AGMA 11FTM08-2011 A Comprehensive System for Predicting Assembly Variation with Potential Application to Transmission Design.pdf
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1、11FTM08AGMA Technical PaperA ComprehensiveSystem for PredictingAssembly Variation withPotential Application toTransmission DesignBy K. Chase and C. Sorensen,Brigham Young UniversityA Comprehensive System for Predicting Assembly Variationwith Potential Application to Transmission DesignKenneth W. Cha
2、se and Carl D. Sorensen, Brigham Young UniversityThe statements and opinions contained herein are those of the author and should not be construed as anofficial action or opinion of the American Gear Manufacturers Association.AbstractRecent advances in tolerance analysis of assemblies allow designers
3、 to:S Predict tolerance stack-up due to process variations.S Examine variation in clearances and fits critical to performance.S Use actual production variation data or estimates from prior experience.S Use engineering design limits to predict the percent rejects in production runs.Acomprehensivesyst
4、emhasbeendevelopedformodeling1D,2D,and3Dassemblies,whichincludesthreesources of variation: dimensional (lengths and angles), geometric (GD theclosedlooplocates theArm as it slides inor out toaccom-modate dimensional variation. In this case, to properly grip the Reel, the Gap must be negative over th
5、e fullrangeof dimensional variations. As is often thecase, theopen loopdepends onelements of the closedloopfor its solution. In this case, RLis the result of the vector chain in the closed loop, so the loops are coupled.Figure 4. General 2-D vector loop, showing relative angles between adjacent vect
6、ors6 11FTM08Figure 5. Vector assembly model showing an open and a closed loop, representing a lockinghub assemblyThe vectors in a vector loop are not simply pin jointed together. To accurately represent solid bodies, thevectorsmustbefixedtothepartstheyrepresent. Thus,therelativeanglebetweentwovector
7、smayrepresenta machined angle between two surfaces on the same part, in which case the nominal angle and tolerancewould be specified. Alternately, if two adjacent vectors are fixed to two mating parts, their angles or lengthsmay vary kinematically, describingthedegreesof freedombetweentheparts, inwh
8、ichcaseonly thenominallengths andangles of thekinematic variables would beknown. Their variations could only be determinedbyan assembly tolerance analysis.Kinematic degrees of freedomThe kinematic degrees of freedom, which describe the small displacements between mating parts, may beadded to a vecto
9、r assembly model by inserting kinematic joints into the vector loops. Figure 6 shows 12common kinematic joints, which may be used to represent mating surfaces in assemblies. The arrows andnumbers indicate the degrees of freedom in each case.Figure 6. 3-D kinematic joints representing mating surfaces
10、 and degrees of freedom inassemblies7 11FTM08Vector models havebeenwidely usedtorepresent therigidbodykinematics ofmechanisms. They mayalsobeusedtomodelstaticassemblies. Themajordifferencesbetweenakinematicmodelofamechanismandakinematicmodelofastaticassemblyaretheinputsandoutputs. Formechanismanalys
11、is,theinputsarelargemotions of one or more of the members; the outputs are the rigid body displacements, velocities, etc. of themembers. For static assemblies, theinputs aresmall variations inthedimensions andgeometric form ofthemembers; the outputs are the small rigid body displacements that occur
12、due to production variations. For amechanismmodel,thesolutiondescribesthemotionofasinglemechanismwithtime,fromonepositiontothenext. For a static assembly, a statistical solution predicts the variation of all assemblies compared to thenominal assembly, or the change from one assembly to the next.Geom
13、etric variationsGeometricvariationsofform,orientationandlocationarethefinalsourceofvariationtobeincludedinavectorassemblymodel. Suchvariationscanonlyintroducevariationintoanassemblywheretwopartsmakematingcontact. Themannerinwhichgeometricvariationpropagatesacrossmatingsurfacesdependsonthenatureof th
14、e contact.Figure 7 illustrates this concept. Consider a cylinder on a plane, both of which are subject to surfacewaviness,representedbyatolerancezone. Asthetwopartsarebroughttogethertobeassembled,thecylin-der could be on the top of a hill or down in a valley of a surface wave. Thus, for this case, t
15、he center of thecylinder will exhibit translational variation from assembly-to-assembly in a direction normal to the surface.Similarly, the cylinder could be lobed, as shown in the figure, resulting in an additional vertical translation,depending on whether the part rests on a lobe or in between.Inc
16、ontrast tothecylinder/planejoint, theblock onaplane, showninFigure 7, exhibits rotational variation. Intheextremecase,onecorneroftheblockcouldrestonawavinesspeak,whiletheoppositecornercouldbeatthebottomofthevalley. Themagnitudeofrotationwouldvaryfromassembly-to-assembly. Wavinessonthesurface of the
17、block would have a similar effect.In general, for two mating surfaces, we have two independent surface variations, which introduce variationinto the assembly. How they propagate depends on the nature of the contact, that is, the type of kinematicjoint. Figure 8shows two3-D joints, subject tosurfacev
18、ariation. An unconstrainedbody has six degrees offreedom (arrows). Contact between mating surfaces creates constraints. Each arrow is either a K or an F.ThearrowsmarkedwithaKindicatethekinematicdegreesoffreedominthejoint. ThearrowsmarkedbyanFindicateaconstraineddirectionforformvariationpropagation.K
19、inematic displacementspropagatealongthekinematic axes. Geometric form variations can only propagate through the constrained axes of the joint.Asanestimateofthemagnitudeofassemblyvariationproducedbysurfacevariation,wecanusethegeomet-ric tolerancezonespecifiedas designlimits andthelengthof contactbetw
20、eenthematingparts,as definedinequation1aand1b. For translational variation, theextrememagnitudedis assumed tobe equal to half thetolerancezone. For rotational variation, the extremeangle dis formed by the contact length extendedoverthe peak-to-valley height.Figure 7. Propagation of 2-D translational
21、 and rotational variation due to surface waviness8 11FTM08Figure 8. Simultaneous propagation of translational and rotational variation due to surfacewaviness in 3-DTranslational variation(1a)d 12tol zoneRotational variation(1b)d= tan1tol zonecontact lengthSincetheextremevalueisprobablyarareoccurrenc
22、e,settingthetolerancezoneequal tothe 3 limits ofanormal distribution will make an extreme less likely to occur in the assembly model. A catalog of models forgeometricvariationshasbeendefinedforeachofthe12jointsshowninFigure 6,correspondingtoeachoftheANSI Y14.5 geometric tolerance specifications 2.Th
23、e models for geometric variation are only approximations to permit the effects to be included in toleranceanalysis. More study is needed to develop improved models. In particular, the propagation of surface vari-ation in assemblies needs to be characterized andverified. The interactionof geometric v
24、ariations withsizevariations and the consequences of the Envelope Rule are other issues which need to be resolved.Assembly tolerance specificationsAmanufacturedproductmustperformproperlyinspiteofdimensionalvariation. Toachievethis,engineeringdesignrequirements mustincludeassemblytolerancelimits. The
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