Explanations & Calculations
By resolving the pulling force into orthogonal components we can find the verticle & horizontal applications of it. The vertical component of the pulling force that acts downwards on the ring is P v = T × cos 60 = T 2 \qquad\qquad
\begin{aligned}
\small P_v &=\small T\times\cos60=\frac{T}{2}
\end{aligned} P v = T × cos 60 = 2 T
And it's horizontal component which applies horizontally on the ring (pulling away) is P h = T × sin 60 = 3 T 2 \qquad\qquad
\begin{aligned}
\small P_h &=\small T\times \sin60=\frac{\sqrt3 T}{2}
\end{aligned} P h = T × sin 60 = 2 3 T
Now, the ring's weight is 4 g \small 4g 4 g downwards and the frictional force is holding the ring sliding downwards the rod hence it applies on the rod upwards. Since the ring is in equilibrium, all the vertical forces should be balanced or the net vertical force on the ring should be zero. Then, ↑ Σ F = F − 4 g − T 2 = 0 F = 4 g + T 2 \qquad\qquad
\begin{aligned}
\small \uparrow\Sigma F&=\small F-4g-\frac{T}{2}=0\\
\small F&=\small 4g+\frac{T}{2}
\end{aligned} ↑ Σ F F = F − 4 g − 2 T = 0 = 4 g + 2 T
Frictional force is found then.
Treating the ring's horizontal equilibrium the same way, we can find the normal force that acts on the ring. → 3 T 2 − R = 0 R = 3 T 2 \qquad\qquad
\begin{aligned}
\small \to \frac{\sqrt3 T}{2}-R&=\small 0\\
\small R&=\small \frac{\sqrt 3 T}{2}
\end{aligned} → 2 3 T − R R = 0 = 2 3 T
The contact force on the ring is obtained by R 2 + F 2 \small \sqrt{R^2+F^2} R 2 + F 2
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