<?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.2015.75024</article-id><article-id pub-id-type="publisher-id">ENG-56648</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>
 
 
  The Low-Frequency Oscillation Restrain Method Research of Converter-Fed Multi-Phase Induction Motor Propulsion system
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>aiyan</surname><given-names>Zeng</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>Mingzhong</surname><given-names>Qiao</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Peng</surname><given-names>Zhu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Electric Engineering, Naval University of Engineering, Wuhan, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>guicaitang@163. com(AZ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>06</day><month>05</month><year>2015</year></pub-date><volume>07</volume><issue>05</issue><fpage>272</fpage><lpage>284</lpage><history><date date-type="received"><day>31</day>	<month>March</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>23</month>	<year>May</year>	</date><date date-type="accepted"><day>26</day>	<month>May</month>	<year>2015</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>
 
 
  The inverter-fed induction motor drive system may become unstable at low frequencies and light load, and phase current and speed of the induction motor may oscillate periodically, which will threaten safety and reliability of the system. This paper chooses nine-phase induction motor simulated propulsion system as the research object, small disturbance model of three-phase induction motor is built, and average equivalent model of the converter is built by introducing switch function. On the basis above, small disturbance mathematic model of the whole system is obtained. As for the limitation of parameters adjustment method of restrain low-frequency oscillation, the restrain method combining current close-loop with dead-time compensation is put forward. Finally, the proposed restrain method is verified respectively on the built simulation and experimental analogue platform. And the simulation and experimental results indicate that the proposed method can not only satisfy the requirement of low-frequency oscillation restraining, but also be expanded widely, and the stability of the system can get improved greatly.
 
</p></abstract><kwd-group><kwd>Induction Motor Propulsion System</kwd><kwd> Low Frequency Oscillation</kwd><kwd> Small Disturbance Model</kwd><kwd>  Restrain Method</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>For the industrial application of induction motor system powered by inverters, the oscillation phenomenon existed in many low frequency situations. Regular inverter-powered induction motor system usually worked at 50 Hz, and in this situation the oscillation problem could be solved by frequency-skip method. But it is not suitable for electrical propelling in ship, whose propulsion motor is designed to work at low speed and frequency. The low frequency oscillation problem threatened the safety of crew and equipments [<xref ref-type="bibr" rid="scirp.56648-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.56648-ref2">2</xref>] .</p><p>Some papers have studied the reasons of low frequency oscillation. Reference [<xref ref-type="bibr" rid="scirp.56648-ref3">3</xref>] regarded the exchange between filter device and motor magnetic field as the reason, and its author established the small-signal model of inverter-powered induction motor and analyzed the influence from motor and filter parameters to system stability. And on the basis of this method, many other references studied the oscillation problem in various aspects [<xref ref-type="bibr" rid="scirp.56648-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.56648-ref9">9</xref>] . But until now the researchers around the world do not make an agreement on the oscillation problem.</p><p>Although the reason of low frequency oscillation is not clear until now, researchers still work out some methods to restrain this problem. Just as said in reference [<xref ref-type="bibr" rid="scirp.56648-ref10">10</xref>] , the method of regulating stator frequency is used, and when the motor speeds up, input frequency and power are all decreased and when the motor speeds down, input frequency and power are all increased, and the system oscillation is restrained. The shortage of this method is that the control parameters need to be adjusted constantly. Reference [<xref ref-type="bibr" rid="scirp.56648-ref11">11</xref>] provided a method called “DPWM” regulate strategy, and this method was effective in some occurrence, but could not be applied in all working ranges. In addition, references [<xref ref-type="bibr" rid="scirp.56648-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.56648-ref12">12</xref>] weakened the oscillation using dead zone compensation method, but it was difficult to restrain the oscillation in a widen speed range.