To find the tension at the lowest point of a flexible chain hanging between two fixed points, we need to consider the equilibrium condition of the chain. Each half of the chain experiences forces due to gravity and tension at the endpoints.
Let's break down the forces acting on one half of the chain:
Considering the vertical component of the tension at the support point, we have:
\(T_s \sin 30^\circ = \dfrac{mg}{2}\)
The sine of \(30^\circ\) is \(\dfrac{1}{2}\), so:
\(T_s \cdot \dfrac{1}{2} = \dfrac{mg}{2}\)
Solving this, we find that:
\(T_s = mg\)
Now, consider the horizontal component of the tension at the support point:
\(T_s \cos 30^\circ = T\)
The cosine of \(30^\circ\) is \(\dfrac{\sqrt{3}}{2}\), so we substitute \(T_s = mg\):
\(mg \cdot \dfrac{\sqrt{3}}{2} = T\)
Simplifying, the tension at the lowest point of the chain is:
\(T = \dfrac{\sqrt{3}}{2}mg\)
Thus, the correct answer is \(\dfrac{\sqrt{3}}{2}mg\).
A wooden cubical block of relative density 0.4 is floating in water. Side of cubical block is $10 \text{ cm}$. When a coin is placed on the block, it dips by $0.3 \text{ cm}$, weight of coin is: