Respuesta :
In order to solve the problem, we must require the equilibrium of all the torques acting on the rod. The fixed point is in X, so we have:
- The weight of the rod (mg) acting at the center of the rod (so, at a distance L/2 from X, where L is the length of the rod). So, the torque is
[tex]T_W = mg \frac{L}{2} [/tex]
- The vertical component of F (so, [tex]F \sin 30^{\circ}[/tex]) applied in Y, so at a distance L from X. Its torque is
[tex]F \sin 30^{\circ} L[/tex]
The weight points downwards (so, the torque is clockwise), while the torque of F points anti-clockwise, so the equilibrium of torques is
[tex]F \sin 30^{\circ} L = mg \frac{L}{2} [/tex]
and since the weight is mg=10 N, re-arranging the equation we find
[tex]F = \frac{10 N}{2 sin 30^{\circ}} = 10 N[/tex]
- The weight of the rod (mg) acting at the center of the rod (so, at a distance L/2 from X, where L is the length of the rod). So, the torque is
[tex]T_W = mg \frac{L}{2} [/tex]
- The vertical component of F (so, [tex]F \sin 30^{\circ}[/tex]) applied in Y, so at a distance L from X. Its torque is
[tex]F \sin 30^{\circ} L[/tex]
The weight points downwards (so, the torque is clockwise), while the torque of F points anti-clockwise, so the equilibrium of torques is
[tex]F \sin 30^{\circ} L = mg \frac{L}{2} [/tex]
and since the weight is mg=10 N, re-arranging the equation we find
[tex]F = \frac{10 N}{2 sin 30^{\circ}} = 10 N[/tex]
The value of the horizontal force acting on the rod is 10 N. Therefore option (C) is correct.:
Given data:
The weight of rod is, W = 10.0 N.
The angle made by force with respect to horizontal is, [tex]\theta = 30^\circ[/tex].
To maintain the steady position (equilibrium condition), the vertical component of force F must be balanced by the moment of force due to weight.
Therefore,
[tex](Fsin\theta) \times L = W \times \dfrac{L}{2} \\\\(F \times sin30^{\circ}) = \dfrac{10}{2} \\F = 10 \;\rm N[/tex]
Thus, the value of the horizontal force acting on the rod is 10 N. And option (C) is correct.
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