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Bearing Dynamic Coefficients in Rotordynamics
Computation Methods and Practical Applications
Łukasz BreńkaczInstitute of Fluid Flow MachineryPolish Academy of SciencesGdańsk, Poland
This Work is a co-publication between John Wiley & Sons Ltd and ASME Press.
© 2021 John Wiley & Sons LtdThis Work is a co-publication between John Wiley & Sons Ltd and ASME Press
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Library of Congress Cataloging-in-Publication Data
Names: Breńkacz, Łukasz, author.Title: Bearing dynamic coefficients in rotordynamics : computation methods and practical applications / Łukasz Breńkacz.Description: First edition. | Hoboken, NJ : Wiley, 2021. | Includes bibliographical references and index. Identifiers: LCCN 2020053700 (print) | LCCN 2020053701 (ebook) | ISBN 9781119759263 (hardback) | ISBN 9781119759249 (adobe pdf) | ISBN 9781119759171 (epub) | ISBN 9781119759287 (obook) Subjects: LCSH: Rotors–Dynamics. | Bearings (Machinery) Classification: LCC TJ1058 .B74 2022 (print) | LCC TJ1058 (ebook) | DDC 621.8/2–dc23 LC record available at https://lccn.loc.gov/2020053700LC ebook record available at https://lccn.loc.gov/2020053701
Cover Design: WileyCover Image: © photosoup/iStock/Getty Images
Set in 9.5/12.5pt STIXTwoText by SPi Global, Pondicherry, India
10 9 8 7 6 5 4 3 2 1
vii
Contents
List of Figures x List of Tables xviPreface xviiSymbols and Abbreviations xixAbout the Companion Website xxi
1 Introduction 11.1 CurrentStateof Knowledge 11.2 Reviewof theLiteratureon NumericalDeterminationof DynamicCoefficients
of Bearings 61.3 Reviewof theLiteratureon ExperimentalDeterminationof DynamicCoefficients
of Bearings 71.4 Purposeand Scopeof theWork 10
2 PracticalApplicationsof BearingDynamicCoefficients 142.1 SingleDegreeof FreedomSystemOscillations 16
2.1.1 Constant excitationForce 182.1.2 Excitation byUnbalance 202.1.3 Impactof Dampingand Stiffness 24
2.2 Oscillationof Masswith TwoDegreesof Freedom 262.3 Cross-CoupledStiffnessand DampingCoefficients 282.4 Summary 33
3 Characteristicsof theResearchSubject 343.1 BasicTechnicalDataof theLaboratoryTestRig 343.2 Analysisof RotorDynamics 363.3 Analysisof theSupportingStructure 423.4 Summary 44
4 ResearchTools 464.1 TestEquipment 464.2 Test.LabSoftware 494.3 SamcefRotorsSoftware 514.4 MatlabSoftware 51
Contentsviii
4.5 MESWIRSeriesSoftware(KINWIR,LDW,NLDW) 524.6 AbaqusSoftware 53
5 Algorithmsfor theExperimentalDeterminationof DynamicCoefficientsof Bearings 55
5.1 Developmentof theCalculationAlgorithm 555.2 Verificationof theCalculationAlgorithmon theBasisof aNumericalModel 585.3 Resultsof Calculationsof DynamicCoefficientsof Bearings 625.4 Summary 64
6 Inclusionof theImpactof anUnbalancedRotor 656.1 CalculationScheme 656.2 Definitionof theScopeof Identification 676.3 Resultsof theCalculationof DynamicCoefficientsof BearingsIncludingRotor
Unbalance 686.4 Summary 69
7 SensitivityAnalysisof theExperimentalMethodof DeterminingDynamicCoefficientsof Bearings 70
7.1 Methodof CarryingOuta SensitivityAnalysis 707.2 Descriptionof theReferenceModel 717.3 Influenceof theStiffnessof theRotorMaterial 717.4 Influenceof UnevenForceDistributionon TwoBearings 727.5 Changingthe Directionof theExcitationForceand itsEffecton theResults
Obtained 757.6 EddyCurrentSensorDisplacementImpactAssessment 767.7 CalculationResultsfor anAsymmetricalRotor 777.8 Summary 79
