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

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Chapter 2 / Target Modelling<br />

_ _<br />

then subjected to filtering followed by transformation back to the Alignment<br />

frame thereby preserving the Target model interfaces in TG_DYNAMICS.<br />

These idealised target motions start after 10 s of constant velocity flight, and<br />

end after 30 s; Missile launch is suspended when IMM filter tuning.<br />

2.4.1 Constant Velocity<br />

Target Model 1 is activated with the Alignment frame acceleration set to<br />

zero. The target trajectory is a flypast at a constant velocity of - 400 m/s<br />

parallel to X A starting from the same initial state as Target Trajectory 2.<br />

2.4.2 Constant Acceleration<br />

This trajectory starts the same as that for the constant velocity case. After<br />

10 s the following acceleration profile is invoked:<br />

2.4.3 Lagged Motion<br />

A<br />

[ 0 , 10 ] ∪ ] 24 , 30 ] ⇒ & P&<br />

t : 0 3<br />

t ∈<br />

=<br />

A<br />

] 10 , 17 ] ⇒ & P&<br />

: = ϕ ( 10 , 10 , 10)<br />

t<br />

2-13<br />

D1L<br />

Equation 2.4-1<br />

T<br />

( , t )<br />

t ∈<br />

−<br />

A<br />

] 17 , 24 ] ⇒ P&<br />

& : = ϕ ( −10<br />

, 10 , 10)<br />

t ∈<br />

−<br />

t<br />

D1L<br />

ta<br />

Equation 2.4-2<br />

T<br />

( , t )<br />

ta<br />

Equation 2.4-3<br />

Again the target starts as for the constant velocity case. After 10 s the target<br />

performs a 50 g “U” turn retreating at high speed. The demanded<br />

accelerations in this case are,<br />

A<br />

[ 0 , 10 ] ∪ ] 24 , 30 ] ⇒ P&<br />

&<br />

t : 0 3<br />

t ∈<br />

=<br />

A<br />

] 10 , 17 ] ⇒ & P&<br />

: = ϕ ( 50 , 50 , 50)<br />

t<br />

D1L<br />

Equation 2.4-4<br />

T<br />

( , t )<br />

t ∈<br />

−<br />

A<br />

] 17 , 24 ] ⇒ P&<br />

& : = ϕ ( 50 , 50 , 50)<br />

t ∈<br />

−<br />

t<br />

D1L<br />

ta<br />

Equation 2.4-5<br />

T<br />

( , t )<br />

ta<br />

Equation 2.4-6

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