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Question: The linear density of a vibrating spring is \(1.3 \times {10^{ - 4}}kg/m\) . A transverse wave propa...

The linear density of a vibrating spring is 1.3×104kg/m1.3 \times {10^{ - 4}}kg/m . A transverse wave propagating on the string is described by the equation y=0.021sin(x+30t)y = 0.021\sin (x + 30t) where x and y are measured in meter and t in second. Tension in the string is
(A) 0.12N0.12N
(B) 0.48N0.48N
(C) 1.20N1.20N
(D) 4.80N4.80N

Explanation

Solution

If the wavelength and the angular frequency of a wave is respectively λ\lambda and ω\omega then the equation of a wave is y(x,t)=Asin(2πλxωt+φ)y(x,t) = A\sin (\dfrac{{2\pi }}{\lambda }x \mp \omega t + \varphi ) where A is the amplitude and φ\varphi is the phase shift.

Complete step by step answer:
The velocity of a wave (V) = wavelength (λ\lambda ) ×\times frequency (f)
Now the given wave equation is y=0.021sin(x+30t)y = 0.021\sin (x + 30t) where x and y are measured in meter and t in second. So comparing this equation with the general wave equation we get
2πλ=1\dfrac{{2\pi }}{\lambda } = 1 and ω=30\omega = 30
So λ=2π\lambda = 2\pi
Now the angular frequency (ω\omega ) is 3030 so the regular frequency (f) will be 302π\dfrac{{30}}{{2\pi }}
The velocity of the wave is =λ×f = \lambda \times f =2π×302π=30 = 2\pi \times \dfrac{{30}}{{2\pi }} = 30 m/sm/s
We know that if the linear mass density and the tension of a string are respectively μ\mu and TT the velocity of the wave propagating on the string is V=TμV = \sqrt {\dfrac{T}{\mu }}
According to the question μ=1.3×104kg/m\mu = 1.3 \times {10^{ - 4}}kg/m and we got V=30m/sV = 30m/s
So, T=V2×μT = {V^2} \times \mu
T=90×1.3×104 T=.117  \Rightarrow T = 90 \times 1.3 \times {10^{ - 4}} \\\ \Rightarrow T = .117 \\\
Therefore, the tension, T=.117N0.12NT = .117N \approx 0.12N

The correct answer is option A.

Note: The velocity of a wave propagating on a string can be got by the ratio of angular frequency and the wave number. In this particular problem the wave number (k) is 11 and the relation will be V=ωkV = \dfrac{\omega }{k}.