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As a further example of the relationship between D1 and D0, the equation of planar motion in D1 (3.18) is, in this appendix, transformed to the axes of Do.
From (2.19) and (4.18)
and from (2.19), (4.12) and (4.18)
and finally from (4.12)
The full transformation of (3.18) in terms of u then becomes, from (4.24),
(A.1), (A.2) and (A.3)
Substitution of (4.7) and (4.18) for u and s, then expands this to
the final result
G1 Version 2.2.4
Ó
P.G.Bass, November 2009
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