Talk:PlanetPhysics/Euler 232 Sequence

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For more info on Euler Sequences, notation and convention see the generic entry on Euler Angle Sequences. \\

$ R_{232}(\phi, \theta, \psi) = R_2(\psi) R_3(\theta) R_3(\phi) $ \\

The rotation matrices are

\begin{equation} R_2(\psi) = \left[ \begin{array}{ccc} c_{\psi} & 0 & -s_{\psi} \\ 0 & 1 & 0 \\ s_{\psi} & 0 & c_{\psi} \end{array} \right] \end{equation}

\begin{equation} R_3(\theta) = \left[ \begin{array}{ccc} c_{\theta} & s_{\theta} & 0 \\ -s_{\theta} & c_{\theta} & 0 \\ 0 & 0 & 1 \end{array} \right] \end{equation}

\begin{equation} R_2(\phi) = \left[ \begin{array}{ccc} c_{\phi} & 0 & -s_{\phi} \\ 0 & 1 & 0 \\ s_{\phi} & 0 & c_{\phi} \end{array} \right] \end{equation}

Carrying out the matrix multiplication from right to left \\

$ R_3(\theta)R_2(\phi) = \left[ \begin{array}{ccc} c_{\theta} & s_{\theta} & 0 \\ -s_{\theta} & c_{\theta} & 0 \\ 0 & 0 & 1 \end{array} \right] \left[ \begin{array}{ccc} c_{\phi} & 0 & -s_{\phi} \\ 0 & 1 & 0 \\ s_{\phi} & 0 & c_{\phi} \end{array} \right] = \left[ \begin{array}{ccc} c_{\theta} c_{\phi} & s_{\theta} & -c_{\theta} s_{\phi} \\ -s_{\theta} c_{\phi} & c_{\theta} & s_{\theta} s_{\phi}  \\ s_{\phi} & 0 & c_{\phi} \end{array} \right] $ \\

Finaly leaving us with the Euler 232 sequence \\

$ R_2(\psi)R_3(\theta)R_2(\phi) = \left[ \begin{array}{ccc} c_{\psi} c_{\theta} c_{\phi} - s_{\psi} s_{\phi} & c_{\psi} s_{\theta}  & -c_{\psi} c_{\theta} s_{\phi} - s_{\psi} c_{\phi}   \\ -s_{\theta} c_{\phi} & c_{\theta} & s_{\theta} s_{\phi} \\ s_{\psi} c_{\theta} c_{\phi} + c_{\psi} s_{\phi} & s_{\psi} s_{\theta} &  - s_{\psi} c_{\theta} s_{\phi} +  c_{\psi} c_{\phi}  \end{array} \right] $

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