On the Modeling and Simulation of Friction
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OntheModelingandSimulationofFriction
DavidA.Haessig,Jr.
PlesseyElectronicSystemsCorporation
Wayne,NJBernardFriedland
NewJerseyInstituteofTechnology
Newark,NJ
Abstract
TwonewmodeLsfor"slp-stick
ionarepresented.One,called
the"bristle
model,"isanapprxiationdesigned
toapturetheps-
ical
phenomenonofsticking.This
modelisrelativelyinefficent
nu-
mericaly.The
othermodel,calledthe"resetintegratormodel,"
does
notCapturethedetailsofthesticingphenomenon,butisnumeri-
callyefficient
andexhibitsbehaviorsimilar
tothemodelpropoedby
Karnoppin1985.Allthreeofthesemodelsarepreferable
tothecas-
sical
modelwhichpoorly
representsthefriction
force
atzerovelcdty.
Simulationexperiments
showthatthe
newmodelsandtheKarnopp
modelgivesimflarresultsin
twoexamplesIn
adosed-loopexample,
theclassical
modelpredktsamimitcyclewhichisnotobservedinthe
laboratory.Thenewmodeis
andtheKarnoppmodel,
ontheother
hand,agreewiththeexperimentalobserntio.
Introduction
Frictionis
thenemesis
ofprecision
controLItdefiesanalysis
andfols
theapplicationofthe
bestmoderndesignmethods.Becausefrition
doesnotreadilyyield
torigorousmathematcl
treatmentitisof-
tenregardedasaphenomenonunworthy
ofincusion
in
thecaon
ofcontroltheory.Neverthekssitisresponsible
for
manyproblems
assoclated
withthecontrolandaccracy
ofmechanial
systems.It
can,forexample,
causethemoving
body
to"Jitter"during
motionin
anyonedirection;
it
cancausebrgetrackig
errorswhenchanging
direction;
anditisalsoknown
tocauselimitcycling
about
afinal
po-
sition.Thesepractical
problemsnotwithstanding,theengineer
who
has
tofacetheeffectsoffrictionintherealworldlacksthetools
to
makeiteasiertodealwith.
Thetpeoffrictionthatthis
paperdealswithisgenerayclled
"coulombfrition,"
or"slip-stickfriction".Ts
sortoffritionisrep-
resented
asaforcethatis
anonlinearfunctionof
therelativelcoc-
ityof
twobodiesin
contactOnthemicroscopic
level,thesurface
ofeachbody
canbeimagined
asconsistingof
arangeofmountains
that
isinterposedagint
aninrted
mountain
rangeontheother
surface,
asshowninFR
1.lbe(aerage)heightofthemountain,
thedegreeofinterpenetration,
andthe(average)distancebetwee
thepeaks
depend
onphysicalcharacteristimofthematerialsandthe
lubriatingmedium.Thescienceoftnboog
hascontributedmuch
toreductionoffriction,
Le.,
toreducing
themountin
tofoothis,
buthow
todealeffetively
withthefoothlsstiremais
aprobiem-Sincethesurfaceirregulariies
aregenerallythought
toberan-
dom,anaccuraterepresentationoffrictio
wouldentailue
ofthe
theory
ofrandomprocesses.Moreovr,
whentwomountainscome
intooDntacttheforcebetwen
theminitiallyresembles
thatofastiff
spring-damper
system.Assldingcontinue
encrgyislst
toplastic
deformation.
Itfollows,therefore,
thattheforceshould
bercpr
sentedasafunctionofpositionratherthanvelocity.
In
somccasme
itisbelievedthtthereisactuallyamokleurbondingbetweenthe
surfaces
Suchabondwoudaowwerylittlemotionbetweenthetwo
contactingbodies
andthus
thespring
would
appearverystiff.In
the
absenceofmolecularbondingtherelative
motioncouldbesubstan-
tiallylargerandthe
spring
rateloer.
Thedevelopmentof
amodel
thatfaithfuly
butefficientlydescibes
theposiion
dependencythat
could
existduringthis"sticking
phase
offriction,andalsorepresents
thevekocty
dependencyduring"sipping,"
isthepurpseofthceffort
described
herein.
Theelementyrepresentation
offriction
asafunction
ofonly
therelativeveocty
V,
betweenthetwooontactingsurfaces
asshown
inFig.
ZSlip-stikfrictiDn
is
apanicular
typeoffriction
thatishighly
nonlnear
atthepointVr
=0.Atthatpointthisfuncion
ismultival-
ued,whichimpiesthatthefritionforewillassumewhatevervalue
intherangeI-FH,FH,]
thatisnecesary
tokeepthecontactingsur-
facesfromsliding.Tis
effeais
arepresentationof"sticing."
This
function
abosowsthattheforce
canbelarger
atVr
=O
thanthatof
nonzeroveloit,which
isoftencalled"stition."
Only
ifthemag-
nitudeoftheexernal
forces
exceedthepeakstiction
forceFH,,will
thebodybegin
toslide.
f
FH
VI
-F,
Fig
2.StandardSlip-StickFrictionModel
Thedicntinuity
attheorigin
isphysicaly
unrealistic
andunac-
ceptable
forpurposesofsimulatio.
Oneapproachtoovercoming
thediscntinuity
hasbeentoapproximate
itby
anear
regionas
shownin
Fig.3.hiapp
tionresuls
in
whatiscommonly
knownasthe"cassical(coulomb)riction
modeL"Buttheproblem
withthismodelisthatitallow
thebodytoaccelerate
eventhough
theextenalforce
onthebodyareles
than
thepeaksttion
force
F,,.
Thismodel,therefore,canot
beexpected
toaccuratelypredict
limitcyclig
orothereffecasociated
withthesticingphenomena.
Also,the
verysteep
slopearoundV7
Ocanresultin
veryshortinte-
grationtime
stepsandnumericaldifficuis.
improvementsaver
thecsicalfriction
modelhavebeenpro-
posedbyDahl[11,
byBo,PavecKu
[21,
and
byKamechi[3I
but,like
theclassicalmodel,
thesemodel
donotinclude
amechanismfor
rep-
resentingthe
zerovelocityfricion
forcethatonn
duringstickdng.
1256FHg
1.MicroscopicViewofFrictionPhenomenonI
*
.--