</p><p>In this paper, the mathematical model of inverter-induction motor system is established, the small-signal model is analyzed, and the influence from dead zone to system is discussed. In addition, aimed at the characteristic of inverter, the oscillation restrain strategy based on current closed loop and dead zone compensation is presented. At the end of this paper, the strategy given above is verified through simulation and experiment, which suggest the effectiveness and prosperity of this method.</p></sec><sec id="s2"><title>2. Small Signal Model of Induction Motor Powered by Inverter</title><p>In this paper, a 9-phase induction motor system is studied, and its system structure is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The system consists of rectifier, LC filter, 9-phase inverter and 9-phase induction motor. In <xref ref-type="fig" rid="fig1">Figure 1</xref>, DZ<sub>1</sub>~DZ<sub>6</sub> are diodes of 3-phase rectifier unit; Lf and Cf are filter inductance and capacitance on the DC output side; VT<sub>1</sub>~ VT<sub>6</sub> are switches in a 3-phase inverter unit.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Structure of converter-fed nine-phase induction motor variable-frequency driven system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x5.png"/></fig><sec id="s2_1"><title>2.1. Mathematical Model of 9-Phase Induction Motor</title><p>The stator winding of 9-phase induction motor is composed by three 3-phase windings, and each 3-phase winding is apart from others with 20 degree. The rotor can be equaled with 3-phase winding. The relationship between stator and rotor winding is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>Considering the convenience for analysis, transform matrix is introduced, and the formulation in natural coordinate system is transformed into de-coupling form. Transform matrix in stator side is as follows:</p><disp-formula id="scirp.56648-formula2266"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x6.png"  xlink:type="simple"/></disp-formula><p>Its backwards matrix is:</p><disp-formula id="scirp.56648-formula2267"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x7.png"  xlink:type="simple"/></disp-formula><p>which,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x8.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x9.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x10.png" xlink:type="simple"/></inline-formula>.</p><p>We can obtain the formulations of induction motor as follows:</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Position relationship of nine-phase induction motor between stator and rotor</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x11.png"/></fig><p>1) Flux formulation:</p><disp-formula id="scirp.56648-formula2268"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x12.png"  xlink:type="simple"/></disp-formula><p>which,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x13.png" xlink:type="simple"/></inline-formula>, ,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x15.png" xlink:type="simple"/></inline-formula>, ,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x17.png" xlink:type="simple"/></inline-formula>, , ,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x20.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x21.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x22.png" xlink:type="simple"/></inline-formula>, ,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x25.png" xlink:type="simple"/></inline-formula>.</p><p>2) Voltage formulation:</p><disp-formula id="scirp.56648-formula2269"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x26.png"  xlink:type="simple"/></disp-formula><p>which</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x27.png" xlink:type="simple"/></inline-formula>, ,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x29.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x30.png" xlink:type="simple"/></inline-formula>, ,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x32.png" xlink:type="simple"/></inline-formula>.</p><p>3) Torque formulation:</p><disp-formula id="scirp.56648-formula2270"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x33.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_2"><title>2.2. Small Signal Model of Induction Motor</title><p>The 9-phase induction motor in this paper can be regarded as three individual 3-phase windings, and through controlling 3-phase winding, the control of 9-phase induction motor can be realized. So it is convenient to start with small-signal model of 3-phase induction motor to analyze the 9-phase motor.</p><p>The mathematical model in d-q coordinate system of single 3-phase motor is as follows:</p><disp-formula id="scirp.56648-formula2271"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x34.png"  xlink:type="simple"/></disp-formula><p>Make the p in formula (6) equal to 0, and we can obtain the following result:</p><disp-formula id="scirp.56648-formula2272"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x35.png"  xlink:type="simple"/></disp-formula><p>When disturbing signal is applied at stable working point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x36.png" xlink:type="simple"/></inline-formula>, the system parameters would generate some gain nearby the stable working point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x37.png" xlink:type="simple"/></inline-formula>. So we can obtain formulation (8):</p><disp-formula id="scirp.56648-formula2273"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x38.png"  xlink:type="simple"/></disp-formula><p>which, Δ means the variable quantity gain at small disturbance.