8 ExperimentalStudies 818.1 SoftwareUsedfor Processingof Signalsfrom ExperimentalResearch 828.2 SoftwareUsedfor Calculationsof DynamicCoefficientsof Bearings 838.3 Preparationof ExperimentalTests 858.4 Implementationof ExperimentalResearch 878.5 Processingof theSignalMeasuredDuringExperimentalTests 918.6 Resultsof Calculationsof DynamicCoefficientsof HydrodynamicBearingson the
Basisof ExperimentalResearch 938.7 Verificationof ResultsObtained 988.8 Summary 100
9 NumericalCalculationsof BearingDynamicCoefficients 1029.1 Methodof CalculatingDynamicCoefficientsof Bearings 1029.2 Calculationof DynamicCoefficientsof BearingsUsinga Methodwith Linear
CalculationAlgorithm 107
Contents ix
9.3 CalculationofDynamicCoefficientsofBearingsUsingaMethodwithNon-linearCalculationAlgorithm 113
9.4 Verificationof ResultsObtained 1199.5 Summary 123
10 Comparisonof BearingDynamicCoefficientsCalculatedwith DifferentMethods 125
11 Summaryand Conclusions 129
AppendixA 134AppendixB 145AppendixC 152ResearchFunding 155References 156Index 163
x
Figure 1.1 Lubricationfilmmodelforsmalljournaldisplacement. 3Figure 1.2 Methodsofanalysisfor(a)smalland(b)largedisplacementofthe
journal. 6Figure 2.1 Bearingaspartofarotatingsystem.Questionmarksindicatetheplaces
wheredynamiccoefficientsofbearingsoccur. 15Figure 2.2 Differentbearingmodels:(a)oscillatingmasswithonedegreeof
freedom;(b)bi-directionaloscillatingmass(twodegreesoffreedom);and(c)bi-directionaloscillatingmasswiththeinclusionofcross-coupledstiffnessanddampingcoefficients. 16
Figure 2.3 Displacementofthemassattachedtoafixedsupportbymeansofstiffnessanddampingcoefficientsasaresultofaconstantforce. 18
Figure 2.4 Theeffectofachangeinthedampingcoefficientsonthedisplacementofthemasspointwhichisbeingactedonbyaconstantforce.Thearrowsrepresentthedirectionofdisplacementchangeduetotheincreaseofdampingcoefficientvalues. 19
Figure 2.5 Theeffectofachangeinthestiffnesscoefficientsonthedisplacementofthemasspointwhichisbeingactedonbyaconstantforce.Thearrowsrepresentthedirectionofdisplacementchangeduetothedecreaseofstiffnesscoefficientvalues. 19
Figure 2.6 Asingledegreeoffreedomsystemwithharmonicexcitation. 20Figure 2.7 Theeffectofachangeinthedampingcoefficientsonthedisplacement
ofthemasspointwhichisbeingactedonbyaconstantharmonicwithafrequencyof300Hz. 21
Figure 2.8 Theeffectofachangeinthestiffnesscoefficientsonthedisplacementofthemasspointwhichisbeingactedonbyaconstantharmonicwithafrequencyof300Hz. 22
Figure 2.9 Excitationforceofconstantvalueandofvariablevaluechangingalongwithfrequency. 23
Figure 2.10 TherelationshipbetweentheexcitationforcefrequencyandtheamplitudeofthesystemresponseforaconstantforceF. 23
Figure 2.11 TherelationshipbetweentheexcitationforcefrequencyandtheamplitudeofthesystemresponsefortheforceFvariablealongwithfrequency. 24
List of Figures
List of Figures xi
Figure 2.12 Impactofdampingcoefficients. 25Figure 2.13 Impactofstiffnesscoefficients. 25Figure 2.14 Impactofmasscoefficients. 26Figure 2.15 Areasofinfluenceofdifferenttypesofcoefficientsforvariable
amplitudevaluesofexcitationforce. 26Figure 2.16 Areasofinfluenceofdifferenttypesofcoefficientsfortheconstant
amplitudeofexcitationforce. 27Figure 2.17 Combinationofoscillationintwodirectionstakingintoaccountthe
mainstiffnessanddampingcoefficientsofthebearing. 27Figure 2.18 Two-directionaldisplacementandtrajectories:(a)
cxx = cyy =6400N·s/m;(b)cxx·2;and(c)cyy·2. 29Figure 2.19 Combinationofoscillationintwodirectionstakingintoaccountthe
mainandcross-coupledstiffnessanddampingcoefficientsofthebearing. 30
Figure 2.20 Trajectorychanges:(a)cxyandcyx =0N·s/m;(b)cxy=0N·s/mandcyx =6400N·s/m;and(c)cxy =0N·s/mandcyx =6400N·s/m. 31
Figure 2.21 Trajectorychanges:(a)kxyandkyx =0N/m;(b)kxy=6630000N/mandkyx =0N/m;and(c)kxy=0N/mandkyx =6630000N/m. 32
