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Fractional potential field in path planning for mobile robot obstacle ...

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Collision Avoidance<br />

Now we consider the safety issue of the <strong>mobile</strong> <strong>robot</strong>. It is highly likely that the<br />

<strong>robot</strong> will encounter mov<strong>in</strong>g <strong>obstacle</strong>s that travel through the polluted area, <strong>for</strong> example,<br />

the mov<strong>in</strong>g cargo vessels. In order to avoid collision between the <strong>robot</strong> and<br />

the mov<strong>in</strong>g <strong>obstacle</strong> effectively, the relative position and velocity between <strong>robot</strong><br />

and <strong>obstacle</strong> should be considered. Here we <strong>in</strong>troduce a <strong>potential</strong> <strong>field</strong> method<br />

from reference 3 that is used <strong>for</strong> dynamic <strong>obstacle</strong> avoidance.<br />

The repulsive <strong>potential</strong> generated by the <strong>obstacle</strong> is given by:<br />

Urep(p, v) =<br />

⎧<br />

⎪⎨<br />

⎪⎩<br />

0 :<br />

if ρs(p, p obs) − ρm ≥ ρ0 or vRO ≤ 0<br />

η(Urep) :<br />

if 0 < ρs(p, p obs) − ρm < ρm and vRO > 0<br />

undef<strong>in</strong>ed :<br />

if vRO > 0 and ρs(p, p obs) < ρm<br />

The positive <strong>for</strong>ce between the <strong>robot</strong> and the <strong>obstacle</strong> is def<strong>in</strong>ed as the negative<br />

gradient of the repulsive <strong>potential</strong> with respect to <strong>robot</strong> position and velocity.<br />

11 - 15<br />

(3)

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