</p><p>By solving formulation (9), we can obtain the small disturbance model of single 3-phase induction motor as follow:</p><disp-formula id="scirp.56648-formula2274"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x39.png"  xlink:type="simple"/></disp-formula><p>which:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x40.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x41.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x42.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.56648-formula2275"><graphic  xlink:href="http://html.scirp.org/file/7-8102368x43.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_3"><title>2.3. Small Signal Model of Inverter</title><p>By introducing switch function, inverter can be equivalent as voltage source or current source circuit, and its mathematical model can be further transformed in d-q coordinate system, which is shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. In the figure above, d<sub>d</sub> and d<sub>q</sub> are duty function of inverter switch device in d-q rotating coordinate system.</p><p>Suppose the phase voltage of stator winding a<sub>s</sub> is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x44.png" xlink:type="simple"/></inline-formula>, and it is easy to obtain follow result, namely<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x45.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x46.png" xlink:type="simple"/></inline-formula>.</p><p>From <xref ref-type="fig" rid="fig3">Figure 3</xref>, we can obtain the small signal model of inverter as follows:</p><disp-formula id="scirp.56648-formula2276"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x47.png"  xlink:type="simple"/></disp-formula><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Average model of three-phase converter</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x48.png"/></fig><p>In which<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x49.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x50.png" xlink:type="simple"/></inline-formula></p><p>Suppose the DC voltage is constant, namely<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x51.png" xlink:type="simple"/></inline-formula>, and we can get:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x52.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x53.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x54.png" xlink:type="simple"/></inline-formula>.</p><p>The small signal model of inverter can be further expressed as:</p><disp-formula id="scirp.56648-formula2277"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x55.png"  xlink:type="simple"/></disp-formula><p>In actual system, formula (11) can be simplified as follows:</p><disp-formula id="scirp.56648-formula2278"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x56.png"  xlink:type="simple"/></disp-formula><p>Dead time t<sub>d</sub> need to be set in order to avoid that the two switches in the same bridge of inverter open at the same time. When the switch frequency is pretty high, deviation voltage <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x57.png" xlink:type="simple"/></inline-formula> could be decomposed and its fundamental component is:</p><disp-formula id="scirp.56648-formula2279"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x58.png"  xlink:type="simple"/></disp-formula><p>In the rotating system, deviation voltage of inverter caused by dead time effect is:</p><disp-formula id="scirp.56648-formula2280"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x59.png"  xlink:type="simple"/></disp-formula><p>The dead time can be regarded as cascading a resistance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x60.png" xlink:type="simple"/></inline-formula> in stator winding:</p><disp-formula id="scirp.56648-formula2281"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x61.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_4"><title>2.4. Small Signal Model of Induction Motor System</title><p>On the basis above, we can obtain the state formulation of 3-phase unit as follow:</p><disp-formula id="scirp.56648-formula2282"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x62.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56648-formula2283"><graphic  xlink:href="http://html.scirp.org/file/7-8102368x63.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56648-formula2284"><graphic  xlink:href="http://html.scirp.org/file/7-8102368x64.