Figure 3.1 Photographofthelaboratorytestrig. 35Figure 3.2 Diagramofthelaboratorytestrig. 35Figure 3.3 (a)Hydrodynamicbearingand(b)bearingdiagram. 36Figure 3.4 Run-upofthelaboratorytestrig;during66.4secondsthespeedwas
increasedlinearlyfrom1000to8400rpm. 37Figure 3.5 Maximumdisplacementoftherotorjournals. 37Figure 3.6 Stableoperationofbearingsno.1(aandb)andno.2(candd)at
3250rpm;thediagramsshowthesignalrecordedinX(aandc)andY (b andd)directions;theshorttimeinterval(0.3seconds)showsapproximately8revolutions. 38
Figure 3.7 Stableoperationofbearingsno.1(aandb)andno.2(candd)at3250rpm;thediagramsshowthesignalrecordedinX(aandc)andY(bandd)directionsduring10seconds. 39
Figure 3.8 FFTanalysisofthestableoperationsignalfromeddycurrentsensorsbearingsno.1(aandb)andno.2(candd)at3250rpm;thediagramsshowthesignalmeasuredinX(aandc)andY(bandd)directions. 40
Figure 3.9 Trajectoryofbearingjournalmovementno.2duringstableoperationataspeedof3250rpm:(a)signalmeasuredbysensorsand(b)signalafterfilteringoperation. 41
Figure 3.10 Combinationofthevibrationtrajectoriesofasecondbearingoperatingonalaboratorytestrigfor(a)belowresonancespeed(3250rpm),(b)closetoresonancespeed(4500rpm),and(c)aboveresonancespeed(5750rpm). 41
Figure 3.11 Cascadediagrambasedontheaccelerometersignalplacedonsupportno.2 intheXdirection(horizontal);onthedrawingishighlightedtheresultoftheFFTanalysisatarotationalspeedof3000rpm(darkgrayhorizontalline). 42
List of Figuresxii
Figure 3.12 Thefirstformofnaturalvibrationsofthelaboratorytestrig. 44Figure 4.1 SCADASmobileanalyzer. 47Figure 4.2 (a)Eddycurrentsensorsplacedata90°angletoeachotherand
perpendiculartotherotoraxisand(b)moduleusedforprocessingsignalsfromeddycurrentsensors–demodulator. 47
Figure 4.3 (a)Accelerometerusedtomeasureaccelerationsofvibrationsofthebearingsupportsand(b)portableaccelerometercalibrator. 48
Figure 4.4 Impacthammer. 48Figure 4.5 (a)Speedmeasurementusingalasersensorand(b)fiberoptic
switch. 48Figure 4.6 TheVisionResearchPhantomv2512camera(right),theLEDlamps
usedforillumination(center),andthelaboratorytestrig(left). 49Figure 4.7 (a)MBJDiamond401 measuringdeviceusedforbalancingtherotor
and(b)theOPTALIGNSmartRSdeviceforshaftalignment. 50Figure 4.8 InterfaceoftheTest.Lab11Bsoftware. 50Figure 4.9 InterfaceoftheSamcefRotorssoftware. 51Figure 4.10 InterfaceoftheMatlabsoftware. 52Figure 4.11 InterfaceofGRAFMESWIR–agraphicalprocessoroftheNLDW
software. 53Figure 4.12 InterfaceoftheAbaqus/CAEsoftware6.14-2. 54Figure 5.1 (a)RotormodelintheSamcefRotorssoftwareand(b)bearingmodel. 56Figure 5.2 Diagramforthecalculationofdynamicbearingcoefficients. 59Figure 5.3 (a)ForceindirectionXasafunctionoftimeand(b)displacementof
bearingno.2asafunctionoftime. 61Figure 5.4 (a)Frequencydistributionofforceand(b)amplitudeofnodeno.2asa
functionoffrequency. 61Figure 5.5 Bearingno.1:(a)flexibilityamplitudeand(b)flexibilityphase. 61Figure 5.6 Thefirstformofnaturalvibrationsoftherotorat46Hz. 62Figure 6.1 Calculationschemeofdynamiccoefficientsofbearingsincluding
unbalance. 66Figure 6.2 (a)Stableoperationoftherotor–referencesignalinthebearingand(b)
amplitudeofvibrationsafterinducingtherotorbymeansofaimpacthammer–signalinthebearing. 66
Figure 6.3 (a)Amplitudeofvibrationsaftersubtractingthereferencesignalfromtheexcitationsignaland(b)fastFouriertransformofthissignal. 67
Figure 6.4 ThefastFouriertransformdisplacementsignalinbearingsforrotationalspeed(a)2800rpmand(b)10000rpm. 68
Figure 6.5 Dynamicflexibilityofbearings:(a)amplitudecourseand(b)phaseanglecourse. 68
Figure 7.1 Diagramshowingthesensitivityanalysisscheme. 71Figure 7.2 (a)Rotormodelonwhichthemethodofforcedisplacementismarked.
