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Table 6.

Dimensional static stability derivatives with respect to tunnel speed U and body angle αbfor the three locusts, resolved in the stability axes

\({\partial}X{/}{\partial}{\alpha}_{\mathrm{b}}\)
\({\partial}Z{/}{\partial}{\alpha}_{\mathrm{b}}\)
\({\partial}M{/}{\partial}{\alpha}_{\mathrm{b}}\)
\({\partial}X{/}{\partial}U\)
\({\partial}Z{/}{\partial}U\)
\({\partial}M{/}{\partial}U\)
Locust(10−3 N rad−1)(10−3 N rad−1)(10−6 N m rad−1)(10−3 N m−1 s)(10−3 N m−1 s)(10−6 N s)
`R' −9.9 −31 −924 −7.8 −1.4 −416 
`G' −23 −25 −1467 −8.3 [0.53] −461 
`B' [−1.5] −34 [−739] −9.0 [0.05] −492 
\({\partial}X{/}{\partial}{\alpha}_{\mathrm{b}}\)
\({\partial}Z{/}{\partial}{\alpha}_{\mathrm{b}}\)
\({\partial}M{/}{\partial}{\alpha}_{\mathrm{b}}\)
\({\partial}X{/}{\partial}U\)
\({\partial}Z{/}{\partial}U\)
\({\partial}M{/}{\partial}U\)
Locust(10−3 N rad−1)(10−3 N rad−1)(10−6 N m rad−1)(10−3 N m−1 s)(10−3 N m−1 s)(10−6 N s)
`R' −9.9 −31 −924 −7.8 −1.4 −416 
`G' −23 −25 −1467 −8.3 [0.53] −461 
`B' [−1.5] −34 [−739] −9.0 [0.05] −492 
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