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Question: A string of length 1m and linear mass density 0.01kgm\(^{−1}\) is stretched to a tension of 100N. Wh...

A string of length 1m and linear mass density 0.01kgm1^{−1} is stretched to a tension of 100N. When both ends of the string are fixed, the three lowest frequencies for standing waves are f1f_1​, f2f_2​ and f3f_3​. When only one end of the string is fixed, the three lowest frequencies for standing waves are n1n_1​, n2n_2​ and n3n_3​. Then
\eqalign{ & A.{n_3} = 5{n_1} = {f_3} = 125Hz \cr & B.{f_3} = 5{f_1} = {n_2} = 125Hz \cr & C.{f_3} = {n_2} = 3{f_1} = 150Hz \cr & D.{n_2} = \dfrac{{{f_1} + {f_2}}}{2} = 75Hz \cr}

Explanation

Solution

when string is fixed from both ends noses will be formed at both ends. When a string is only fixed from one end and set free at the other end node is formed at fixed end and antinode is formed at the free end. Since tension and linear mass density are given it is possible to find out the velocity of the standing wave in the string and wavelengths can be found as length of string(l) is given and finally frequencies can be found.

Formula used:
v=fλv = f\lambda
v=Tμv = \sqrt {\dfrac{T}{\mu }}

Complete answer:
When string is fixed at both ends initially one loop will be formed and hence wavelength of that loop be λ1{\lambda _1}
For one loop distance is λ12\dfrac{{{\lambda _1}}}{2}
So initially λ12=l\dfrac{{{\lambda _1}}}{2} = l, λ1=2l=2{\lambda _1} = 2l = 2 … eq1
Then next it forms two loops this time wave length be λ2{\lambda _2}
So distance would be λ2=l{\lambda _2} = l λ2=1{\lambda _2} = 1 … eq2

Then it forms three loops now wavelength is λ3{\lambda _3}
So distance would be 3λ32=l\dfrac{{3{\lambda _3}}}{2} = l λ3=23{\lambda _3} = \dfrac{2}{3} … eq3
Velocity of wave would be Tμ\sqrt {\dfrac{T}{\mu }} where T is tension and μ\mu is linear mass density
Velocity(v) = 1000.01=100m/s\sqrt {\dfrac{{100}}{{0.01}}} = 100m/s
v=fλv = f\lambda
f is frequency
From equation 1 and 2 and 3
We get
f1=vλ1=1002=50Hz{f_1} = \dfrac{v}{{{\lambda _1}}} = \dfrac{{100}}{2} = 50Hz
f2=vλ2=1001=100Hz{f_2} = \dfrac{v}{{{\lambda _2}}} = \dfrac{{100}}{1} = 100Hz
f3=vλ3=1002×3=150Hz{f_3} = \dfrac{v}{{{\lambda _3}}} = \dfrac{{100}}{2} \times 3 = 150Hz
now when string is free at one side fundamental frequency would be n1=v4l=1004=25Hz{n_1} = \dfrac{v}{{4l}} = \dfrac{{100}}{4} = 25Hz
And the ratio of n1,n2,n3{n_1},{n_2},{n_3} would be 1:3:51:3:5
So n2=3×25=75,n3=5×25=125{n_2} = 3 \times 25 = 75,{n_3} = 5 \times 25 = 125
So n2=f1+f22=75Hz{n_2} = \dfrac{{{f_1} + {f_2}}}{2} = 75Hz

Hence option D would be correct.

Note:
In case of string fixed at both ends or fixed at one end length of the string is constant but wavelengths are varying and hence frequencies vary. If one clearly observes in the first case i.e both ends, the fixed case ratio of frequencies will be 1:2:3:4:5….. and in the second case it would be 1:3:5:7…. and so on. So without calculations if we find first fundamental frequencies in both cases we can find the other frequencies.