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Question: A pot maker rotates a pot making wheel of radius \(3m\) by applying a force of \(200N\) tangentially...

A pot maker rotates a pot making wheel of radius 3m3m by applying a force of 200N200N tangentially. If wheel completes exactly 32\dfrac{3}{2} revolutions, work done by him is:
A) 5654.86J5654.86J
B) 4321.32J4321.32J
C) 4197.5J4197.5J
D) 1884.96J1884.96J

Explanation

Solution

While calculating work done in a rotational motion, we need to consider all the angular equivalents of linear parameters. Maximum angular calculations are done in radians not in degrees.

Complete step by step answer:
In rotational motion the angular equivalents of linear parameters are,
Sθ vω aα Fτ S \to \theta \\\ v \to \omega \\\ a \to \alpha \\\ F \to \tau
So, To find work done, we need to find torque(τ)\left( \tau \right) first,
τ=r×F\Rightarrow \tau = r \times F
τ=3×200\Rightarrow \tau = 3 \times 200
τ=600Nm\Rightarrow \tau = 600Nm
Now to calculate work done by the man,
W=τdθ\Rightarrow W = \int {\tau d\theta }
Since torque is constant,
W=τΔθ\Rightarrow W = \tau \Delta \theta
In this case total angular displacement(θ)\left( \theta \right),
Δθ=32×2π\Rightarrow \Delta \theta = \dfrac{3}{2} \times 2\pi
Δθ=3π\Rightarrow \Delta \theta = 3\pi
So, W=600×3πW = 600 \times 3\pi
W=1800πJ\Rightarrow W = 1800\pi J
W=5654.86J\Rightarrow W = 5654.86J

Therefore, the correct answer is option A.

Note: Work done can also be calculated by work-energy theorem in a rotational motion. It says that work done during a rotational motion is equal to change in kinetic energy. In vector form the dot product of torque vector and radial vector is known as work done.