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Concepts Of Physics MCQ Edition [Volume 1]
Exam
Concepts Of Physics MCQ Edition [Volume 1]
Subject
Physics
Chapter
Wave Motion and Waves on a String

Concepts Of Physics MCQ Edition [Volume 1] · Physics · Wave Motion and Waves on a String

A string, 2 m long and fixed at both ends, is set into vibrations...

A string, 2 m2 \text{ m} long and fixed at both ends, is set into vibrations in its first overtone. The wave speed on the string is 200 m s−1200 \text{ m s}^{-1} and the amplitude is 0.5 cm0.5 \text{ cm}. Determine the equation giving the displacement of different points as a function of time. Choose the XX-axis along the string with the origin at one end and t=0t = 0 at the instant when the point x=50 cmx = 50 \text{ cm} has reached its maximum displacement.

Options

  1. A(0.5 cm)sin⁡[(2π m−1)x]cos⁡[(100π s−1)t](0.5 \text{ cm}) \sin[(2\pi \text{ m}^{-1})x] \cos[(100\pi \text{ s}^{-1})t]
  2. B(0.5 cm)sin⁡[(π2 m−1)x]cos⁡[(100π s−1)t](0.5 \text{ cm}) \sin[\left(\dfrac{\pi}{2} \text{ m}^{-1}\right)x] \cos[(100\pi \text{ s}^{-1})t]
  3. C(0.5 cm)sin⁡[(π m−1)x]sin⁡[(200π s−1)t](0.5 \text{ cm}) \sin[(\pi \text{ m}^{-1})x] \sin[(200\pi \text{ s}^{-1})t]
  4. D(0.5 cm)sin⁡[(π m−1)x]cos⁡[(200π s−1)t](0.5 \text{ cm}) \sin[(\pi \text{ m}^{-1})x] \cos[(200\pi \text{ s}^{-1})t]

Correct answer

D. (0.5 cm)sin⁡[(π m−1)x]cos⁡[(200π s−1)t](0.5 \text{ cm}) \sin[(\pi \text{ m}^{-1})x] \cos[(200\pi \text{ s}^{-1})t]

Step-by-step solution

For a string fixed at both ends, the wavelength in the first overtone (n=2n = 2) is given by L=2(λ2)=λL = 2 \left(\dfrac{\lambda}{2}\right) = \lambda.

Given L=2 mL = 2 \text{ m}, we have λ=2 m\lambda = 2 \text{ m}.

The wave number kk is k=2πλ=π m−1k = \dfrac{2\pi}{\lambda} = \pi \text{ m}^{-1}.

The angular frequency ω\omega is ω=vk=200×π=200π s−1\omega = v k = 200 \times \pi = 200\pi \text{ s}^{-1}.

The general equation for a standing wave with nodes at x=0x = 0 and x=Lx = L is y(x,t)=Asin⁡(kx)cos⁡(ωt+ϕ)y(x, t) = A \sin(kx) \cos(\omega t + \phi).

Given the amplitude A=0.5 cmA = 0.5 \text{ cm}.

At t=0t = 0, the point x=50 cm=0.5 mx = 50 \text{ cm} = 0.5 \text{ m} has maximum displacement.

Substituting x=0.5 mx = 0.5 \text{ m} into the spatial part gives sin⁡(π×0.5)=1\sin(\pi \times 0.5) = 1, which means it is an antinode.

For the displacement to be maximum at t=0t = 0, the temporal part cos⁡(ω×0+ϕ)=cos⁡(ϕ)\cos(\omega \times 0 + \phi) = \cos(\phi) must be 11, giving ϕ=0\phi = 0.

Therefore, the equation of the standing wave is y(x,t)=(0.5 cm)sin⁡[(π m−1)x]cos⁡[(200π s−1)t]y(x, t) = (0.5 \text{ cm}) \sin[(\pi \text{ m}^{-1})x] \cos[(200\pi \text{ s}^{-1})t].
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