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\begin{array}{l} F_{G} = -mg\hat{y}\\ \\ F_{D} = -\tfrac{1}{2}\rho A C_{D} v^{2} \hat{v}\\ \\ F_{M} = -\tfrac{1}{2}\rho A C_{L} v^{2} \left (\hat{\omega } \times \hat{v} \right ) \end{array} \large \omega_{2} = \omega_{1}+\frac{\mu\left ( 1+e_{y} \right )v_{y1} }{0.4R}

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