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Lecture notes on tire modelling - University of Waterloo

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An Introducti<strong>on</strong> to Tire Modelling<br />

for Multibody Dynamics Simulati<strong>on</strong><br />

SD 652<br />

Pr<strong>of</strong>essor John McPhee<br />

<strong>University</strong> <strong>of</strong> <strong>Waterloo</strong><br />

March 2013


Acknowledgement:<br />

Kevin Morency, Automatic Generati<strong>on</strong> <strong>of</strong><br />

Real-Time Simulati<strong>on</strong> Code for Vehicle<br />

Dynamics using Linear Graph Theory<br />

and Symbolic Computing, MASc Thesis,<br />

<strong>University</strong> <strong>of</strong> <strong>Waterloo</strong>, 2007


SAE Axis System


ISO Axis System


Rolling Resistance (M y )<br />

Produced by hysteresis in <strong>tire</strong> tread<br />

and sidewall rubber<br />

M y = (Fz)(δx)


Braking Force (F x )<br />

S = (V – wR) / V<br />

0 < S < 1


Braking Force (F x )<br />

S = (V – wR) / V<br />

0 < S < 1<br />

L<strong>on</strong>gitudinal Stiffness, C S , is the slope <strong>of</strong><br />

the F x vs. S curve at S=0


Driving Force (F x )<br />

S = (wR-V) / wR<br />

0 < S < 1


Lateral Force (F y ) and<br />

Aligning Moment (M z )


Lateral Force (F y ) and<br />

Aligning Moment (M z )<br />

Cornering Stiffness, C α , is the slope <strong>of</strong> the<br />

F y vs. α curve at α=0


Effect <strong>of</strong> Camber Angle (γ)<br />

<strong>on</strong> Lateral Force (F y )


Combined Slip (F x AND F y )


Overturning Moment (M x )


Characterizing a Pneumatic Tire:<br />

Physical Testing


Characterizing a Pneumatic Tire:<br />

Physical Testing


Data From Physical Tests<br />

C<strong>on</strong>sider how Fx varies with S: Fz, 20 and S,α, data S: γ : 20 20 points 24 =<br />

160 400 000 data data points points<br />

x5 = 800 000 data points


Tire Models:<br />

Mathematical Functi<strong>on</strong>s to Fit Measured Data<br />

Fiala: 6 parameters needed to describe a <strong>tire</strong><br />

•Easy to understand the physical significance <strong>of</strong> all parameters<br />

•Simple force and moment equati<strong>on</strong>s.<br />

•Does not handle combined slip<br />

•Effects <strong>of</strong> normal force and camber are largely ignored.<br />

Pacejka 2002 : 117 parameters needed<br />

•Very good fit to experimental data<br />

•More complicated force and moment equati<strong>on</strong>s


How Tire Forces are Included In<br />

Multibody Vehicle Model<br />

1. Define a point where <strong>tire</strong> forces and<br />

moments will act <strong>on</strong> the multibody model<br />

C2<br />

C1<br />

P<br />

2<br />

P<br />

1


How Tire Forces are Included In<br />

Multibody Vehicle Model<br />

2. Determine an expressi<strong>on</strong> for the vertical <strong>tire</strong><br />

force, Fz, which is required as an input to the<br />

<strong>tire</strong> model.


How Tire Forces are Included In<br />

Multibody Vehicle Model<br />

3. Establish vector directi<strong>on</strong>s for l<strong>on</strong>gitudinal<br />

and lateral comp<strong>on</strong>ents <strong>of</strong> <strong>tire</strong> force.


How Tire Forces are Included In<br />

Multibody Vehicle Model<br />

4. Determine kinematic inputs to <strong>tire</strong> model (S, γ, α)<br />

5. Use a <strong>tire</strong> model to calculate Fx, Fy, Mx, My, Mz


MapleSim Demo


The Fiala Tire Model<br />

The original <strong>tire</strong> model in MSC.ADAMS<br />

Inputs:<br />

1. Multibody model (mass, rotati<strong>on</strong>al inertia)<br />

2. Tire parameters (C s , C α , etc.)<br />

3. The current kinematic state (S, α ,γ, etc.)


Effect <strong>of</strong> Normal Force (F z )<br />

<strong>on</strong> Lateral Force (F y )

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