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

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Chapter 6 / Missile Guidance<br />

_ _<br />

For BTT, the missile manoeuvres in the pitch plane only,<br />

( & YB ZB<br />

D ZR R Y<br />

P& , P&<br />

& ) : = ( 0 , ϕ ( A ⋅ cosΦ<br />

, ζ , ω ) )<br />

o , m<br />

o,<br />

m<br />

6-37<br />

D2L<br />

B<br />

LA<br />

LA<br />

Equation 6.10-11<br />

When AUTOP_SW is set to 1 constant values of 0.7 and 6 Hz are used for<br />

the damping ratio and natural frequency, otherwise they are incidence and<br />

Mach number dependent,<br />

⎛<br />

⎜<br />

⎜<br />

⎜<br />

⎝<br />

Y<br />

Z<br />

ω<br />

L<br />

ω<br />

LA<br />

LA<br />

⎞<br />

⎟<br />

⎟<br />

⎟<br />

⎠<br />

M<br />

m<br />

<<br />

1<br />

⇒<br />

⎧<br />

⎪<br />

⎨<br />

⎪<br />

⎩<br />

Y<br />

ω<br />

LA<br />

ζ<br />

LA<br />

: =<br />

: =<br />

Z<br />

ω<br />

LA<br />

0.<br />

6<br />

: =<br />

4 ⋅ π<br />

( M − 1 )<br />

M m ≥ 1 ⇒ ζ LA : = 0.<br />

6 + 0.<br />

1⋅<br />

M<br />

: =<br />

2 ⋅<br />

π ⋅<br />

⎛<br />

⎜<br />

2 +<br />

⎜<br />

⎜<br />

⎜<br />

⎝<br />

M<br />

≥<br />

( M −1<br />

)<br />

m<br />

m<br />

1<br />

⋅<br />

⇒<br />

⎛<br />

⎜<br />

⎜ 1.<br />

5<br />

⎜<br />

⎝<br />

+<br />

MAX<br />

The natural frequency is subject to an incidence limit (<br />

6.10.2 Angular Motion<br />

1<br />

ξ<br />

MV<br />

B<br />

⎫<br />

⎪<br />

⎬<br />

⎪<br />

⎭<br />

Equation 6.10-12<br />

Equation 6.10-13<br />

⎛<br />

⎜<br />

⋅ ⎜<br />

⎜<br />

⎝<br />

Θ<br />

Ψ<br />

MV<br />

B<br />

L<br />

MV<br />

B<br />

⎞ ⎞ ⎞<br />

⎟ ⎟ ⎟<br />

⎟ ⎟ ⎟<br />

⎟ ⎟ ⎟<br />

⎟ ⎟<br />

⎠<br />

⎟<br />

⎠ ⎠<br />

Equation 6.10-14<br />

MV<br />

MAX B<br />

ξ ) of 40°.<br />

The external moment (M) acting on the missile at the mass centre equals the<br />

rate of change of angular momentum (H) in inertial space. When measured<br />

in the rotating Missile Body frame,<br />

m<br />

I<br />

( Hm<br />

) : = DB<br />

( Hm<br />

) + ω Hm<br />

M : = D<br />

×<br />

C,<br />

B<br />

Equation 6.10-15<br />

The local inertial axes are referred to the missile reference point (m). When<br />

the mass is evenly distributed the inertial tensor [Im] is diagonal comprising<br />

only moments of inertia. As the Missile Body frame is fixed in the missile,<br />

B<br />

m<br />

B B B T B<br />

( I , I , I ) ⊗<br />

H : =<br />

ω<br />

XX<br />

YY<br />

ZZ<br />

C,<br />

B<br />

Equation 6.10-16

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