctuation modulating wave amplitude 0.02, frequency  6 Hz; interharmonics content 2%,frequency 125 Hz;  harmonics THD 2%; voltage sag amplitude 0.8 pu</td><td align="center" valign="middle" >4.11</td><td align="center" valign="middle" >3.70</td><td align="center" valign="middle" >Voltage fluctuation plus  harmonics plus interharmonics  plus voltage sag</td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table10"  position="float"><object-id pub-id-type="pii">Table 10</object-id><label>Table 9</label><caption><p>. The voltage sag experiments results comparison table</p></caption><table><thead><tr><th align="center" valign="middle" >Identifying results</th><th align="center" valign="middle" >t<sub>m</sub> (ms)</th><th align="center" valign="middle" >t<sub>om</sub> (ms)</th><th align="center" valign="middle" >e<sub>t</sub></th><th align="center" valign="middle" >a<sub>m</sub> (pu)</th><th align="center" valign="middle" >a<sub>om</sub> (pu)</th><th align="center" valign="middle" >e<sub>a</sub></th></tr></thead><tbody><tr><td align="center" valign="middle" >Voltage sag</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >102</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.842</td><td align="center" valign="middle" >0.854</td><td align="center" valign="middle" >0.012</td></tr><tr><td align="center" valign="middle" >Voltage sag</td><td align="center" valign="middle" >102</td><td align="center" valign="middle" >105</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.838</td><td align="center" valign="middle" >0.833</td><td align="center" valign="middle" >0.005</td></tr><tr><td align="center" valign="middle" >Voltage sag</td><td align="center" valign="middle" >101</td><td align="center" valign="middle" >103</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.857</td><td align="center" valign="middle" >0.872</td><td align="center" valign="middle" >0.015</td></tr><tr><td align="center" valign="middle" >Voltage sag</td><td align="center" valign="middle" >108</td><td align="center" valign="middle" >110</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.813</td><td align="center" valign="middle" >0.801</td><td align="center" valign="middle" >0.012</td></tr><tr><td align="center" valign="middle" >Voltage sag</td><td align="center" valign="middle" >113</td><td align="center" valign="middle" >114</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.839</td><td align="center" valign="middle" >0.825</td><td align="center" valign="middle" >0.014</td></tr></tbody></table></table-wrap><p>a: Error means the difference between values evaluated by PQ monitor and ones measured by the oscilloscope. For the oscilloscope measured value has error itself, but here, no error is considered. The meaning of error in the other tables is the same.</p></sec><sec id="s5_3"><title>5.3. Field Measurement Results</title><p>A PQ monitor is equipped to a steel pipe factory substation to monitor the harmonics disturbance and the oscillatory transient disturbances. The results are shown in <xref ref-type="table" rid="table10">Table 10</xref> and <xref ref-type="table" rid="table11">Table 11</xref>.</p><p>The field monitoring results in <xref ref-type="table" rid="table10">Table 10</xref> show that the PQ monitor identifies harmonics correctly and evaluates the THD accurately.</p><p>To catch the oscillatory transients, a PQ monitor is equipped to Shi-Qiao substation. The oscillatory transient signals are generated by switching three phase capacitors. The three phase voltage waveform is shown as <xref ref-type="fig" rid="fig6">Figure 6</xref>.</p><fig-group id="fig5"> <caption><title>Figure 5</title><p> The voltage sag experiment. (a) The voltage sag experiment circuit; (b) The waveform of u<sub>1</sub></p></caption><fig id ="fig5_1"><label>(a)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\3a2a1af6-4853-47b4-82cc-c97fcad3b2fa.png"/></fig><fig id ="fig5_2"><label>(b)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\621ee1f1-4bdb-4060-ac28-c2c28a5f57bf.png"/></fig></fig-group><fig id="fig6"><label>Figure 6</label><caption><p> The three phase voltage waveform of capacitors switching in Shi-Qiao substation</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\6-8102085x\c2a21e5c-84a4-4af3-9024-145031568da4.png"/></fig><table-wrap