VehicleDynamicsFHRegensburg,UniversityofAppliedSciences
Withtheaccordingapproximationforthecosine-function
rS1
=cos =1 2or 2=2r02
one nallygets
rS
1
r0
(2.7)
rD=r0
remains.
11
3
rS1
r0
=
21r0+rS33
(2.8)
TheradiusrDdependsonthewheelloadFzbecauseofrS=rS(Fz)andthusisnamed
dynamictireradius.Withthis rstapproximationitcanbecalculatedfromtheundeformedradiusr0andthesteadystateradiusrS.By
vt=rD
(2.9)
theaveragevelocityisgivenwithwhichtreadparticlesaretransportedthroughthecontactarea.
2.2.2ContactPoint
Thecurrentpositionofawheelinrelationtothe xedx0-,y0-z0-systemisgivenbythewheelcenterMandtheunitvectoreyRinthedirectionofthewheelrotationaxis,
Fig.2.3.
Figure2.3:ContactGeometry
Theirregularitiesofthetrackcanbedescribedbyanarbitraryfunctionoftwospatialcoordi-nates
z=z(x,y).(2.10)
16