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s3"><title>3. Low Frequency Oscillation Restrain of Induction System</title><p>Parameter match of motor and inverter is the main reason to cause low frequency oscillation of system. Two kinds of methods are available: 1) adjusting motor parameters (such as stator resistance and inductance) to weaken system oscillation; 2) dead time compensation can be adopted to make the output voltage more ideal. However, the methods above can only weaken the oscillation but cannot eliminate it.</p><p>After analyzing lots of low frequency oscillation phenomenon of induction motor system, we can conclude that the characteristic of this phenomenon is the period variation of stator phase current and line-line voltage. Aiming at the characteristics of low frequency oscillation and influence from inverter dead time to system stability, this paper presents the restrain policy, which is based on current closed loop and dead time compensation.</p><sec id="s3_1"><title>3.1. Dead Time Compensation Based on Current Feed Back</title><p>The error voltage expression of 3-phase unit in α-β coordinate system is given in formula (18):</p><disp-formula id="scirp.56648-formula2285"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x65.png"  xlink:type="simple"/></disp-formula><p>The error voltage vector in α-β coordinate system is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>. The current vector plane is divided into 6 sectors (I~VI), corresponding with 6 output voltage error vector ΔU<sub>s</sub> (001~110).</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Relationship between current polarity and dead-time error voltage</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x66.png"/></fig><p>According to the sector of current vector, output voltage vector is compensated to offset the influence of dead time effect. <xref ref-type="table" rid="table1">Table 1</xref> gives the relationship between stator current <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x67.png" xlink:type="simple"/></inline-formula> and voltage vector (ΔU<sub>s</sub>) and output error voltage<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-8102368x68.png" xlink:type="simple"/></inline-formula>.</p><p>The way to judge sector of current vector is:</p><disp-formula id="scirp.56648-formula2286"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-8102368x69.png"  xlink:type="simple"/></disp-formula><p>From <xref ref-type="table" rid="table1">Table 1</xref>, we know that in order to get compensation voltage, stator current polarity must be judged correctly. If we judge the current polarity by detecting stator current directly, the error would be quite large. To avoid this risk, this paper provides a new method, which combines the coordinate transformation with low pass filter. Its theory chart is given in <xref ref-type="fig" rid="fig5">Figure 5</xref>.</p><p>The detected 3-phase unit phase current is transformed into d-q coordinate system to get i<sub>ds</sub> and i<sub>qs</sub> components, which are filtered to get DC component (i<sub>dfs</sub> and i<sub>qfs</sub>) of stator current. Then, i<sub>dfs</sub> and i<sub>qfs</sub> are transformed in natural coordinate system to obtain phase current i<sub>afs</sub>, i<sub>bfs</sub> and i<sub>cfs</sub>. In the end, according to filtered current polarity, output voltage is compensated.</p></sec><sec id="s3_2"><title>3.2. Low Frequency Oscillation Restrain Strategy</title><p><xref ref-type="fig" rid="fig6">Figure 6</xref> is theory picture of low frequency oscillation restrain strategy, which combines closed current loop and dead time compensation. There is no speed loop of rotor in this method, so it is actually a open loop to some degree, but it can be easily realized and has a good effect.</p></sec></sec><sec id="s4"><title>4. Simulation and Experiment</title><p>In order to imitate real ship propulsion and verify the effectiveness of restrain strategy proposed above, test platform of electrical ship propulsion system is designed and manufactured, and the test experiment concludes generator unit, 9-phase inverter, 400 kW 9-phase induction motor and power measurement in <xref ref-type="fig" rid="fig7">Figure 7</xref>.</p><p>Parameters of multi-phase induction motor propulsion system are shown in <xref ref-type="table" rid="table2">Table 2</xref>.</p><sec id="s4_1"><title>4.1. Simulation</title><p>A 3-phase unit in the 9-phase induction motor system is chosen to be analyzed, and the fundamental frequency is 10 Hz. The system has no load, in which situation it is more likely to oscillate. <xref ref-type="fig" rid="fig8">Figure 8</xref>(a) shows the system simulation results with no restrain measure. <xref ref-type="fig" rid="fig8">Figure 8</xref>(b) shows the system experiment results with the restrain</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Schematic diagram of current polarity identification</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x70.