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Answer: 12.0 m/s^2
Explanation:
Let [tex]\alpha[/tex] be the angular acceleration of the end of the rod
Taking torque about the link, we have:
[tex]\tau = W \times OM\\ or\\ \tau = mg\times \left(\dfrac{L}{2}\right)\sin 55^\circ ....(i)[/tex]
Torque is also given in terms of moment of inertia of the rod and its angular acceleration i.e.
[tex]\tau = I_{rod}\ \alpha......(ii)[/tex]
From equations (i) and (ii) we have:
[tex]mg\times \left(\frac{L}{2}\right)\sin 55^\circ = \left(\frac{mL^2}{3}\right)\alpha\ \ \ \ \ \ \ (\because I_{rod} = \dfrac{mL^2}{3}) \\ \\ \alpha = \left(\frac{3g}{2L}\right)\sin 55^\circ\\ \\ \alpha = \left(\frac{3\times 9.8}{2\times 2.4}\right)\sin 55^\circ\\ \\ \boxed{\alpha = 5.02\ rad/s^2} }[/tex]
The acceleration of the end of the rod farthest from the link is given by:
[tex]a = L\alpha\\ \\ a = (2.4\ m)(5.02\ rad/s^2)\\ \\ \boxed{a = 12.0\ m/s^2}[/tex]