id="table11"  position="float"><object-id pub-id-type="pii">Table 11</object-id><label>Table 10</label><caption><p>. The harmonics experiments results comparison table</p></caption><table><thead><tr><th align="center" valign="middle" >Identifying results</th><th align="center" valign="middle" >THD<sub>m</sub></th><th align="center" valign="middle" >THD<sub>om</sub></th><th align="center" valign="middle" >Error</th></tr></thead><tbody><tr><td align="center" valign="middle" >Harmonics</td><td align="center" valign="middle" >4.2%</td><td align="center" valign="middle" >4.4%</td><td align="center" valign="middle" >0.0020</td></tr><tr><td align="center" valign="middle" >Harmonics</td><td align="center" valign="middle" >5.0%</td><td align="center" valign="middle" >5.2%</td><td align="center" valign="middle" >0.0020</td></tr><tr><td align="center" valign="middle" >Harmonics</td><td align="center" valign="middle" >4.8%</td><td align="center" valign="middle" >5.0%</td><td align="center" valign="middle" >0.0020</td></tr><tr><td align="center" valign="middle" >Harmonics</td><td align="center" valign="middle" >4.5%</td><td align="center" valign="middle" >4.8%</td><td align="center" valign="middle" >0.0030</td></tr><tr><td align="center" valign="middle" >Harmonics</td><td align="center" valign="middle" >5.7%</td><td align="center" valign="middle" >6%</td><td align="center" valign="middle" >0.0030</td></tr></tbody></table></table-wrap><p>THD<sub>m</sub>: THD measured by the PQ monitor; THD<sub>om</sub>: THD measured by the oscilloscope.</p><table-wrap id="table12"  position="float"><object-id pub-id-type="pii">Table 12</object-id><label>Table 11</label><caption><p>. The experiments results of oscillatory transient in Shi-Qiao substation</p></caption><table><thead><tr><th align="center" valign="middle" >Identifying results</th><th align="center" valign="middle" >t<sub>m</sub> (ms)</th><th align="center" valign="middle" >t<sub>om</sub> (ms)</th><th align="center" valign="middle" >Error</th><th align="center" valign="middle" >a<sub>m</sub> (pu)</th><th align="center" valign="middle" >a<sub>om</sub> (pu)</th><th align="center" valign="middle" >Error</th></tr></thead><tbody><tr><td align="center" valign="middle" >Oscillatory transients</td><td align="center" valign="middle" >12.43</td><td align="center" valign="middle" >12.56</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.78</td><td align="center" valign="middle" >0.08</td></tr><tr><td align="center" valign="middle" >Oscillatory transients</td><td align="center" valign="middle" >13.56</td><td align="center" valign="middle" >13.63</td><td align="center" valign="middle" >0.070</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >0.82</td><td align="center" valign="middle" >0.07</td></tr><tr><td align="center" valign="middle" >Oscillatory transients</td><td align="center" valign="middle" >14.28</td><td align="center" valign="middle" >14.39</td><td align="center" valign="middle" >0.11</td><td align="center" valign="middle" >0.78</td><td align="center" valign="middle" >0.79</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >Oscillatory transients</td><td align="center" valign="middle" >12.85</td><td align="center" valign="middle" >12.98</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >0.74</td><td align="center" valign="middle" >0.85</td><td align="center" valign="middle" >0.11</td></tr><tr><td align="center" valign="middle" >Oscillatory transients</td><td align="center" valign="middle" >14.50</td><td align="center" valign="middle" >14.01</td><td align="center" valign="middle" >0.49</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >0.93</td><td align="center" valign="middle" >0.05</td></tr></tbody></table></table-wrap><p>t<sub>om</sub>: The oscillatory transients lasting time measured by the oscilloscope; a<sub>om</sub>: The oscillatory transients amplitude measured by the oscilloscope.</p><p>The author takes one phase wave to analyze (the purple one). The field experiment results are shown in <xref ref-type="table" rid="table11">Table 11</xref>.