On the Modeling and Simulation of Friction

  • 格式:pdf
  • 大小:574.51 KB
  • 文档页数:6

TA88:30

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

*

.--