Question
Question: The earring of Ms. Shon is \(5\;cm\) long. She sits in a merry-go-round moving at \(4\;ms^{-1}\) in ...
The earring of Ms. Shon is 5cm long. She sits in a merry-go-round moving at 4ms−1 in a circle of radius 2m. The time period of oscillations is nearly:
A. 0.6 s
B. 0.4 s
C. 0.8 s
D. None of these
Solution
Try and deduce the types of acceleration that the earring is subjected to. In other words, the earring naturally experiences a gravitational acceleration but bringing in the motion of the merry-go-round lends a centripetal acceleration to the earring that is normal to gravity. Finding the resultant acceleration, and thereby using the time period equation for any periodic motion (simple pendulum) will yield the required result.
Formula used:
Time period of a simple pendulum is, in general, T=2πgl
But in case of external factors contributing to the acceleration, T=2πanetl
Where, l is the length of the pendulum, g is the acceleration due to gravity , anet is the net acceleration influencing the pendulum.
Complete step by step answer:
We can approximate the earing to the working of a simple pendulum.
We know that the time period of a simple pendulum is given as: T=2πgl
This would be the case if Ms. Shon was just stationary. However, since she sits in a merry-go-round the earring, in addition to the gravitational acceleration is also subjected to a centripetal acceleration from the rotation of the merry-go-round.
This means that in order to obtain the right time period, our acceleration must be inclusive of both gravitational and centripetal forces acting on the earring.
The centripetal acceleration is given by a=rv2=242=8ms−2
The gravitational acceleration is numerically given as g=9.8ms−2
Therefore, the net acceleration will be the resultant of the two since centripetal forces and gravity act normal to each other.
Therefore, anet=g2+a2=9.82+82=96.04+64=160.04⇒anet=12.65ms−2
Given that the length of her earring is l=5cm=0.05m, the time period can be obtained as follows:
T=2πanetl=2π12.650.05=0.395s
Therefore, the time period is found to be approximately 0.40s
Hence the correct choice would be B. 0.4 s
Note:
Remember to calculate the resultant acceleration after including the two normal centripetal and gravitational accelerations, since discounting any one of them results in an inconsistent solution.
The centripetal force comes into play only because there is circular motion executed via the merry-go-round, and hence we can treat the entire scenario as that of a periodic circular motion.