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04 Steering And Turning Vehicles - Department of Mechanical ...

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Y<br />

Recall: position and velocity in inertial frame<br />

We defined the vehicle’s kinematic state in the inertial frame by,<br />

l2<br />

y<br />

B<br />

l1<br />

x<br />

ψ<br />

So, for our simple (single-axle) vehicle,<br />

the velocities in the inertial frame in<br />

terms <strong>of</strong> the wheel velocities are,<br />

ME 360/390 – Pr<strong>of</strong>. R.G. Longoria<br />

Vehicle System Dynamics and Control<br />

X<br />

X<br />

Velocities in the local (body-fixed)<br />

reference frame are transformed<br />

into the inertial frame by the<br />

rotation matrix,<br />

or, specifically, qɺ = R( ψ ) ⋅qɺ<br />

I<br />

q<br />

I<br />

⎡ X ⎤<br />

=<br />

⎢<br />

Y<br />

⎥<br />

⎢ ⎥<br />

⎢⎣ ψ ⎥⎦<br />

⎡ cosψ sinψ 0⎤<br />

R(<br />

ψ ) =<br />

⎢<br />

−sinψ<br />

cosψ 0<br />

⎥<br />

⎢ ⎥<br />

⎢⎣ 0 0 1⎥⎦<br />

Inverting, we arrive at the velocities in the global reference<br />

frame,<br />

⎡ Xɺ ⎤ ⎡U ⎤ ⎡cosψ ⎢ ⎥<br />

qɺ I = Yɺ ⎢<br />

V<br />

⎥<br />

( ψ )<br />

⎢<br />

⎢ ⎥ =<br />

⎢ ⎥<br />

= Ψ ⋅ qɺ<br />

=<br />

⎢<br />

sinψ ⎢ψ ⎥<br />

⎣<br />

ɺ<br />

⎦<br />

⎢⎣ Ω⎥⎦<br />

⎢⎣ 0<br />

−sinψ<br />

cosψ 0<br />

0⎤<br />

⎡ vx<br />

⎤<br />

0<br />

⎥ ⎢<br />

v<br />

⎥<br />

⎥ ⎢ y ⎥<br />

1⎥⎦<br />

⎢⎣ ω ⎥ z ⎦<br />

qɺ<br />

I<br />

⎡ Rw l2Rw ⎤<br />

⎢ ( ω1 + ω2)cos ψ − ( ω1 −ω2<br />

)sinψ<br />

2<br />

B<br />

⎥<br />

⎡Xɺ ⎤ ⎢ ⎥<br />

⎢ ⎥ Rw l2Rw = Yɺ<br />

⎢ ( ω1 ω2)sin ψ ( ω1 ω2)cos ψ ⎥<br />

⎢ ⎥ = + + −<br />

⎢ 2<br />

B<br />

⎥<br />

⎢ψ ⎥<br />

⎣<br />

ɺ<br />

⎦ ⎢ ⎥<br />

⎢<br />

Rw<br />

( ω1 −ω2<br />

)<br />

⎥<br />

⎢⎣ B<br />

⎥⎦<br />

<strong>Department</strong> <strong>of</strong> <strong>Mechanical</strong> Engineering<br />

The University <strong>of</strong> Texas at Austin

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