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Thesis - Leigh Moody.pdf - Bad Request - Cranfield University

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Chapter 7 / Missile Trajectory Optimisation<br />

_ _<br />

7.5 Dynamic Constraints<br />

The cost function is minimised subject to the dynamic equality constraints,<br />

7-13<br />

( f ) ⋅ ∆t<br />

: = 0<br />

X X +<br />

k<br />

k − k + 1<br />

X<br />

k<br />

Equation 7.5-1<br />

The high incidence cost is already accounted for in the control effort. An<br />

active set strategy is used in conjunction with control hard limiting for the<br />

gradients. The remaining constraints are of the form,<br />

h ( X ) ≤ c<br />

Equation 7.5-2<br />

This can be converted to an equality constraint using a slack variable,<br />

s<br />

><br />

0<br />

⇒<br />

h<br />

2 ( X ) + s − c : = 0<br />

Equation 7.5-3<br />

Of the many constraints that may be applied two stand out in importance for<br />

air-defence:<br />

7.5.1 Up-link communications<br />

To maintain up-link communication the LOS to the missile must remain<br />

within the missile receiver beam width. Assuming that the missile is<br />

travelling away from the launcher and the limit for communication purposes<br />

is (ξC),<br />

1<br />

−1<br />

A 147 MV 2<br />

( cos ( nˆ ( P ) • ϕ ) ) ≤ C<br />

h : =<br />

ξ<br />

m<br />

A<br />

Equation 7.5-4<br />

The cost is squared to heavily penalise excursions beyond the threshold.<br />

7.5.2 Avoidance regions<br />

If the region to be avoided is centred at point (j) and extends spherically a<br />

distance RJ,<br />

−<br />

XA 2 YA 2 ZA 2<br />

2 A<br />

A A<br />

( P ) − ( P ) − ( P ) ≤ − R ; P : = P − P<br />

m,<br />

j<br />

m,<br />

j<br />

m,<br />

j<br />

h<br />

2<br />

: =<br />

J<br />

m,<br />

j<br />

o,<br />

j<br />

o,<br />

m<br />

Equation 7.5-5

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