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Question

Question: What is the tension in the string at \( A \) immediately after the string breaks at \( B \) ? \( \...

What is the tension in the string at AA immediately after the string breaks at BB ?
\left( A \right)\dfrac{{mg}}{5} \\\ \left( B \right)\dfrac{{2mg}}{{31}} \\\ \left( C \right)\dfrac{{mg}}{{37}} \\\ \left( D \right)\dfrac{{5mg}}{{37}} \\\

Explanation

Solution

Hint : In order to solve his question, we are going to first compute the centre of mass position and as we know that the torque about the centre of mass is zero, so the torque due to tension at AA is equal to that of string at BB , the tension at AA does not change just after the string breaks.
The torque at any point is given by
τ=F×r\tau = F \times r
Where, FF is forced at the point and rr is the radial distance of the point from the centre of mass.
The torque about centre of mass is zero
τCM=0{\tau _{CM}} = 0

Complete Step By Step Answer:
The centre of mass of the system is given by
xCM=ρ00Lx4dxρ00Lx3dx=L55L44=4L5{x_{CM}} = \dfrac{{{\rho _0}\int\limits_0^L {{x^4}dx} }}{{{\rho _0}\int\limits_0^L {{x^3}dx} }} = \dfrac{{\dfrac{{{L^5}}}{5}}}{{\dfrac{{{L^4}}}{4}}} = \dfrac{{4L}}{5}
The torque about the centre of mass is zero, so the torque due to tension at AA , TA{T_A} is equal to that of string at BB , TB{T_B}
Thus,
{T_A} \times \dfrac{{4L}}{5} = {T_B} \times \dfrac{L}{5} \\\ \Rightarrow {T_A} = \dfrac{{{T_B}}}{4} - - - \left( 1 \right) \\\
The sum of the tensions at AA and BB is equal and opposite to the weight
TA+TB=mg(2){T_A} + {T_B} = mg - - - \left( 2 \right)
Solving (1)\left( 1 \right) and (2)\left( 2 \right) , we get
TA=mg5{T_A} = \dfrac{{mg}}{5} , TB=4mg5{T_B} = \dfrac{{4mg}}{5} ;
Now just after the string breaks, the tension of the string at AA remains the same, i.e. there is no change in the value of the tension at the string
So, TA=mg5{T_A} = \dfrac{{mg}}{5}
Hence, the option (A)mg5\left( A \right)\dfrac{{mg}}{5} is the correct answer.

Note :
It is to be noted that the torque of a string rotating about a point depends upon its distance with the centre of mass and the torque at the centre of mass is always zero because the radial distance there is zero, here the driving force is the tension of the string and the gravity is also present at the string.