<?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">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2015.610150</article-id><article-id pub-id-type="publisher-id">AM-59460</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Tooth Surface Design for Variable Transmission Ratio Bevel Gearing
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>an</surname><given-names>Yang</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>Dawei</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yanling</surname><given-names>Tian</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Tianjin Key Laboratory of the Design and Intelligent Control of the Advanced Mechatronical System, School of Mechanical Engineering, Tianjin University of Technology, Tianjin, China</addr-line></aff><aff id="aff2"><addr-line>School of Mechanical Engineering, Tianjin University, Tianjin, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>y79nzw@163.com(AY)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>08</day><month>09</month><year>2015</year></pub-date><volume>06</volume><issue>10</issue><fpage>1685</fpage><lpage>1695</lpage><history><date date-type="received"><day>31</day>	<month>October</month>	<year>2014</year></date><date date-type="rev-recd"><day>accepted</day>	<month>5</month>	<year>September</year>	</date><date date-type="accepted"><day>8</day>	<month>September</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>
 
 
  A novel CAD method for tooth profile based on the gearing feature has been proposed in this paper, and this method could be applied to the variable transmission ratio and three-dimension situation. The two pitch curves of the two gears can be generated due to the given transmission ratio. The tooth profile curves are formed in each coordinate system of its pitch curve by the gearing process. Finally, the tooth profile could be extracted and translated into a real dimension by CAD method. It is provided a simply thought for tooth profile design to avoid so much complicated mathematical reasoning.
 
</p></abstract><kwd-group><kwd>Computer-Aided Design</kwd><kwd> Computational Geometry</kwd><kwd> Gear Design</kwd><kwd> Gear Geometry</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Bevel gearings are used in the situation of driving between the unparallel axes and have a wide application field. Because the gearing motion is so complex, the mathematical theory is very deep and the calculations are multifarious [<xref ref-type="bibr" rid="scirp.59460-ref1">1</xref>] . In this paper, an apparent and effective method is proposed, although it doesn’t need unfathomable mathematical theory.</p><p>At first, based on the gearing feature, a pair of pitch curves (from gear 1 and 2) are generated. Tooth profile 1 can be arbitrarily drawn around the pitch curve 1; tooth profile 2 is uniquely formed by the motion of the tooth profile 1 along the pitch curve 2. The motion of the tooth profile 1 divides the space into two regions (scanned by gear 1 and not scanned by gear 1) and their boundary line. The region not scanned by gear 1 can be the region where gear 2 exists; otherwise the tooth profile 2 should be the boundary line. The boundary line could be extracted by digital image processing [<xref ref-type="bibr" rid="scirp.59460-ref2">2</xref>] and translated into a real dimension finally. The gear 2 is obtained just like the paper-cut, so the complex process of enveloping line solution of mathematical meaning could be avoided.</p></sec><sec id="s2"><title>2. The Presentation of the Problem</title><p>The aim gears to be design are a pair of bevel gearings whose axes are vertical to each other as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>The transmission ratio:</p><disp-formula id="scirp.59460-formula489"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x6.png"  xlink:type="simple"/></disp-formula><p>where:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x7.png" xlink:type="simple"/></inline-formula>;</p><p>i is the transmission ratio;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x8.png" xlink:type="simple"/></inline-formula>are teeth number;</p><p>c is adjusting constant;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x9.png" xlink:type="simple"/></inline-formula>are the rotation angle of gear 1 and 2.</p><p>The mathematical relationship between t<sub>1</sub> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x10.png" xlink:type="simple"/></inline-formula> is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The position relationship of the pair of bevel gearing, where γ is the angle between the two gear’s axes, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x12.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x11.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The relationship between t<sub>1</sub> and t<sub>2</sub> according to Equation (1), where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x14.png" xlink:type="simple"/></inline-formula> is the integration of Equation (1)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x13.png"/></fig></sec><sec id="s3"><title>3. The Solution of the Two Pitch Curves</title><p>The pitch curves are two fictitious closed curves on the two gears which have pure rolling behavior. Suppose that gear 2 (the axis is OY) lives in coordinate system {O} and don’t move, on the other hand, gear 1 lives in coordinate system {A}, and its rotating axis is OA. OA contrarotates based on OZ axis in XOY plane (see from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x15.png" xlink:type="simple"/></inline-formula> to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x16.png" xlink:type="simple"/></inline-formula>), while gear 1 contrarotates based on OA (see from A to O), as shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p>The {O} coordinate of a point K on the pitch curve in {A} is {x, y, z}. After gearing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x17.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x18.png" xlink:type="simple"/></inline-formula> angle, K moves to K' whose {O} coordinate is {x', y', z'}. So:</p><disp-formula id="scirp.59460-formula490"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x19.png"  xlink:type="simple"/></disp-formula><p>where:</p><disp-formula id="scirp.59460-formula491"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x20.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x21.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x22.png" xlink:type="simple"/></inline-formula>are the small rotating steps of axis OA and gear 1.