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Relationship between current vector and error voltage vector</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Current vector sector</th><th align="center" valign="middle"  colspan="3"  >Current pole</th><th align="center" valign="middle"  rowspan="2"  >Δu<sub>sa</sub></th><th align="center" valign="middle"  rowspan="2"  >Δu<sub>sb</sub></th><th align="center" valign="middle"  rowspan="2"  >Δu<sub>sc</sub></th><th align="center" valign="middle"  rowspan="2"  >ΔU<sub>s</sub></th></tr></thead><tr><td align="center" valign="middle" >i<sub>sa</sub></td><td align="center" valign="middle" >i<sub>sb</sub></td><td align="center" valign="middle" >i<sub>sc</sub></td></tr><tr><td align="center" valign="middle" >I</td><td align="center" valign="middle" >+</td><td align="center" valign="middle" >−</td><td align="center" valign="middle" >−</td><td align="center" valign="middle" >−U<sub>ε</sub></td><td align="center" valign="middle" >U<sub>ε</sub></td><td align="center" valign="middle" >U<sub>ε</sub></td><td align="center" valign="middle" >011</td></tr><tr><td align="center" valign="middle" >II</td><td align="center" valign="middle" >−</td><td align="center" valign="middle" >+</td><td align="center" valign="middle" >−</td><td align="center" valign="middle" >U<sub>ε</sub></td><td align="center" valign="middle" >−U<sub>ε</sub></td><td align="center" valign="middle" >U<sub>ε</sub></td><td align="center" valign="middle" >101</td></tr><tr><td align="center" valign="middle" >III</td><td align="center" valign="middle" >+</td><td align="center" valign="middle" >+</td><td align="center" valign="middle" >−</td><td align="center" valign="middle" >−U<sub>ε</sub></td><td align="center" valign="middle" >−U<sub>ε</sub></td><td align="center" valign="middle" >U<sub>ε</sub></td><td align="center" valign="middle" >001</td></tr><tr><td align="center" valign="middle" >IV</td><td align="center" valign="middle" >−</td><td align="center" valign="middle" >−</td><td align="center" valign="middle" >+</td><td align="center" valign="middle" >U<sub>ε</sub></td><td align="center" valign="middle" >U<sub>ε</sub></td><td align="center" valign="middle" >−U<sub>ε</sub></td><td align="center" valign="middle" >110</td></tr><tr><td align="center" valign="middle" >V</td><td align="center" valign="middle" >+</td><td align="center" valign="middle" >−</td><td align="center" valign="middle" >+</td><td align="center" valign="middle" >−U<sub>ε</sub></td><td align="center" valign="middle" >U<sub>ε</sub></td><td align="center" valign="middle" >−U<sub>ε</sub></td><td align="center" valign="middle" >010</td></tr><tr><td align="center" valign="middle" >VI</td><td align="center" valign="middle" >−</td><td align="center" valign="middle" >+</td><td align="center" valign="middle" >+</td><td align="center" valign="middle" >U<sub>ε</sub></td><td align="center" valign="middle" >−U<sub>ε</sub></td><td align="center" valign="middle" >−U<sub>ε</sub></td><td align="center" valign="middle" >100</td></tr></tbody></table></table-wrap><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Schematic diagram of the restrain method based on current close-loop and dead- time compensated</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x71.png"/></fig><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Parameters of the propulsion system</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameter type</th><th align="center" valign="middle" >Parameter</th><th align="center" valign="middle" >Value</th></tr></thead><tr><td align="center" valign="middle"  rowspan="11"  >Motor parameters</td><td align="center" valign="middle" >Rated power (P/kW)</td><td align="center" valign="middle" >400</td></tr><tr><td align="center" valign="middle" >Rated phase voltage (U<sub>s</sub>/V)</td><td align="center" valign="middle" >260</td></tr><tr><td align="center" valign="middle" >Rated phase current (I<sub>s</sub>/A)</td><td align="center" valign="middle" >200</td></tr><tr><td align="center" valign="middle" >Rated frequency (f<sub>e</sub>/Hz)</td><td align="center" valign="middle" >50</td></tr><tr><td align="center" valign="middle" >Stator resistance (r<sub>s</sub>/Ω)</td><td align="center" valign="middle" >0.009</td></tr><tr><td align="center" valign="middle" >Stator leakage (l<sub>sl</sub>/H)</td><td align="center" valign="middle" >6.73 &#215; 10<sup>−4</sup></td></tr><tr><td align="center" valign="middle" >Main inductance (l<sub>ms</sub>/H)</td><td align="center" valign="middle" >0.0341</td></tr><tr><td align="center" valign="middle" >Rotor equivalent resistance (r<sub>r</sub>/Ω)</td><td align="center" valign="middle" >0.0131</td></tr><tr><td align="center" valign="middle" >Rotor equivalent leakage (l<sub>rl</sub>/H)</td><td align="center" valign="middle" >3.78 &#215; 10<sup>−4</sup></td></tr><tr><td align="center" valign="middle" >Pare of poles (n<sub>p</sub>)</td><td align="center" valign="middle" >2</td></tr><tr><td align="center" valign="middle" >Momentum (J/kg∙m<sup>2</sup>)</td><td align="center" valign="middle" >15.25</td></tr><tr><td align="center" valign="middle"  rowspan="5"  >Inverter parameters</td><td align="center" valign="middle" >Dead time (t<sub>d</sub>/&#181;s)</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >Switch frequency (f<sub>c</sub>/kHz)</td><td align="center" valign="middle" >2</td></tr><tr><td align="center" valign="middle" >DC voltage (V)</td><td align="center" valign="middle" >700</td></tr><tr><td align="center" valign="middle" >DC capacitance (mF)</td><td align="center" valign="middle" >27.2</td></tr><tr><td align="center" valign="middle" >DC filter inductance (mH)</td><td align="center" valign="middle" >2</td></tr></tbody></table></table-wrap><fig-group id="fig7"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Experimental platform of nine-phase induction motor propulsion system. (a) 9- phase inverter; (b) 9-phase induction motor and power testing machine.