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Tyres – The Basics for Recent

Development

Prof. R. Krishna Kumar

Department of Engineering Design

Indian Institute of Technology Madras

Acknowledgement





JK Tyres for sponsoring the largest

project from a private company to

an educational Institution in India

Tyre as a Vehicle Component

• Support the load during dynamic and static

conditions – Filter vibrations in vertical

dynamics

• Traction and Braking support during

longitudinal dynamics

• Key role in Lateral Dynamics – Cornering force

and Moments

• Key gas guzzler and a fantastic replacement

market

Low Rolling Resistance Tyres Green Tyre







Run Flat Tyres Low Aspect Ratio - Radial Tubeless - Radial









Low Aspect Ratio - Bias Tubeless - Bias All Steel Radials







Radial Tyre – Aramid belt Radial Tyre – Steel belt Radial Tyre – Textile belt









Tyre with cotton reinforcement Rayon reinforcement Nylon reinforcement

Wheel Radius = Rim Radius + hT

+1 concept

Passenger Radial Tyre Layout





Inner Liner

Body Ply

Belt-1

Belt-2

Tread





Bead

Chaffer

Filler

Cap Strip

Sidewall

Rim Strip

Truck Radial Tyre

Radial Tyre









Bias Tyre

Radial vs Bias









• How does the tyre transmit load?

Tread Pattern

Tyre Terminologies

• Normal Stiffness

• Longitudinal stiffness

• Longitudinal Slip Stiffness

• Lateral Stiffness

• Cornering Stiffness

• Camber Stiffness

• Self Aligning Moment

• Twisting Moment

• Relaxation Length

• Rolling Resistance

What is Slip ?









Tyre during Braking

Slipping is not skidding









Slip is a micro movement and skid is a macro movement

Vx   re

Longitudinal Slip,  

Vx

Characterizing Longitudinal Force







Range of Operation









Longitudinal Force Coeff., = F / N



Longitudinal Force, F = (kκκ)N = Kκκ



Kκ is called the dimensional stiffness of longitudinal slip.

kκ is called the longitudinal slip stiffness.

These stiffness need not be the same in braking and driving

How does the friction develop







Elastic Visco-elastic

•The loading and the unloading path are not the same – hysteresis

•Hysteresis central to the grip mechanism or friction

Molecular Adhesion – The other

mechanism for grip

Note the decrease

Lateral Force Development

Combined Forces

Rolling Resistance









Fw= fwN = (d / R ) N



fw is called the rolling friction coefficient

0.018 1.59 106 2

f w  0.0085   V for V  165 kmph

p p

0.018 2.91106 2

fw   V for V  165 kmph

p p

Axi Symmetric Model (24-35)

22 plies and

TYRE OD NSD Tread 2 Breakers

Width

OTR 2204 58 550

Full 3D-Model of the Tyre

CPRESS : Simulation vs. Experiment

Contact Pressure Distribution: Rolling

Temperature and Rolling Resistance

filler bead

7% 0%





ply

Contribution of dissipation at 18%



different tyre regions

belt

tread

4%

55%

rs

6%





sw

10%









Variation of tread material loss modulus

Temperature distribution contours

Tread with

Smooth tread

circumferential grooves

RR = 100.1267 RR = 106.3685









Temperatures and Rolling Resistance with Speed

TBR – Temperature Distribution

Mathematical Modelling

Vehicle Road

Data Parameters









Road

Vehicle Model

model









Tyre

Characteristics





Tyre Model

Vehicle Model









A set of degrees of freedom, represented as a vector

A set of location points called hard points

A set of properties, such as Mass and Moment of Inertia

A set of Input Forces from the Environment

Multibody Dynamics Equation









A set of Constraint Equations, Φ

Differential – Algebraic

Equations







Tyre Model Numerical Solution

Fx = F(σ, N, α, …)

Fy = F(σ, N, α,γ …)

M = F(σ, N, α,γ …)

Why does one want to do Vehicle

Dynamics Simulation

• Handling & Stability

• Ride Analysis

• Durability

• Roll Over Stability

• Suspension fine tuning

• Active Suspension Development

• NVH

Is the Tyre Model the Same for all these analysis?

NO !

Tyre Models in Vehicle Dynamics

Classification of Tyre Models

Simple Tyre Models: Fiala Model

•Tyre modelled as a linear springs.

•Longitudinal / Lateral forces defined by a linear relationship.

•No Combined Slip.

•Only Low Frequency Behaviour



Approximation / Empirical Models: “Magic Formula” Model

•Non Linear Approximation of Tyre Force

•Combined Slip

•Can be combined with vertical Stiffness

•Applications restricted by frequency

•Short Wave length Roads are not taken into account





Physical and Semiphysical Models: “Brush Models”

•Can be used for high Frequencies

•Takes into account tyre belt vibrations

•Road Envelopes are considered – A tyre road contact model

Tyre Models in the Market

• 20 different tyre models in the market

• MF group of tyre models, SWIFT model etc.

• RTire and FTire models etc.

• RMOD-K Model

• There are two issues: Measurements and

Representation – Includes tyre and Road

Measurement data

• For many models the procedure is established, but

mathematics is very complex

Magic Formula Tyre Model

y = D sin[C arctan{Bx – E(Bx – arctan Bx)}]



with Y(X) = y(x) + SV

x = X + SH



where Y : Fx or Fy or Mz



X : slip angle tan or slip 

and B – Stiffness Factor

C – Shape Factor

D – Peak Value

E – Curvature Factor

SH – Horizontal Shift

SV – Vertical Shift



B, C, D, E, SH and SV are known as primary MF parameters.



Conicity and plysteer represent tyre cornering behaviour at diminishing slip angle.

These are represented through horizontal shift SH and vertical shift SV.

The primary Coeff., depend on normal load, camber etc.

Force and Moment Characteristics





FEA Experiments FEA

-6000 80

-5000 70

Lateral force (N)









Self-aligning torque

Experiments

60

-4000

50

-3000 40









(Nm)

30

-2000

20

-1000 10

0 2 4 6 8 10

0

0

Slip angle (Deg) -10 0 2 4 6 8 10

-20 Slip angle (Deg)









8000

Longitudinal Force (N)









7000

6000

5000

4000

3000 Experiments FEA

2000

1000

0

0 5 10 15 20 25 30



% Slip

Thank You for Your Attention



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