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Question: The linear speed of the second’s hand of a wall clock is \(1.05\;cm/s\) What will be the length of t...

The linear speed of the second’s hand of a wall clock is 1.05  cm/s1.05\;cm/s What will be the length of the second hand?

Explanation

Solution

We know that linear speed is the measure at which the object travels or covers a certain linear distance. And angular speed is the measure at which a rotating object covers a certain circular path. Using the two and their relationship, we can solve the following question as shown below.

Complete step by step solution:
A body which undergoes rotation like the seconds hand here has two kinds of velocity namely the angular velocityω\omega and the linear velocityvv .The linear velocity is mathematically defined as v=stv=\dfrac{s}{t} where ss is the linear distance covered in time tt whereas angular velocity is mathematically defined as ω=θt\omega=\dfrac{\theta}{t} where θ\theta is the angular distance covered at time tt . Also the relationship between the two is given as v=ωrv=\omega r, where rr is the radius of the circular path
Since s=rθs=r\theta or the length of the arc, ss is the product of the radius rr and the angle θ\theta subtended by it in the circle.
Hence solving the above equations, we getv=ωrv=\omega r
Given that the linear speed of the seconds hand is v=1.05  cm/sv=1.05\;cm/s, then then angular velocity of the seconds hand will be ω=2π60\omega=\dfrac{2\pi}{60},let the length of the second’s hand be rr, then
Then from v=ωrv=\omega r, substituting the values we have
2π×r60=1.05\dfrac{2\pi \times r}{60}=1.05
    r=1.05×602π\implies r=\dfrac{1.05\times 60}{2\pi}
    r=632×3.14\implies r=\dfrac{63}{2\times 3.14}
r=10.03  cm\therefore r=10.03\;cm
Thus the length of the seconds hand was found to be 10.03  cm10.03\;cm

Note: Linear velocity helps in the movement of the object in the forward direction, whereas the angular velocity is due to the centripetal force acting on the rotating object and helps in the tangential direction; hence both are required for the rotating object to be stable.