(b)BearingresponsesignalforthefirstbearingintheXdirectionafterinducingthesystemintheXdirection;comparisonafterexcitationinthemiddleandforcedisplacedbythevalues =30mm. 73
List of Figures xiii
Figure 7.3 (a)Modelshowinghowtheforceisappliedatanangleand(b)theresponsesignalofthefirstbearinginthe X and Y directionsafterexcitationatanangleofα =0°andα =15°. 75
Figure 7.4 Modelonwhichtheplaceofbearingdisplacementmeasurementwasmarked(systemswithpindexes)andplacestakenintoaccountduringcalculationofdynamiccoefficientsofbearings(meansofbearinghousings). 77
Figure 7.5 Diagramofanasymmetricalrotor. 78Figure 7.6 Responseofanasymmetricalrotorsystem. 78Figure 8.1 Programwindowforsignalpreparation;thediagramspresentedthe
datareadforasignalcorrespondingtoaspeedof4500rpmandexcitationintheYdirection. 83
Figure 8.2 Windowofthesoftwareusedforcalculationsofdynamiccoefficientsofbearings. 84
Figure 8.3 Photographshowingtheteststandduringtheshaftalignment. 86Figure 8.4 Photographshowingthetestedrotor. 86Figure 8.5 PhantomCameraControl,aprogramwindowforoperatingahigh-
speedcamera;afragmentoftherecordingofinducingtherotorwithaimpacthammercanbeseeninthebackground. 87
Figure 8.6 Calculationschemeofdynamiccoefficientsofbearings. 88Figure 8.7 Signalmeasurednearbearingno.2 intheYdirectionat4500rpmand
excitationwithaimpacthammerintheYdirection. 89Figure 8.8 ExcitationforcecurveintheYdirectionover20seconds;signalstored
at4500rpm. 89Figure 8.9 ExcitationforceintheXandYdirectionsover0.4ms;excitationat
4500rpm.(a)Valuesnotresetoutsidethemainpeakand(b)signalwithresetting. 90
Figure 8.10 Stablebearingoperationno.2(aandb)at4500rpmandsignalafterexcitation(candd);thegraphsshowthedisplacementsintheXdirection(aandc)andYdirection(bandd);thetimeofthesignalshowninthegraphsis0.1seconds. 91
Figure 8.11 AmplitudeofrotorvibrationsafterexcitationintheXandYdirectionsforthefirst(a)andsecond(b)bearings;thereferencesignalhasbeensubtractedfromthesignalaftertheexcitation. 92
Figure 8.12 Changesinthestiffnesscoefficientsofbearingno.2fortheentirespeedrange. 97
Figure 8.13 Changesinthedampingcoefficientsofbearingno.2fortheentirespeedrange. 97
Figure 8.14 Changesinthemasscoefficientsofbearingno.2fortheentirespeedrange. 97
Figure 8.15 Increasingvibrationamplituderecordedinbearingno.2duringoperationat4000rpmafterexcitationwithanimpacthammerintheYdirection. 98
Figure 8.16 Schematicmodelofmass,damping,andstiffness. 99
List of Figuresxiv
Figure 8.17 Comparisonofthedynamicresponseoftherealrotorandthenumericalmodel(themodeltakesintoaccounttheexperimentallydeterminedstiffnessanddampingcoefficients). 99
Figure 9.1 Coordinatesystemataselectedpointinthelubricationgap. 103Figure 9.2 Algorithmofcalculationofaradialhydrodynamicbearing. 108Figure 9.3 NumericalrotormodelintheKINWIRprogram. 109Figure 9.4 Numericalmodelofhydrodynamicbearing. 110Figure 9.5 Presentationofthepressuredistributioncalculatedforthestatic
equilibriumpointataspeedof3250rpmintheKinwirprogram. 110Figure 9.6 Bearingno.2stiffnesscoefficientscalculatedusingalinearalgorithmin
theKINWIRprogram. 112Figure 9.7 Bearingno.2 dampingcoefficientscalculatedusingalinearalgorithm
intheKINWIRprogram. 112Figure 9.8 Numericalmodeloftherotor,bearinganddiskintheNLDW
program. 113Figure 9.9 PressuredistributioncalculatedusingtheNLDWprogramfor(a–d)
4 journalpositions(in90°increments)at3250rpm. 114Figure 9.10 StiffnesscoefficientscalculatedintheNLDWprogramfor3rotor
revolutionsatarotationalspeedof3250rpm. 116Figure 9.11 DampingcoefficientscalculatedintheNLDWprogramfor3rotor
revolutionsataspeedof3250rpm. 116Figure 9.12 StiffnesscoefficientscalculatedintheNLDWprogramfor3rotor
revolutionsatarotationalspeedof3750rpm. 117Figure 9.13 DampingcoefficientscalculatedintheNLDWprogramfor3rotor
