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

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Chapter 5 / Missile State Observer<br />

_ _<br />

required during transients lasting some 5 s. Whilst the non co-ordinated<br />

models here are specified in Cartesian axes, fixed wing target motion is best<br />

expressed in a body referenced curvature, torsion and bi-normal (Frenet)<br />

axes, Chen [C.7] . Much effort has been expended in this field which is<br />

reviewed by Nabaa [N.4] . Singer’s original model was improved by<br />

Gholson [G.13] (1977), Moose [M.8&9] (1975-79), Ricker [R.13] (1978) by<br />

including randomly switched mean acceleration input with a Gaussian noise<br />

residual.<br />

k + 1<br />

k<br />

4-19<br />

k<br />

k<br />

( U w )<br />

X : = A ⋅ X + Γ ⋅ +<br />

k<br />

k<br />

Equation 4.5-20<br />

Berg [B.8] (1983) added an adaptive mean jerk term to accommodate coordinated<br />

target dynamics with constant thrust, drag, lift and zero roll rate,<br />

A<br />

t<br />

−1<br />

C<br />

A<br />

A<br />

( & A<br />

P&<br />

t − w ) &P&<br />

&<br />

t<br />

& P&<br />

& : = − τ ⋅<br />

+<br />

Equation 4.5-21<br />

Song [S.12] (1988) included target dynamics free of Berg’s restrictions, mean<br />

jerk being a function of target velocity directed lateral acceleration<br />

estimated from its mass, velocity and lift coefficient. Mahapatra [M.6]<br />

introduced jerk states, significantly improving velocity and acceleration<br />

estimates for an idealised circular trajectory, even when jerk was absent.<br />

However, Vergez [V.1] showed that increasing the filter order in general<br />

degrades tracking performance compared with the Singer and acceleration<br />

models.<br />

4.5.4 Weave Filter<br />

Assuming that the target speed and turn rate are constant over the<br />

propagation interval,<br />

W<br />

W<br />

iA<br />

t<br />

A 2 iA iA<br />

( ω ) × P&<br />

w<br />

& P &<br />

: = −<br />

+<br />

A,<br />

TV<br />

⎛ ⎛ 0 , 1 , 0 ⎞<br />

⎜ ⎜<br />

⎟<br />

⎜ ⎜<br />

⎟<br />

i ⎜<br />

Φ : = exp<br />

⎜ 0 , 0 , 1 ⎟<br />

⎜ ⎜<br />

⎟<br />

⋅ ∆t<br />

⎜ ⎜<br />

⎟<br />

⎜ ⎜<br />

⎟<br />

⎝ ⎝ 0 , A,<br />

TV ⎠<br />

W<br />

t<br />

W<br />

( ) ⎟ ⎟⎟⎟⎟⎟⎟<br />

iA 2<br />

ω , 0<br />

Equation 4.5-22<br />

⎞<br />

⎠<br />

Equation 4.5-23

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