</title></caption><fig id ="fig7_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x72.png"/></fig><fig id ="fig7_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x73.png"/></fig></fig-group><fig-group id="fig8"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Simulation results of induction motor before and after using proposed restrain method at no-load. (a) with no restrain measure; (b) use the restrain measure in this paper.</title></caption><fig id ="fig8_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x74.png"/></fig><fig id ="fig8_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x75.png"/></fig></fig-group><p>measure proposed in this paper. From comparison of these two results we can see the effectiveness of the method in this paper.</p></sec><sec id="s4_2"><title>4.2. Experiment</title><p>In order to verify the effectiveness of method in this paper, a single 3-phase unit and the whole 9-phase motor system are both tested.</p><p>1) A single Y unit system experiment</p><p><xref ref-type="fig" rid="fig9">Figure 9</xref>(a) and <xref ref-type="fig" rid="fig9">Figure 9</xref>(b) are experiment results of single Y unit system, respectively without oscillation restrain strategy and with restrain strategy. In <xref ref-type="fig" rid="fig8">Figure 8</xref>(a), oscillation appears in stator current, line voltage and speed. From <xref ref-type="fig" rid="fig9">Figure 9</xref>(b) we can see that there is no oscillation in stator current, voltage and speed after the restrain strategy mentioned above is used, suggesting the effectiveness of this method. In addition, the simulation in <xref ref-type="fig" rid="fig8">Figure 8</xref> coincides with experiment results in <xref ref-type="fig" rid="fig9">Figure 9</xref> very well.</p><p>2) Experimental of 9-phase system</p><p>The three 3-phase units are controlled respectively in 3 groups to simulate the 9-phase system. The voltage of group 2 and group 3 lag out 20 and 40 degree of group 1. Experiment results are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>0. In <xref ref-type="fig" rid="fig1">Figure 1</xref>0, the CH1 represents filtered line-line voltage of phase a<sub>s</sub><sub>1</sub> and b<sub>s</sub><sub>1</sub>; CH2 represents line-line voltage of phase c<sub>s</sub><sub>1</sub></p><fig-group id="fig9"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Experimental waveforms of single Y-system. (a) with no restrain measure; (b) with restrain measure.</title></caption><fig id ="fig9_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x77.png"/></fig><fig id ="fig9_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x76.png"/></fig></fig-group><fig-group id="fig10"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Experimental waveforms of 9-phase system. (a) with no restrain measure; (b) with restrain measure.</title></caption><fig id ="fig10_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x79.png"/></fig><fig id ="fig10_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-8102368x78.png"/></fig></fig-group><p>and b<sub>s</sub><sub>1</sub>; CH3 and CH4 represent current of phase a<sub>s</sub><sub>1</sub> and b<sub>s</sub><sub>1</sub>; CH5 and CH6 represent current of phase a<sub>s</sub><sub>2</sub> and b<sub>s</sub><sub>2</sub>.</p><p>From <xref ref-type="fig" rid="fig1">Figure 1</xref>0, we can see that the low frequency oscillation restrain measure proposed in this paper is effective and can obtain good control performance.</p></sec></sec><sec id="s5"><title>5. Conclusions</title><p>Aiming at the problem that oscillation was likely to occur when induction motor system works at a low frequency range, this paper established the small-signal model of induction, and studied how to restrain the oscillation, and obtain some conclusions:</p><p>1) Analyzing the average model of induction motor-inverter system, and establishing the small-signal model of the whole motor system;</p><p>2) During the low frequency oscillation, the stator current varied in a period. Based on this, the oscillation restrain strategy combining closed current loop with dead time compensation is proposed in this paper. Simulation and experiment results verify the effectiveness of this method.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.56648-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Singh, G.K. (2002) Multiphase Induction Machine Drive Research—A Survey. 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