“Design and development of better alternatives to shrink fit achieved by induction heating in rotor

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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056

Volume: 09 Issue: 09 | Sep 2022 www.irjet.net p-ISSN: 2395-0072

Abstract - Inrotorshaftassemblyofhermeticallysealedreciprocatingcompressor,thereisinterferencefitbetweenrotorand shaft. To obtain this interference fit various methods are used. Without the use of extra mechanical fastening systems, interference-fittedjointsareanefficientandcost-effectivewaytoassemblecomponents.Aninterfacepressureisestablished duringassemblybypress-fittingorashrink-fittingassemblyprocessasaresultofadimensionalmisfitbetweenthetwoparts, whichisfrequentlyinashaftandrotor.Becauseoffrictionalresistance,thejointisabletowithstandaxialforcesandtorques. Thetraditionalmethodforachievingashrinkfitbetweentherotorandshaftisinductionheating.Thisprocessrequiresheating equipmentandhigherenergyconsumption,thiswillincreasethemanufacturingcostofthecompressor.Duetothelimitationsof inductionheatingprocess,thereisaneedtoidentifyanddesignanalternativeoptionsforachievingshrinkfitinrotorshaft assemblyincosteffectivemanneryetensuringthedesiredquality.Thispaperpresentsthestudyofcurrentandproposed assemblyprocedureusedtogetrotor-shaftassemblyinhermeticallysealedreciprocatingcompressor.Inthisstudy,factorsthat affectaninterference-fittedjoints'abilitytofunctionproperlyaregroupedunderafewgeneralheadings,including:coefficientof friction,coefficientofthermalexpansion,surfaces,thegeometry,frictionalforce,torque,tangentialforce,materials,loading,and lastlytheassemblymethodutilizedtocreatethejointbetweentherotorandshaft.

Keywords: Interference fit, , rotor shaftassembly,shrinkfitting,inductionheating,radial orinterfacepressure,torque, frictional force, tangential force.

1. INTRODUCTION:

Inrotorshaftassemblyofthehermeticallysealedreciprocatingcompressor,toachieveaninterferencefitbetweenrotorand shaft,shrinkfittingtechniquesaregenerallyused.Shrinkfittingtypicallyreferstotechniquesthatutilizethephenomenaof thermalcontractionandexpansiontoproduceaninterferencefit.Themostcommonmethodfordoingthisistoheattheouter component,causingittoexpandthermally.Thentwopartsfittogethereasily.Anincrediblytightjointformsaroundtheinner partwhentheouterpartcoolstoroomtemperatureandcontractsbacktoitsoriginalsize.Typically,metalswillexpandin responsetoheating.Soinductionheatingisgenerallyusedtoobtainshrinkfitinrotorshaftassembly.Inexistinginduction heatingprocessrotorisheatedfromoutsidesurfaceandthenheatistransferredfromoutsidetoinsidesurfaceofrotortoobtain thermalexpansionofrotorbore.Afterexpansion,rotorisshrinkfittedintotheshaft.Butthisprocessrequireshigherpower consumptionandhenceincreasesthemanufacturingcostofthecompressor.Soheatingfromtheinsidesurfaceoftherotorbore isthealternativeoptiontoachieveshrinkfitinrotorshaftassembly.

2. Rotor Shaft Assembly:

Figure1.Dimensionsofrotorandshaftinterferencefitpriortoassembling

dA =Outsidediameterofshaft

dM =Insidediameterofrotor

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“Design and development of better alternatives to shrink fit achieved by induction heating in rotor shaft assembly of the hermetically sealed reciprocating compressor”
Nandini Chavan1 , Dr .M. S. Kale 2
Student, Mechanical Engineering Department, Government College Of Engineering, Karad, Maharashtra India.
***

International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056

Volume: 09 Issue: 09 | Sep 2022 www.irjet.net p-ISSN: 2395-0072

d=Diametricinterference

Figureshowsthedimensionsofrotorandshaftinterferencefitpriortoassembling.Interferencefitisalsoknownaspressfitor frictionfit,isafasteningmethodwheretwoparts,typicallycircularcrosssectionshape,arepushedtogether(oneintothe other)andkeptinplaceduetothepressurebetweenthem.Typically,theinnerpartwillhaveanominalouterdiameterslightly greaterthanthenominalinnerdiameteroftheouterpart,andwhenpushedorforcedtogetherthecontactfrictionforceskeep thepartsfrommovingrelativetoeachother Thelevelofinterferencedependsonthenegativedifferenceinnominaldiameters.

