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

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crude initialisation introduces errors that are initially outside expectation<br />

that take upwards of 4 s to decay.<br />

TG_P_MET [metres]<br />

TG_V_MET [m/sec]<br />

11<br />

10<br />

9<br />

8<br />

7<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

10 12 14 16 18 20 22 24 26 28 30<br />

TIME [seconds]<br />

4<br />

3.5<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

T3_IMQV10.MTB<br />

T3_IMQV03.MTB<br />

T3_IMQV01.MTB<br />

T3_IMQV0Q.MTB<br />

9-25<br />

T3_IMQV10.MTB<br />

T3_IMQV03.MTB<br />

T3_IMQV01.MTB<br />

T3_IMQV0Q.MTB<br />

0<br />

10 12 14 16 18 20 22 24 26 28 30<br />

TIME [seconds]<br />

Figure 9-43<br />

Velocity Filter - Position and Velocity Errors, ( PIP ) and ( PIV )<br />

The gradual reduction in the errors, and the improvement in observability as<br />

indicated by the CN, is due to the relative position of the target with respect<br />

to the radar. The closest approach to the radar occurs at approximately 30 s<br />

when range-rate measurements are most effective.<br />

The velocity filter position error when tracking a target performing a “U”<br />

turn designed for Singer filter tuning is shown in Figure 9-45. Although the<br />

performance is poor the velocity filter by remains stable.

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