</p><p>According to the meanings of pitch curve:</p><disp-formula id="scirp.59460-formula492"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x23.png"  xlink:type="simple"/></disp-formula><p>According to Equation (2):</p><disp-formula id="scirp.59460-formula493"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x24.png"  xlink:type="simple"/></disp-formula><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The two coordinate systems of the two gears. Gear 2 in coordinate system {O} and gear 1 in coordinate system {A} <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x26.png" xlink:type="simple"/></inline-formula> because of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x27.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x25.png"/></fig><p>where:</p><disp-formula id="scirp.59460-formula494"><graphic  xlink:href="http://html.scirp.org/file/3-7402537x28.png"  xlink:type="simple"/></disp-formula><p>Because:</p><disp-formula id="scirp.59460-formula495"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x29.png"  xlink:type="simple"/></disp-formula><p>So, the equations have infinite solutions:</p><disp-formula id="scirp.59460-formula496"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x30.png"  xlink:type="simple"/></disp-formula><p>when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x31.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.59460-formula497"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x32.png"  xlink:type="simple"/></disp-formula><p>where transmission ratio <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x33.png" xlink:type="simple"/></inline-formula></p><p>The intersecting line G2 between the bevel surface of Equation (8) and spherical surface</p><disp-formula id="scirp.59460-formula498"><label>(8’)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x34.png"  xlink:type="simple"/></disp-formula><p>is the pitch curve of gear 2 in {O}. The equations of the intersecting line G2 are:</p><disp-formula id="scirp.59460-formula499"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x35.png"  xlink:type="simple"/></disp-formula><p>The equations of the pitch curve G1 of gear 1 in {A} can be also obtained:</p><disp-formula id="scirp.59460-formula500"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x36.png"  xlink:type="simple"/></disp-formula><p>The pitch curves G1 and G2 is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The two pitch curves G1 and G2</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x37.png"/></fig></sec><sec id="s4"><title>4. The Design of the Tooth Profiles</title><sec id="s4_1"><title>4.1. The Generation of Gears</title><p>When the transmission ratio is given, the two pitch curves are determined uniquely. However, the tooth profile curves of the two gears are not unique. When one is given, the other is determined. We can design a three- dimension curve based on G 1’ s pitch curve to be its tooth profile curve:</p><disp-formula id="scirp.59460-formula501"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x38.png"  xlink:type="simple"/></disp-formula><p>where:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x39.png" xlink:type="simple"/></inline-formula>, H is adjusting coefficient，<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x40.png" xlink:type="simple"/></inline-formula> come from Equation (10).</p><p>So, G 1’ s tooth profile curve S1 is shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>.</p><p>Suppose that on the spherical surface, the S1 rolls purely along the pitch curve G2 (G1 and G2 are tangent), then the region where S1 doesn’t sweep should be the region where gear 2 exist. The black region where is swept by S1 (see from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x41.png" xlink:type="simple"/></inline-formula> to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x42.png" xlink:type="simple"/></inline-formula>) is shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>, and the new pitch curve of gear 2 (S2) appears.</p></sec><sec id="s4_2"><title>4.2. The Extraction of Tooth Profile Curve</title><p>The black region (in <xref ref-type="fig" rid="fig6">Figure 6</xref>) swept by S1 is projected on XOY plane, as shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>. The tooth profile curve S2 can be obtained by image processing technology. As shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>, the color region is composed by civil points and the white region is composed by outside points. The boundary line between the color region and white region can be found and extracted orderly in a given direction by image processing.</p><p>OA and OB are calibration lines to translate pixel size into real size; the color region is composed by civil points and the white region is composed by outside points.</p><p>We provide (this provision really makes sense) that these points are boundary points: if there is at least an “outside point” on the position “a, c, e, g” of point M as shown in <xref ref-type="fig" rid="fig8">Figure 8</xref>, then the point M is boundary point. So, there are three types of points: outside point “0”, civil point “1”, boundary point “ 2” . We can find a boundary point “ 2” as a beginning point along any scan line, and name its address “P 1” . Search all the eight positions</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> G 1’ s tooth profile curve S1</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x43.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> The black region swept by S1</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x44.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Inner points and outer points</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x45.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> The eight positions (a, b, c, ∙∙∙, h) of point M</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x46.png"/></fig><p>(a, b, c, d, e, f, g, h) of P1 (see in <xref ref-type="fig" rid="fig8">Figure 8</xref>), name the first boundary point’s address “P2”, and let the content of P1 be “ 3” which won’t be searched anymore. P1 replaces P2, and find the next P 2 in the same way till return to the beginning point. Therefore, at last, all the boundary points are “ 3” . This process is called ordinal extraction, as shown in <xref ref-type="fig" rid="fig9">Figure 9</xref>.</p><p>The flow of the ordinal extraction of boundary line is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>0.