Shrink Fit Process

Obtaining shrink fit by heating from the inside surface of the rotor bore:

Theonlyviablewaytoheattherotorisusinganinductioncoilfromtheinsidesurfaceoftheoftherotorbore,thisheatallowsfor betterenergydeliverytotheassembly.Inthismethodheatingwillbeonlylocalheating.Aninductioncoilcanbeusedtoheatthe rotorbore.Thecoilisinsertedintotherotorboreandpowerisappliedforcertaintimetoreachtherequiredtemperaturefor heatingtherotorboreandtriedtoexpandtherotorboreandplacedontotheshaft.Thisprocessconsumeslesspoweras comparedtoheatingfromtheoutsidesurfaceofrotor.

Theoretical modelling of Thermal expansion:

Part Material Outsidediameter (mm) Inside Diameter(mm) Stack Height(mm) CoefficientofThermal expansion(mm/mm0c) Rotor Aluminium 60.3 19.5 63.5 23.1

Table1:Dimensionsandmaterialpropertiesofaluminiumrotor

DiameterincreaseofrotorborewhenbeingheatedorThermalexpansionofrotorboreiscalculatedas:

Δd=doαΔT

Where,

Δd=changeindiameterofrotorboreorthermalexpansion(mm)

do =insidediameterofrotoratinitialtemperature(mm)

α=coefficientofthermalexpansionofaluminum,23.1 10-6 (mm/mm0C)

ΔT=changeintemperature(0C)

Roomtemperature=27 0C

Originaldiameterof rotorbore(mm) Temperature (0C)

Thermalexpansionof rotorbore(mm) Increaseddiameterof rotorbore(mm)

19.5 50 0.01 19.51 19.5 80 0.023 19.523 19.5 100 0.032 19.53 19.5 150 0.05 19.55 19.5 200 0.07 19.57 19.5 225 0.089 19.58

Table2:TheoreticalmodellingofThermalexpansion

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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056

Volume: 09 Issue: 09 | Sep 2022 www.irjet.net p-ISSN: 2395-0072

Experimental method for obtaining required thermal expansion of rotor bore by heating from inside surface of rotor bore:

RotorMaterial Rotoroutsidediameter(mm) Rotorinsidediameter(mm) Aluminium 60.3 19.5

Table3:Dimensionsofaluminiumrotorbore

Process:A2KWcartridgeheaterrodisusedtoheattherotorbore.Therodisinsertedintotherotorboreandpowerisapplied fortimetoreachtherequiredtemperatureatwhichthermalexpansionofrotorboreisobtained.Inthisprocesstriedtoexpand therotorboreatvarioustemperature.Temperatureismeasuredbythermocouple.Thermalexpansionismeasuredbydigital verniercaliperhavingleastcountof0.01mm.

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Figure2.CartridgeHeaterRod Figure3.AluminumRotor Figure4.ExperimentalSetup Figure5.ThermalExpansionofaluminium rotorbore

International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056

Volume: 09 Issue: 09 | Sep 2022 www.irjet.net p-ISSN: 2395-0072

Experimental Result:

OriginalDiameterof rotorbore(mm)

Temperature(ºC) Thermal expansion(mm) Changeindiameterof rotorbore(mm)

19.5 50 0.03 19.53 19.5 80 0.06 19.56 19.5 100 0.08 19.58 19.5 150 0.18 19.68

Table4:Experimentalresultsofthermalexpansion

Temperature(⁰C)

ThermalExpansion Theoretical(mm) Experimental(mm) 50 0.01 0.03 80 0.023 0.06 100 0.032 0.08 150 0.05 0.18 200 0.07 0.25 225 0.08 0.33

ComparisonofTheoreticalandExperimentalresult

Figure6.Acomparisonbetweentheoreticalandexperimentalmeasuredresults

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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056

Volume: 09 Issue: 09 | Sep 2022 www.irjet.net p-ISSN: 2395-0072

Reasons for getting difference between theoretical and experimental results:

Fromfigure,itisobservedthatthereisdifferencebetweentheoreticalandexperimentalexpansionvalues,itisbecause ofroleofheatingtimeingettingexpansion. 

Inexperimentalmethod,expansionobtainedismorebecauseofheatingtimeisgettingmoreforeverytime.  Moreheatenergyistransferredtomaterial,soexpansionismore.

