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Modelling and assembly of the full vehicle 391<br />

a y lateral acceleration (m/s 2 )<br />

torque around z-axis (Nm)<br />

steer angle (rad)<br />

side slip angle (rad)<br />

ij wheel slip angles (rad)<br />

. yaw rate (rad/s)<br />

F zij vertical forces on each wheel (N)<br />

ij position: i front(f )/rear(r), j left(l)/right(r)<br />

Note that steer angle and the velocity of the vehicle’s centre of gravity<br />

v cog are specified as model inputs.<br />

The relationship between the dynamic vehicle parameters can be formulated<br />

as differential equations. Most of these can be found in the standard<br />

literature. Using formulas by Wong (2001) and Will and Żak (1997) the<br />

following differential equations for acceleration, torque and yaw rate can<br />

be derived:<br />

1 ( )<br />

v˙ cos sin cos sin ˙<br />

x m F xfl F yfl F xfr F yfr F xrl F xrr v y<br />

1 ( )<br />

(6.28)<br />

v˙ cos sin cos sin ˙<br />

y m F yfl F xfl F yfr F xfr F yrl F yrr v x<br />

(6.29)<br />

t f <br />

t f tr<br />

tr<br />

<br />

Fxfl<br />

Fxfr<br />

Fxrl<br />

Fxrr bFyfl bFyfr cFyrl cFyrr<br />

2 2 2 2<br />

M M M M<br />

(6.30)<br />

zfl zfr zrl zrr<br />

˙˙ J z<br />

(6.31)<br />

where the additional parameters are defined as:<br />

F xij longitudinal forces on tyre ij (N)<br />

F yij lateral forces on tyre ij (N)<br />

F xij longitudinal forces on tyre ij in the vehicle’s co-ordinate system (N)<br />

F yij lateral forces on tyre ij in the vehicle’s co-ordinate system (N)<br />

M zij self-aligning moment on tyre ij (Nm)<br />

m mass of vehicle (kg)<br />

J z moment of inertia around vertical axis (Nm 2 )<br />

t f , t r front and rear track width (m)<br />

b, c position of centre of gravity between wheels (m)<br />

Other important states are the wheel slip angles ij and the body slip angle<br />

, defined as follows:<br />

<br />

fl/<br />

r<br />

⎛ ⎞<br />

vy<br />

b˙<br />

arctan<br />

⎜ ⎟<br />

1<br />

⎜ vx<br />

tf˙<br />

⎟<br />

⎝ 2 ⎠<br />

(6.32)

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