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Question: A simple pendulum has a string of length l and bob of mass m. When the bob is at its lower position,...

A simple pendulum has a string of length l and bob of mass m. When the bob is at its lower position, it is given the maximum horizontal speed necessary for it to move in a circular path about the point of suspension. The tension in the string at the lowest position of the bob is
A. 6mgmg
B. 3mg3\,mg
C. 10mg\sqrt {10} \,mg
D. 4mg4\,mg

Explanation

Solution

Hint In the question, length and mass are essential parameters. Here, the bob is at a lower position and it is moved along a circular path about the point of the suspension. So, by using the expression of the work-energy theorem, we get the value of the tension in the string.
Formula used:
Kinetic energy =12mv2 = \dfrac{1}{2}m{v^2}
Potential energy =mg2l = mg2l
Where,
mm be the mass, vv be the velocity, gg be the acceleration due to gravity and ll be the length.

Complete step by step answer
Let A be the topmost point of the circle and B be the lowest point of the circle.
Let v1{v_1}and v2{v_2}be the velocities at A and B respectively.
Applying the principle of the conservation of the energy between A and B.
12mv2212mv12=mg2l\dfrac{1}{2}m{v_2}^2 - \dfrac{1}{2}mv_1^2 = mg2l
Or we written the equation as
mv22l=mv12l+4mg..........(1)\dfrac{{mv_2^2}}{l} = \dfrac{{mv_1^2}}{l} + 4mg..........\left( 1 \right)
At the lowest point of the circle B, mv22l=Tmg...........(2)\dfrac{{mv_2^2}}{l} = T - mg...........\left( 2 \right)
At the top most point of the circle A, mv12l=mg...........(3)\dfrac{{mv_1^2}}{l} = mg...........\left( 3 \right)
Solving all the above three equations, we get
mg+4mg=Tmgmg + 4mg = T - mg
Performing the arithmetic operation in the above equation, we get
T=6mg.T = 6\,mg.
Therefore, the tension in the lowest position of the bob is 6mg.6\,mg.

Hence from the above options, option A is correct.

Note In the question, the pendulum is moved about a point of the suspension. So, there must be a potential and kinetic energy. By using the parameters of the work-energy theorem, we get the result.