Mathematical Modelling of Friction Force:

Frictionorfrictionalforceisdefinedastheforcethatresistsanobject’smotiononasurface.Theobjectcaneitherbestationary orinmotionrelativetothesurface.Frictionoccurswheretheobjectisincontactwiththesurface.Inotherwords,ittakesplace betweentwosurfaces,andhence,isacontactforce.

Figure7.SchematicofShrinkfitassembly

The“coulombfriction”modelisusedformodellingtangentialforcesbetweencontactsurfaces.Iftangentialforcesarelower thanfrictionforcesµN,theywillbeproportionaltotherelativedisplacementbetweenthecontactsurfaces.Iftheyarelarger, thecontactsurfacesstarttoslipandthetangentialforceswillequalthefrictionforces.Thisconditioniscalledas“macro-slip" model. Sotoavoidthisphenomenonincaseofrotorshaftshrinkfitassembly,frictionalforceshouldbegreaterthanthe tangentialforce.Thentherewillberelativedisplacementbetweenrotorandshaft.

ThecontactpressurebetweenrotorandshaftinvolvedininterferencefitisgivenbytheLame´sequation:

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                     i i i i o o o o R R R R E R R R R R E R p    2 2 2 2 2 2 2 2 Where, p =contactpressurebetweenrotorandshaftduringassembly(Pa) δ=Radial
(m) R=
Ro=
Ri=
interference
Outsideradiusofshaft(m)
Outsideradiusofrotor(m)
Insideradiusofshaft=zero(solidshaft)

International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056

Eo =Modulusofelasticityofrotor(Pa)

Ei =Modulusofelasticityofshaft Pa)

γ0=Poisson’sRatioforrotor

γi=Poisson’sRatioforshaft 

Maximumfrictionalforcedevelopedduetocontactpressure:

FF = p ×2π×R×L×µ

Where, p =contactpressure(Pa)

R=Radiusofshaft(m)

µ=Coefficientoffrictionbetweenrotorandshaft

L=Lengthofcontact(m) 

Tangentialforcegivenbymotor:

Torque=Tangentialforce×radiusofshaft

T=FT ×R

Where, T=Motorstartingtorque(Nm)

FT =TangentialForce(N)

R=Radiusofshaft(m)

Iffrictionalforceisgreaterthantangentialforcethenshaftcantransmitthespecifiedpowerofmotorandinterferencefitis suitableforrotorshaftassembly.

Conclusion: 

Heatingfrominsideoftherotorborecanbeabetteroptionforheatingrotortogetquickerexpansionofrotorbore. 

Incaseofheatingrotorbore,heatingwillbeonlylocalheating.Onlyrequiredpartisheatedandexpanded. 

Thismethodgivespossibilityofavoidingcoolingofassembly,soitcouldremovecoolingoperationalltogether.

Future Scope:

Someopportunitiesforfutureworkonpresentdissertationworkareoutlinedasfollows:

Heatingfromborediametercanbeachievedbysuitablydesignedinductioncoilthatfitsintobore.  Studytheeffectofvaryingthesizeandshapeoftheinductionheatingcoilincaseofexternalheatingoftherotor.  Addasleeveofhighlyconductivematerialtotheinnersurfaceoftherotorsothatitexpandseasily.

References:

1. Fiji Toma, Optimization of rotor shaft shrink-fit method for motor using ‘‘Robust design,’’ Journal of Industrial EngineeringInternational(2018),pp.705–717

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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056

2. Mitesh. S. Agrawal, Ankit. M. Rathi, Prof. Prashant. B. Shiwalkar, ‘Algorithm in Automated Press Fit for Rotor Shaft AssemblyofanInductionMotor’,IJIRSET,Vol.5,Issue11,November2016,pp.20143-20149.

3. NazımArda Eyyuboğlu, ‘Investigationofthe Parameters Affecting CrankshaftandRotor Interference Fit’, school of mechanicalengineering,2014,pp.1-10.

4. SomnathKolgiri,“StaticandDynamicAnalysisforRotorShaftofElectricMotor”,(2009),pp.1-17.

5. J.D.BookerandC.E.Truman,MEASURINGTHECOEFFICIENTOFFRICTIONFOR USEINSHRINK-FITCALCULATIONS, DepartmentofMechanicalEngineering,UniversityofBristol,UK,November2009,pp.7-13.

6. Truman,C.E.,andBooker,J.D.,‘‘AnalysisofaShrink-fitFailureonaGearHub/ShaftAssembly,’’EngineeringFailure Analysis14(4):557–572(2007).

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