</p><p><xref ref-type="table" rid="table11">Table 11</xref> shows that the PQ monitor identifies the oscillatory transients correctly and evaluates their parameters accurately. The difference between the values evaluated by the PQ monitor and ones measured by oscilloscope is small.</p></sec></sec><sec id="s6"><title>6. Conclusion</title><p>Comparing with analyzing power quality disturbance signals in frequency domain, the method presented by this paper has some advantages. First, if one feature or some features satisfied some conditions, a disturbance or mixed disturbances can be sure. That is to say, the disturbance classification would not be probable, but be definitive. Second, the features extracted won’t change a lot for the existence of the other disturbances. This characteristic is the key of classifying the mixed disturbances. Third, the features have clear physical meanings. So it profits the evaluation of the disturbance parameters.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.46715-ref1"><label>1</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>HEYDT</surname><given-names> G.T.</given-names></name>,<name name-style="western"><surname> FJELD</surname><given-names> P.S.</given-names></name>,<name name-style="western"><surname> LIU</surname><given-names> C.C.</given-names></name>,<name name-style="western"><surname> ET AL. </surname><given-names>  </given-names></name>,<etal>et al</etal>. (<year>1999</year>)<article-title>APPLICATIONS OF THE WINDOW FFT TO ELECTRIC POWER QUALITY ASSESSMENT</article-title><source> IEEE TRANSACTIONS ON POWER DELIVERY</source><volume> 14</volume>,<fpage> 1411</fpage>-<lpage>1416</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/61.796235</pub-id></mixed-citation></ref><ref id="scirp.46715-ref2"><label>2</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>GAING</surname><given-names> Z.-L. </given-names></name>,<etal>et al</etal>. (<year>2004</year>)<article-title>WAVELET-BASED NEURAL NETWORK FOR POWER DISTURBANCE RECOGNITION AND CLASSIFICATION</article-title><source> IEEE TRANSACTIONS ON POWER DELIVERY</source><volume> 19</volume>,<fpage> 1560</fpage>-<lpage>1568</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/TPWRD.2004.835281</pub-id></mixed-citation></ref><ref id="scirp.46715-ref3"><label>3</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>ECE</surname><given-names> D.G. </given-names></name>,<name name-style="western"><surname> GEREK</surname><given-names> O.N. </given-names></name>,<etal>et al</etal>. (<year>2004</year>)<article-title>POWER QUALITY EVENT DETECTION USING JOINT 2-D-WAVELET SUBSPACES</article-title><source> IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENTS</source><volume> 53</volume>,<fpage> 1040</fpage>-<lpage>1046</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/TIM.2004.831137</pub-id></mixed-citation></ref><ref id="scirp.46715-ref4"><label>4</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>CHILUKURI</surname><given-names> M.V. </given-names></name>,<name name-style="western"><surname> DASH</surname><given-names> P.K. </given-names></name>,<etal>et al</etal>. (<year>2004</year>)<article-title>MULTIRESOLUTION S-TRANSFORM-BASED FUZZY RECOGNITION SYSTEM FOR POWER QUALITY EVENTS</article-title><source> IEEE TRANSACTIONS ON POWER DELIVERY</source><volume> 19</volume>,<fpage> 323</fpage>-<lpage>330</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/TPWRD.2003.820180</pub-id></mixed-citation></ref><ref id="scirp.46715-ref5"><label>5</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>GAOUDA</surname><given-names> A.M.</given-names></name>,<name name-style="western"><surname> SALAMA</surname><given-names> M.M.A.</given-names></name>,<name name-style="western"><surname> SULTAN</surname><given-names> M.K. </given-names></name>,<name name-style="western"><surname> CHIKHANI</surname><given-names> A.Y. </given-names></name>,<etal>et al</etal>. (<year>1999</year>)<article-title>POWER QUALITY DETECTION AND CLASSIFICATION USING WAVELET-MULTIRESOLUTION SIGNAL DECOMPOSITION</article-title><source> IEEE TRANSACTIONS ON POWER DELIVERY</source><volume> 14</volume>,<fpage> 1469</fpage>-<lpage>1476</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/61.796242</pub-id></mixed-citation></ref><ref id="scirp.46715-ref6"><label>6</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>SANTOSO</surname><given-names> S.