revolutionsataspeedof3750rpm. 117Figure 9.14 StiffnesscoefficientscalculatedintheNLDWprogramfor3rotor
revolutionsatarotationalspeedof5500rpm. 118Figure 9.15 DampingcoefficientscalculatedintheNLDWprogramfor3rotor
revolutionsataspeedof5500rpm. 118Figure 9.16 Bearingjournaldisplacementscalculatedusingthemethodwitha
linearcalculationalgorithm. 119Figure 9.17 BearingjournaldisplacementscalculatedusingtheNLDW
program. 120Figure 9.18 Vibrationtrajectoriesofthejournalofbearingno.2:(a)measured
duringexperimentaltests:(b)calculatedusingalinearalgorithm:and(c)calculatedusingtheNLDWprogram. 121
Figure 9.19 TheFFTanalysisofthesignalforaspeedof5750rpmbasedonexperimentaltestsinthedirectionof(a) X and(b)Y;analogousresultscalculatednumericallyforthelinearalgorithminthedirectionof(c) X and(d)Y;calculationsbymeansofanon-linearalgorithmintheNLDWprograminthedirectionof(e) X and(f)Y. 122
Figure 10.1 (a)Changeinjournalvibrationtrajectoryduetoe.g.increasedrotorunbalanceorchangesinbearingparameters(trajectory1,2,or3).(b)Trajectoryafterinducingabearingoperatingatastaticequilibriumpoint(Oc).Amodelshowingtheassumptionsoflinearoperationofthe
List of Figures xv
system.(c)Trajectoryafterexcitationduringoperationwithalargerellipseofvibrations.ThedottedlineshowsasampletrajectoryafterexcitationinpointOw.Afterashorttime,therotorjournalreturnstothepreviousconstantellipseonwhichitwasmovingearlier(shownbyacontinuousline). 127
Figure 11.1 Adiagramoftheworkcarriedout.Thedivisionintoexperimentaltestsandnumericalanalysesandtherelationshipsbetweenthevariouschaptersandsectionsofthemonographareindicated. 130
FigureA.1 FastFouriertransform(FFT)diagramsofthefirstandsecondbearingsintheXandYdirectionsforrotationalspeedsof2250–3000rpm. 135
FigureA.2 FFTdiagramsofthefirstandsecondbearingsintheXandYdirectionsforrotationalspeedsof3250–4000rpm. 136
FigureA.3 FFTdiagramsofthefirstandsecondbearingsintheXandYdirectionsforrotationalspeedsof4250–5000rpm. 137
FigureA.4 FFTdiagramsofthefirstandsecondbearingsintheXandYdirectionsforrotationalspeedsof5250–6000rpm. 138
FigureA.5 Vibrationtrajectoryofthefirstbearingfor16rotationalspeeds,from2250to6000rpm. 139
FigureA.6 Vibrationtrajectoryofthesecondbearingfor16rotationalspeeds,from2250to6000rpm. 140
FigureA.7 Cascadediagramofanaccelerometerplacedonsupportno.1 intheXdirection(horizontal). 141
FigureA.8 Cascadediagramofanaccelerometerplacedonsupportno.1 intheYdirection. 141
FigureA.9 Cascadediagramofanaccelerometerplacedonsupportno.2 intheXdirection. 142
FigureA.10 Cascadediagramofanaccelerometerplacedonsupportno.2 intheYdirection. 142
FigureA.11 Shaftalignmentreport–partone. 143FigureA.12 Shaftalignmentreport–parttwo. 144FigureC.1 Vibrationtrajectoriescalculatedforthesecondbearingusingalinear
algorithmbasedontheKINWIRandLDWprograms. 153FigureC.2 Vibrationtrajectoriescalculatedforthesecondbearingusinganon-
linearalgorithmintheNLDWprogram. 154
xvi
List of Tables
Table 3.1 Successiveeigenfrequenciesand thecorrespondingdampingvaluescalculatedfor thelaboratorytestrig. 43
Table 5.1 Parametersof thenumericalmodel. 59Table 5.2 Stiffnesscoefficients. 60Table 5.3 Dampingcoefficients. 60Table 5.4 Masscoefficients. 63Table 7.1 Summaryof therealand calculatedstiffness,dampingand mass
coefficientsfor thetwobearingsfor thereferencecase;representationof therelativecalculationserror. 72
Table 7.2 Summaryof therealand calculatedstiffness,damping,and masscoefficientsfor thetwobearingsfor acasewith displacedforce;results“withcorrection”takeintoaccountthe unevendistributionof excitationforcein thecalculationprocedure. 74
Table 7.3 Summaryoftherealandcalculatedstiffness,dampingandmasscoefficientsforthetwobearingsforacasewithanexcitationatanangleofα =15°. 76
