<?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.2011.38104</article-id><article-id pub-id-type="publisher-id">ENG-6830</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>
 
 
  Diagnosis on Surface Failure in Gear Equipment Using Time - Frequency Domain Analysis
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>uji</surname><given-names>Ohue</given-names></name><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Toshiya</surname><given-names>Kounou</given-names></name></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Katsuhiko</surname><given-names>Yazama</given-names></name></contrib></contrib-group><author-notes><corresp id="cor1">* E-mail:<email>ohue@eng.kagawa-u.ac.jp(UO)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>12</day><month>08</month><year>2011</year></pub-date><volume>03</volume><issue>08</issue><fpage>851</fpage><lpage>858</lpage><history><date date-type="received"><day>July</day>	<month>14,</month>	<year>2011</year></date><date date-type="rev-recd"><day>July</day>	<month>28,</month>	<year>2011</year>	</date><date date-type="accepted"><day>August</day>	<month>5,</month>	<year>2011</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>
 
 
  In order to make more progress in the gear performance, it is important to evaluate the gear dynamics more precisely, since gear is a main machine element in motion and power transmissions. For preventing the unexpected failure in mechanical systems, a large amount of work has been carried out based on a statistical model developed by Lundberg and Palmgren [1] with reliability models using the classical fatigue theory. However, most of these works did not consider the operating conditions of machine during the fatigue process.
 