</p></sec><sec id="s4_3"><title>4.3. The Translation of Pixel Size into Real Size</title><p>The tooth profile S2 which has been extracted is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>1(a). But S2 is pixel meaning, so it should be translated into real size. The relationship between pixel size and real size is shown in Equation (12).</p><disp-formula id="scirp.59460-formula502"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7402537x47.png"  xlink:type="simple"/></disp-formula><p>where xp, yp are pixel coordinate; x, y are real coordinate; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x48.png" xlink:type="simple"/></inline-formula>are the length of the lines which we know;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x49.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x50.png" xlink:type="simple"/></inline-formula>are the pixel number in OA and OB. S 2 in a real coordinate is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>1(b). The XOY projections of the four positions of S1 gearing with S2 are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>2.</p></sec><sec id="s4_4"><title>4.4. Discussion</title><p>Will the two gears run steadily? Will their profile curves leave each other? These are not in the scope of this paper</p><fig-group id="fig9"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> The ordinal extraction of boundary line.</title></caption><fig id ="fig9_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x51.png"/></fig><fig id ="fig9_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x52.png"/></fig></fig-group><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> The flow of ordinal extraction of boundary line</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x53.png"/></fig><fig-group id="fig11"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> (a) The extraction of S2 and (b) S 2 in a real coordinate.</title></caption><fig id ="fig11_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x54.png"/></fig></fig-group><fig-group id="fig12"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> The XOY projection of four position of S1 gearing with S2. (a)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x57.png" xlink:type="simple"/></inline-formula>; (b)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x58.png" xlink:type="simple"/></inline-formula>; (c)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x59.png" xlink:type="simple"/></inline-formula>; (d)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7402537x60.png" xlink:type="simple"/></inline-formula>.</title></caption><fig id ="fig12_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x55.png"/></fig><fig id ="fig12_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x56.png"/></fig></fig-group><p>(which could be known from [<xref ref-type="bibr" rid="scirp.59460-ref3">3</xref>] -[<xref ref-type="bibr" rid="scirp.59460-ref6">6</xref>] ). But a geometrical answer can be given. At an ecumenical position of gearing, via a tangent point of two tooth profile curve, draw a normal line of a tooth profile curve. The directions of the normal line and the press force at this point are same. If there are some normal lines upon the rotating axis and some normal line below the rotating axis, that is to say, the moments of the press forces of the rotating axis are complete negatively and positively, and then the gearing is steady reasonably.</p><p>For example, as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>3, draw three normal lines of gear 2 via the tangent points, the moments of press force F1, F2 are clockwise and moment of F3 is counterclockwise. But this is only a geometrical precondition to be steady; the detailed mechanical analyzation is not in the scope of this paper.</p></sec><sec id="s4_5"><title>4.5. Three-Dimension Situation</title><p>In the three-dimension situation, S2 is a space curve on the spherical surface (the “S 2” mentioned before is its projection on XOY). Given a radius “a” (from Equation (8’)), there will be a pair of gears S1 and S2, as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>4. Therefore, the part of the spherical surface encircled by S1 or S2 is a cut section of a bevel gearing corresponding radius “a”. All the cut sections corresponding different radius “a” compose the whole bevel gearing.</p><fig id="fig13"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> The normal lines via the tangent points</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x61.png"/></fig><fig id="fig14"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>4</label><caption><title> The cut sections of the two bevel gearings on the spherical surface</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7402537x62.png"/></fig></sec></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, a novel design method of space bevel gearing based on gearing feature is proposed. The two pitch curves are generated based on the transmission ratio, and then a tooth profile could be designed based on its pitch curve independently. According to its motion, the second tooth profile could be found and translated into a real size by image processing technology. Comparing to complicated method [<xref ref-type="bibr" rid="scirp.59460-ref7">7</xref>] -[<xref ref-type="bibr" rid="scirp.59460-ref11">11</xref>] , this method could avoid complex calculation and exceptional solution, and could almost design any gear or rack. However, this method is also limited in precision, if the image is very small, the size error will arise due to lack of pixels [<xref ref-type="bibr" rid="scirp.59460-ref12">12</xref>] . So, the image must be zoomed in enough.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This work was supported by China Post-Doctoral Foundation No. 2012M520572, Tianjin Municipal Education Commission Grant No. 20120401, and Tianjin Municipal Science and Technology Commission Key Grant No. 14JCZDJC39500.</p></sec><sec id="s7"><title>Conflict of Interests</title><p>None.</p></sec><sec id="s8"><title>Cite this paper</title><p>NanYang,DaweiZhang,YanlingTian, (2015) Tooth Surface Design for Variable Transmission Ratio Bevel Gearing. Applied Mathematics,06,1685-1695. doi: 10.4236/am.2015.610150</p></sec><sec id="s9"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.59460-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Jia, J.M., Gao, B. and Zhao, D.L. (2008) Analysis Method for Noncircular Bevel Gearing Based on Geodesic Curvature Preserving Mapping. Chinese Journal of Mechanical Engineering, 44, 53-57.  
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