Question #65640

The linear density of a vibrating string is 1.3 × 10^-4 kg m1. A transverse wave is propagating on the string and is described by the equation y (x, t) = 0.021 sin (30t - x) where x and y are in metres and t is in seconds. Calculate the tension in the string.
1

Expert's answer

2017-03-07T11:53:05-0500

Answer on Question #65640, Physics / Mechanics | Relativity

The linear density of a vibrating string is 1.3×104 kg m31.3 \times 10^{\wedge} - 4\ \mathrm{kg\ m^{-3}}. A transverse wave is propagating on the string and is described by the equation y(x,t)=0.021sin(30tx)y(x,t) = 0.021\sin(30t - x) where xx and yy are in metres and tt is in seconds. Calculate the tension in the string.

Find: T?T - ?

Given:


ρ=1.3×104 kg×m3y(x,t)=0.021sin(30tx)\begin{array}{l} \rho = 1.3 \times 10^{-4}\ \mathrm{kg} \times \mathrm{m}^{-3} \\ y(x,t) = 0.021\sin(30t - x) \\ \end{array}


Solution:

Wave velocity:


v=Tρ(1), where T is tension, ρ is densityOf (1)v2=Tρ(2)Of (2)T=v2×ρ(3)v = \sqrt{\frac{T}{\rho}}(1), \text{ where } T \text{ is tension, } \rho \text{ is density} \\ \text{Of } (1) \Rightarrow v^2 = \frac{T}{\rho}(2) \\ \text{Of } (2) \Rightarrow T = v^2 \times \rho(3) \\


Wave velocity:


v=f×λ(4)v = f \times \lambda(4)


Linear frequency:


f=ω2π(5), where ω is cyclic frequencyf = \frac{\omega}{2\pi}(5), \text{ where } \omega \text{ is cyclic frequency}


Wavelength:


λ=2πk(6), where k is wave number\lambda = \frac{2\pi}{k}(6), \text{ where } k \text{ is wave number}


(5) and (6) in (4):


v=ω2π×2πk=ωk(7)v = \frac{\omega}{2\pi} \times \frac{2\pi}{k} = \frac{\omega}{k}(7)


Equation of plane wave:


y(x,t)=Asin(ωtx)(8)y(x,t) = A \sin(\omega t - x)(8)


From the condition of the task:


y(x,t)=0.021sin(30tx)(9)y(x,t) = 0.021\sin(30t - x)(9)


Of (8) and (9) ω=30 s1, k=1 m1(10)\Rightarrow \omega = 30\ \mathrm{s}^{-1},\ k = 1\ \mathrm{m}^{-1}(10)

(10) in (7): v=30 m×s1(11)v = 30\ \mathrm{m} \times \mathrm{s}^{-1}(11)

(11) in (3) T=0.117 NT = 0.117\ \mathrm{N}

Answer:

0.117 N

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