KCET · Physics · Laws of Motion
A mass M is hung with a light inextensible string as shown in figure. Find the tension of the horizontal string.

- A \(\sqrt{2}Mg\)
- B \(\sqrt{3}Mg\)
- C \(Mg\)
- D \(3Mg\)
Answer & Solution
Correct Answer
(C) \(Mg\)
Step-by-step Solution
Detailed explanation
Let \(T_1\) be the tension in the horizontal string, \(T_2\) be the tension in the slanted string, and \(T_3\) be the tension in the vertical string.
For the mass \(M\) in equilibrium, the tension in the vertical string is:
\(T_3 = Mg\)
Considering the equilibrium of the knot O, we can resolve the forces in the horizontal and vertical directions.
Balancing the forces in the vertical direction:
\(T_2 \sin 45^{\circ} = T_3 = Mg\)
Balancing the forces in the horizontal direction:
\(T_1 = T_2 \cos 45^{\circ}\)
Dividing the vertical force equation by the horizontal force equation, we get:
\(\dfrac{T_2 \sin 45^{\circ}}{T_2 \cos 45^{\circ}} = \dfrac{Mg}{T_1}\)
\(\tan 45^{\circ} = \dfrac{Mg}{T_1}\)
Since \(\tan 45^{\circ} = 1\), we have:
\(1 = \dfrac{Mg}{T_1}\)
\(T_1 = Mg\)
Thus, the tension in the horizontal string is \(Mg\).
Answer: \(Mg\)
For the mass \(M\) in equilibrium, the tension in the vertical string is:
\(T_3 = Mg\)
Considering the equilibrium of the knot O, we can resolve the forces in the horizontal and vertical directions.
Balancing the forces in the vertical direction:
\(T_2 \sin 45^{\circ} = T_3 = Mg\)
Balancing the forces in the horizontal direction:
\(T_1 = T_2 \cos 45^{\circ}\)
Dividing the vertical force equation by the horizontal force equation, we get:
\(\dfrac{T_2 \sin 45^{\circ}}{T_2 \cos 45^{\circ}} = \dfrac{Mg}{T_1}\)
\(\tan 45^{\circ} = \dfrac{Mg}{T_1}\)
Since \(\tan 45^{\circ} = 1\), we have:
\(1 = \dfrac{Mg}{T_1}\)
\(T_1 = Mg\)
Thus, the tension in the horizontal string is \(Mg\).
Answer: \(Mg\)
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