</given-names></name>,<name name-style="western"><surname> POWERS</surname><given-names> E.J.</given-names></name>,<name name-style="western"><surname> GRADY</surname><given-names> W.M. </given-names></name>,<name name-style="western"><surname> HOFMANN</surname><given-names> P. </given-names></name>,<etal>et al</etal>. (<year>1996</year>)<article-title>POWER QUALITY ASSESSMENT VIA WAVELET TRANSFORM ANALYSIS</article-title><source> IEEE TRANSACTIONS ON POWER DELIVERY</source><volume> 11</volume>,<fpage> 924</fpage>-<lpage>930</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/61.489353</pub-id></mixed-citation></ref><ref id="scirp.46715-ref7"><label>7</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>DASH</surname><given-names> P.K.</given-names></name>,<name name-style="western"><surname> PANIGRAHI</surname><given-names> B.K. </given-names></name>,<name name-style="western"><surname> P</surname><given-names>A</given-names></name>,<name name-style="western"><surname> G. </surname><given-names>  </given-names></name>,<etal>et al</etal>. (<year>2003</year>)<article-title>POWER QUALITY ANALYSIS USING S-TRANSFORM</article-title><source> IEEE TRANSACTIONS ON POWER DELIVERY</source><volume> 18</volume>,<fpage> 406</fpage>-<lpage>411</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/TPWRD.2003.809616</pub-id></mixed-citation></ref><ref id="scirp.46715-ref8"><label>8</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>STOCKWELL</surname><given-names> R.G.</given-names></name>,<name name-style="western"><surname> MANSINHA</surname><given-names> L. </given-names></name>,<name name-style="western"><surname> LOWE</surname><given-names> R.P. </given-names></name>,<etal>et al</etal>. (<year>1996</year>)<article-title>LOCALIZATION OF THE COMPLEX SPECTRUM THE S TRANSFORM</article-title><source> IEEE TRANSACTIONS ON SIGNAL PROCESSING</source><volume> 44</volume>,<fpage> 998</fpage>-<lpage>1001</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/78.492555</pub-id></mixed-citation></ref><ref id="scirp.46715-ref9"><label>9</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>AXELBERG</surname><given-names> P.G.V.</given-names></name>,<name name-style="western"><surname> GU</surname><given-names> I.Y.-H. </given-names></name>,<name name-style="western"><surname> BOLLEN</surname><given-names> M.H.J. </given-names></name>,<etal>et al</etal>. (<year>2007</year>)<article-title>SUPPORT VECTOR MACHINE FOR CLASSIFICATION OF VOLTAGE DISTURBANCES</article-title><source> IEEE TRANSACTIONS ON POWER DELIVERY</source><volume> 22</volume>,<fpage> 1297</fpage>-<lpage>1303</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/TPWRD.2007.900065</pub-id></mixed-citation></ref><ref id="scirp.46715-ref10"><label>10</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>MISHRA</surname><given-names> S.</given-names></name>,<name name-style="western"><surname> BHENDE</surname><given-names> C.N. </given-names></name>,<name name-style="western"><surname> PANIGRAHI</surname><given-names> B.K. </given-names></name>,<etal>et al</etal>. (<year>2008</year>)<article-title>DETECTION AND CLASSIFICATION OF POWER QUALITY DISTURBANCES USING S-TRANSFORM AND PROBABILISTIC NEURAL NETWORK</article-title><source> IEEE TRANSACTIONS ON POWER DELIVERY</source><volume> 23</volume>,<fpage> 280</fpage>-<lpage>287</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/TPWRD.2007.911125</pub-id></mixed-citation></ref><ref id="scirp.46715-ref11"><label>11</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>ZHAO</surname><given-names> F.Z. </given-names></name>,<name name-style="western"><surname> YANG</surname><given-names> R.G. </given-names></name>,<etal>et al</etal>. (<year>2007</year>)<article-title>POWER-QUALITY DISTURBANCE RECOGNITION USING S-TRANSFORM</article-title><source> IEEE TRANSACTIONS ON POWER DELIVERY</source><volume> 22</volume>,<fpage> 944</fpage>-<lpage>950</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1109/TPWRD.2006.881575</pub-id></mixed-citation></ref><ref id="scirp.46715-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">IEEE STD 1159-1995 (1995) IEEE RECOMMENDED PRACTICE FOR MONITORING ELECTRIC POWER QUALITY.</mixed-citation></ref></ref-list></back></article>