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value="-A" /> value="\${asset-dir}" /> value="-I" /> value="\${android-jar}" /> value="\${out-package}" />
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1 0 sin( ) cos( ) sin( ) cos( ) where E = 0 0 sin( ) cos( ) cos( ) 1 sin( ) tan( ) cos( ) tan( ) 1 . cos( ) sin( ) and E = 0 cos( ) sin( ) 0 cos( ) cos( ) Neither E nor its inverse is a rotation matrix. Eqns. (2.73) and (2.74) do not represent vector transformations between frames-of-reference. The matrix E is singular when = . 2 Eqn. (2.74) is a nonlinear ordinary di erential equation for the Euler angles. Numeric integration of eqn. (2.74) provides estimates of the Euler angles from which the direction cosine matrix can by computed using eqn. (2.43). This approach requires numerous trigonometric operations at the high rate of the attitude portion of the INS system. The vector b is not gb directly measured; instead it is computed as b = b b where b is ig gb ib ib measured by the body mounted gyros and b = Rb g with g expressed g ig ig ig in eqn. (2.57).
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