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

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Appendix I / Utilities / Point Mass Kinematics<br />

_ _<br />

22.5.3 Average Angular Rates from Direction Cosines<br />

AVG_W_RATES takes the transform defining the orientation of frame (B)<br />

with respect to frame (A) at time (t - ∆t) and again at time (t), and returns<br />

the average angular rate over time interval (∆t).<br />

AVG_W_RATES<br />

≡<br />

ϕ<br />

AR<br />

The transformation over time (∆t) is,<br />

∆ T<br />

22.5-2<br />

B<br />

B B<br />

( T ( t − ∆t<br />

) , T , ω , ∆t<br />

)<br />

B<br />

B<br />

( T ( t − ∆t<br />

) , T )<br />

A<br />

A<br />

B<br />

B<br />

( t ) : = T ( t − ∆t<br />

) ⋅ T ( t )<br />

A<br />

A<br />

A<br />

A<br />

A,<br />

B<br />

Equation 22.5-9<br />

Equation 22.5-10<br />

( ( ) ( ) ( ) ( ) ( ) ( ) ) T<br />

∆T<br />

6 − ∆T<br />

6 , ∆T<br />

7 − ∆T<br />

7 , ∆T<br />

2 − T 2<br />

2 ⋅ Λ : =<br />

∆<br />

Λ<br />

≥<br />

10<br />

−12 B<br />

−1<br />

⇒ Λ ⋅ ∆t<br />

⋅ ωA,<br />

B : = Λ ⋅ sin<br />

−12<br />

B<br />

A, B<br />

Λ < 10 ⇒ ω =<br />

22.5.4 Dynamics of a Point in Inertial Space<br />

0<br />

3<br />

Equation 22.5-11<br />

( Λ )<br />

Equation 22.5-12<br />

Equation 22.5-13<br />

Consider a general point (p) moving with respect to frame (B) that is itself<br />

in motion with respect to the non-rotating frame (A). PTM_DYNAMICS<br />

provides the inertial velocity and acceleration of point (p), expressed in (B).<br />

PTM_DYNAMICS<br />

B B B B B B B B B<br />

( Aa,<br />

b , Va,<br />

b , ω&<br />

A,<br />

B , ωA,<br />

B , Pb,<br />

p , P&<br />

b, p , &P<br />

&<br />

b, p , k , Aa,<br />

p , Va,<br />

p )<br />

If (p) is moving with respect to (B) then (k = 0) and,<br />

V : = V + P&<br />

+ ω ×<br />

a, p<br />

a, b<br />

b,<br />

p<br />

A,<br />

B<br />

P<br />

b,<br />

p<br />

Equation 22.5-14<br />

Equation 22.5-15

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