Table 7.4 Summaryof therealand calculatedstiffness,dampingand masscoefficientsof twobearingsfor anasymmetricalrotor. 78
Table 8.1 Stiffness,dampingand masscoefficientsof therotor–bearingsystemfor theentirespeedrange. 95
Table 8.2 Standarddeviationof stiffness,dampingand masscoefficientsof therotor–bearingsystemfor theentirespeedrange. 96
Table 9.1 Parametersof thenumericalmodelin theKINWIRprogram. 109Table 9.2 Stiffnessand dampingcoefficientsobtainedfrom linearcalculations
in theKINWIR. 111Table 9.3 Minimumand maximumvaluesof stiffnesscoefficients(N/m)
calculatedin theNLDWprogram. 115Table 9.4 Minimumand maximumvaluesof dampingcoefficients(N·s/m)
calculatedin theNLDWprogram. 115Table 10.1 Comparisonof thecalculatedstiffnessand dampingcoefficientsfor the
threemethodsusedfor aspeedof 3000rpm. 126
xvii
This monograph concerns the experimental and numerical methods of determination of dynamic coefficients of hydrodynamic radial bearings. Bearings are one of the basic ele-ments influencing the dynamics of rotor machinery. The main parameters with which the operation of bearings can be described (and thus the operation of the entire rotating sys-tem) are their stiffness and damping coefficients.
This book includes a chapter about practical applications of bearing dynamic coeffi-cients. It is shown how changes of bearing dynamic coefficients affect the dynamic perfor-mance of rotating machinery. Some examples are included with all the necessary data to allow rotordynamics analysis to be conducted and the dynamic coefficients of journal bear-ings to be calculated so that the readers can replicate the results presented in this book and compare them with their own results. This book presents in detail an experimental method of determining dynamic coefficients of bearings. An additional objective is to describe numerical methods of determining dynamic coefficients of hydrodynamic bearings (linear and non-linear). The range of applicability of various calculation methods was determined based on measurements made for a rotating machine equipped with hydrodynamic bear-ings with clearly non-linear operating characteristics.
Experimental research was carried out with the use of the impulse method, on the basis of which dynamic parameters of hydrodynamic bearings were determined. The applied method with a linear calculation algorithm allows the determination of stiffness and damp-ing coefficients and the determination of mass coefficients in one algorithm. The stiffness and damping coefficients cannot be determined directly, thus indirect calculation methods are used. The mass of the rotor is a directly measurable parameter. Indirectly calculated mass coefficients can be compared with the known mass of the rotor. On this basis, it is possible to make preliminary estimations of the correctness of the results obtained.
As part of the study, the sensitivity analysis of the aforementioned experimental method was carried out with the use of a model created in Samcef Rotors software. The influence of unbalance, displacement of measuring sensors, and various variants of driving force were analyzed. Based on experimental research, dynamic coefficients of hydrodynamic bearings in a wide range of rotational speeds, taking into account resonance speeds and higher speeds, were determined. They were verified using Abaqus software.
Numerical calculations of stiffness and damping coefficients of hydrodynamic bearings with the use of linear and non-linear calculation models developed by IMP PAN in Gdańsk were also carried out. The obtained results were verified. The stiffness and damping
Preface