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

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Chapter 6 / Missile Guidance<br />

_ _<br />

⎛<br />

⎜<br />

⎜<br />

⎜<br />

⎝<br />

ϕ2<br />

L<br />

ϕ<br />

3<br />

⎞<br />

⎟<br />

⎟<br />

⎟<br />

⎠<br />

6-41<br />

MV<br />

( 30 − M ) ⋅ ( Θ )<br />

⎛<br />

⎜<br />

m<br />

: = 0.<br />

85 − 0.<br />

15 ⋅ M + ⎜<br />

m<br />

L<br />

⎜<br />

⎜<br />

m<br />

⎝<br />

( ) ( ) ⎟ ⎟⎟⎟ MV 2<br />

30 − M ⋅ Ψ<br />

Table 6-2 : Sea-Level Missile Incidence Lag (Seconds)<br />

B<br />

B<br />

2<br />

⎞<br />

⎠<br />

Equation 6.10-30<br />

MACH INCIDENCE ( DEGREES )<br />

NUMBER 0 5 10 20 30 40<br />

1.0 1.429 1.086 0.632 0.236 0.116 0.067<br />

1.5 1.067 0.792 0.446 0.163 0.079 0.046<br />

2.0 0.909 0.655 0.356 0.126 0.061 0.035<br />

2.5 0.842 0.584 0.305 0.105 0.050 0.029<br />

3.0 0.833 0.550 0.273 0.090 0.043 0.026<br />

The variation in incidence lag with Mach number and sea-level incidence is<br />

given in Table 6-2. Incidence lag sensitivity with respect to the missile<br />

observer states,<br />

∂ TI<br />

∂ X<br />

SO<br />

YB<br />

∂ TI<br />

∂ X<br />

SO<br />

ZB<br />

M<br />

M<br />

: =<br />

: =<br />

−<br />

−<br />

( ) ⎟ YB 2 ⎛ ∂ ϕ<br />

∂ ϕ ⎞<br />

⎜ 1<br />

2<br />

T ⋅ ⋅ ϕ + ϕ ⋅<br />

I<br />

⎜<br />

⎝<br />

∂<br />

SO<br />

X<br />

M<br />

2<br />

1<br />

∂<br />

SO<br />

X<br />

M<br />

⎠<br />

Equation 6.10-31<br />

( ) ⎟ ZB 2 ⎛ ∂ ϕ<br />

∂ ϕ ⎞<br />

⎜ 1<br />

3<br />

T ⋅ ⋅ ϕ + ϕ ⋅<br />

I<br />

⎜<br />

⎝<br />

∂<br />

SO<br />

X<br />

M<br />

3<br />

1<br />

∂<br />

SO<br />

X<br />

M<br />

⎠<br />

Equation 6.10-32<br />

The sensitivity of incidence lag to geodetic height depends on the change in<br />

static air pressure and temperature given in §19,<br />

∂ ϕ<br />

∂ X<br />

: =<br />

⎛<br />

⎜<br />

⎜<br />

⎝<br />

5969 ⎛<br />

⋅ ⎜<br />

⎝<br />

∂ TS<br />

⋅<br />

∂ P<br />

∂ PS<br />

−<br />

∂ P<br />

1 S<br />

02<br />

,<br />

, 0<br />

2<br />

ZG ZG<br />

16<br />

SO M<br />

PS<br />

TS<br />

m m<br />

Decomposing the remaining Jacobians,<br />

∂ ϕ ⎛<br />

⎜ ∂ ϕ2<br />

∂ ϕ<br />

: = 02<br />

, ,<br />

∂<br />

⎜<br />

ZA<br />

SO XM ⎝<br />

∂ Pm<br />

∂ P&<br />

P<br />

⎞<br />

⎟<br />

⎠<br />

⎞<br />

⎟<br />

⎟<br />

⎠<br />

Equation 6.10-33<br />

∂ ϕ<br />

∂ Q<br />

2 2<br />

A , 03<br />

, 2<br />

B , 06<br />

m<br />

A<br />

⎞<br />

⎟<br />

⎟<br />

⎠<br />

Equation 6.10-34

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