</p></abstract><kwd-group><kwd>Natural Asset</kwd><kwd> Financial Value</kwd><kwd> Neural Network</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In order to make more progress in the gear performance, it is important to evaluate the gear dynamics more precisely, since gear is a main machine element in motion and power transmissions. For preventing the unexpected failure in mechanical systems, a large amount of work has been carried out based on a statistical model developed by Lundberg and Palmgren [<xref ref-type="bibr" rid="scirp.6830-ref1">1</xref>] with reliability models using the classical fatigue theory. However, most of these works did not consider the operating conditions of machine during the fatigue process.</p><p>Generally, the gear dynamic performance has been analyzed using Fast Fourier Transform (FFT) as a function of frequency. However, it is difficult to identify an instantaneous change of signals. In many health monitoring applications, it is more useful to analyze how measurement characteristics change as a function of both time and frequency. The Wavelet Transform (WT) is a method for the time-frequency analysis of signals [2,3]. The WT involves decomposing a signal into a representation comprised of local basis functions called wavelets. Each wavelet is located at a different position on the time axis and is local in the sense that it decays to zero when sufficiently far away from its center. The structure of a non-stationary signal can be analyzed in this way with local features represented by closely-packed wavelets of short length. Therefore, the WT can provide more beneficial information about the frequency compared with the FFT. By reason of the advantage on the WT, the applications of the WT to the diagnostics of the gear sets have been studied [4-7]. Their studies have focused mainly on whether some kinds of the WTs can provide the information to detect the fault of the gear system. However, it is also important to diagnose the failure of the gear sets using not only the WT but also the tooth meshing of the gear pair. Considering the tooth meshing of the gear pair would enable to construct the new diagnosis for the gear sets, which is different from the conventional diagnosis.</p><p>In order to evaluate the dynamic characteristics of gear pair, the dynamic performance of sintered and steel gears were measured using a power circulating gear testing machine. The dynamic characteristics were analyzed in a time-frequency domain by the continuous WT, and also those signals were decomposed and reconstructed by the discrete WT. The validity of the new evaluation method by the WT was discussed. Furthermore, in order to perform the health monitoring of the gear sets, a gear fatigue test was carried out and the dynamic characteristics during the fatigue test were measured and discussed by using the WT.</p></sec><sec id="s2"><title>2. Wavelet Transform</title><p>The Wavelet Transform (WT) has been extensively developed. Applications of the WT are actively studied in a variety of fields in engineering [4-9]. The Continuous Wavelet Transform (CWT) of a function f(t) is defined as follows.</p><disp-formula id="scirp.6830-formula154372"><label>(1)</label><graphic position="anchor" xlink:href="9-8101490\90e63dda-9d8d-4a65-ab09-ebcc4a617c38.jpg"  xlink:type="simple"/></disp-formula><p>where, the bar over ψ(t) indicates the conjugate of a mother wavelet function ψ(t), a and b indicate the parameters on frequency and time. The Gabor function defined by Equation (2) is adopted as the wavelet function ψ(t).</p><disp-formula id="scirp.6830-formula154373"><label>(2)</label><graphic position="anchor" xlink:href="9-8101490\22db613e-a1f6-44eb-9db1-a6e31008b804.jpg"  xlink:type="simple"/></disp-formula><p>where, ω<sub>p</sub> is a center of angular frequency, γ is a constant and was set at <img src="9-8101490\e2a873a3-7252-460a-8c9c-36aa42630c6c.jpg" /> = 5.336 in this study. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows Gabor function based on sinusoidal waves e<sup>i</sup><sup>ωt</sup> and its Fourier spectrum.</p><p>When the coordinates (b, a) of the CWT shown in Equation (1) are discretized to the coordinates (2<sup>-j </sup>k, 2<sup>-j</sup>) using two integers j and k, the Discrete Wavelet Transform (DWT) is defined as follows.</p><disp-formula id="scirp.6830-formula154374"><label>(3)</label><graphic position="anchor" xlink:href="9-8101490\222dd2cb-597b-4a13-92d1-a980e5e414dc.jpg"  xlink:type="simple"/></disp-formula><p>where, <img src="9-8101490\36a387ef-0303-4a16-a492-cdfc034a13d9.jpg" />is equal to (W<sub>ψ</sub> f)(2<sup>-j</sup>k, 2<sup>-j</sup>). j is called level. The Inverse Discrete Wavelet Transform (IDWT) is defined as</p><disp-formula id="scirp.6830-formula154375"><label>(4)</label><graphic position="anchor" xlink:href="9-8101490\723fcdc7-bf61-4ef2-af0c-3d0b128adc53.jpg"  xlink:type="simple"/></disp-formula><p>The function g<sub>j</sub>(t) on the wavelet component is given by</p><disp-formula id="scirp.6830-formula154376"><label>(5)</label><graphic position="anchor" xlink:href="9-8101490\c31cfcf0-478d-4b2d-aee5-30bd20a47e56.jpg"  xlink:type="simple"/></disp-formula><p>Suppose that f<sub>j</sub>(t) is the function at a level j, f<sub>j</sub>(t) is satisfied with the following relation.</p><disp-formula id="scirp.6830-formula154377"><label>(6)</label><graphic position="anchor" xlink:href="9-8101490\078069fc-449f-494d-a6e2-ea7fb4cea39d.jpg"  xlink:type="simple"/></disp-formula><p>where, <img src="9-8101490\dd365855-8019-4832-a7fa-8255cbea3d6b.jpg" />is a sequence at a level j, and <img src="9-8101490\9173e895-5f1c-4146-b5b7-b06bfb5fef54.jpg" />(t) is a scaling function. The scaling function <img src="9-8101490\1a0f47ee-6eb4-40b9-a118-0a220aa45f80.jpg" />(t) and the mother wavelet function ψ(t) are satisfied with the two-scale relations as follows.</p><disp-formula id="scirp.6830-formula154378"><label>(7)</label><graphic position="anchor" xlink:href="9-8101490\4f0f5ba8-f493-457c-9aa1-fc4201a4d6f1.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.6830-formula154379"><label>(8)</label><graphic position="anchor" xlink:href="9-8101490\fb414d73-b88b-4af7-8e83-b5e2b5f6ebac.jpg"  xlink:type="simple"/></disp-formula><p>where, {p<sub>k</sub>} and {q<sub>k</sub>} are two-scale sequences. The functions g<sub>j</sub>(t) and f<sub>j</sub>(t) at a level j are able to be found by using Equations (5) and (6). The function f<sub>j</sub>(t) decomposed into the function g<sub>j</sub>(t) on the wavelet component is satisfied with the following relation.</p><disp-formula id="scirp.6830-formula154380"><label>(9)</label><graphic position="anchor" xlink:href="9-8101490\29688e8e-79c1-495f-ae0d-d5681f741f8e.jpg"  xlink:type="simple"/></disp-formula><p>In this study, the scaling and the mother wavelet functions based on the cardinal B-spline function in order of m = 4 was adopted. The cardinal B-spline function N<sub>m</sub>(t) in order of m is defined as follows.</p><disp-formula id="scirp.6830-formula154381"><label>(10)</label><graphic position="anchor" xlink:href="9-8101490\cfdcb15b-d2e8-4fdd-b287-e64b080d0921.jpg"  xlink:type="simple"/></disp-formula><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the scaling function <img src="9-8101490\0dd84475-ca08-46f1-ab90-9b65f81c74fd.jpg" />(t) and the mother wavelet function ψ(t) based on the function N<sub>4</sub>(t). The sequences {a<sub>k</sub>}, {b<sub>k</sub>}, {p<sub>k</sub>} and {q<sub>k</sub>} are given in Reference [<xref ref-type="bibr" rid="scirp.6830-ref2">2</xref>].</p></sec><sec id="s3"><title>3. Dynamic Characteristics of Gear</title><sec id="s3_1"><title>3.1. Test Gear and Testing Machine</title><p><xref ref-type="table" rid="table1">Table 1</xref> shows the specifications of gear pair employed in this dynamic performance test. The module is 5 mm and the pressure angle is 20 deg. The test gears are</p></sec></sec></body><back><ref-list><title>References</title><ref id="scirp.6830-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">G. Lundberg and A. Palmgren, “Dynamic Capacity of Rolling Bearings,” ACTA, Polytechnica, Mechanical Engineering Se-ries, Vol. 1, No. 3, 1947, p. 7.</mixed-citation></ref><ref id="scirp.6830-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">C. K. 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