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Question: A string of mass \(2.50kg\) is under a tension of \(200N\). The length of the stretched string is \(...

A string of mass 2.50kg2.50kg is under a tension of 200N200N. The length of the stretched string is 20.0m20.0m. If the transverse jerk is struck at one end of the string, how long does his disturbance take to reach the other end?

Explanation

Solution

The velocity of longitudinal waves on the string depends on mass per unit length and the tension applied to the string. The time taken to cover the length can be calculated using the basic formula of motion,
time=Distancespeed\text{time}=\dfrac{\text{Distance}}{\text{speed}}

Complete step by step solution:
It is given that the mass of the string is m=2.50kgm=2.50kg
The magnitude of the tension applied is T=200NT=200N
Length of the string is L=20.0mL=20.0m
The mass per unit length of the string, μ=MassLength\mu =\dfrac{\text{Mass}}{\text{Length}}
Putting the values m=2.50kgm=2.50kg and L=20.0mL=20.0m, we get
μ=2.520kg/m =0.125kg/m\begin{aligned} & \mu =\dfrac{2.5}{20}kg/m \\\ & =0.125kg/m \end{aligned}
Hence, the mass per unit length of string isμ=0.125kg/m\mu =0.125kg/m.
Speed of the longitudinal wave on the string is given by the formula,
v=Tμv=\sqrt{\dfrac{T}{\mu }}
Putting the valuesT=200NT=200N and μ=0.125kg/m\mu =0.125kg/m, we get
v=2000.125m/s =1600m/s =40m/s\begin{aligned} & v=\sqrt{\dfrac{200}{0.125}}m/s \\\ & =\sqrt{1600}m/s \\\ & =40m/s \end{aligned}

Hence, the speed of the longitudinal wave on the string is 40m/s40m/s
Now, the distance to cover on the string for the longitudinal wave is L=20mL=20m
The time taken by the longitudinal wave can be given as,
t=distancespeedt=\dfrac{\text{distance}}{\text{speed}}
Putting the valuesdistance=20m\text{distance=20m} and speed=40m/s\text{speed}=40m/s, we get
t=2040s =0.5s\begin{aligned} & t=\dfrac{20}{40}s \\\ & =0.5s \end{aligned}

Therefore, the time taken by the longitudinal wave to cover the string length is 0.5s.

Note: It is assumed that the mass is uniformly distributed all over the length of the string. It is assumed that the tension applied to the string is uniform all over the string along the length of the string.