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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 clamped at both ends is set into vibration by a 660 Hz...

A string clamped at both ends is set into vibration by a 660 Hz660 \text{ Hz} tuning fork, causing it to vibrate in three loops. The wave speed for a transverse wave on the string is 220 m s−1220 \text{ m s}^{-1}. If the maximum amplitude of a particle is 0.5 cm0.5 \text{ cm}, which of the following is a suitable equation describing the motion?

Options

  1. A(0.5 cm)sin⁡[(0.06π cm−1)x]cos⁡[(1320π s−1)t](0.5 \text{ cm}) \sin[(0.06\pi \text{ cm}^{-1})x] \cos[(1320\pi \text{ s}^{-1})t]
  2. B(0.5 cm)sin⁡[(0.06π cm−1)x]cos⁡[(660π s−1)t](0.5 \text{ cm}) \sin[(0.06\pi \text{ cm}^{-1})x] \cos[(660\pi \text{ s}^{-1})t]
  3. C(0.5 cm)cos⁡[(0.06π cm−1)x]cos⁡[(1320π s−1)t](0.5 \text{ cm}) \cos[(0.06\pi \text{ cm}^{-1})x] \cos[(1320\pi \text{ s}^{-1})t]
  4. D(0.5 cm)sin⁡[(6π cm−1)x]cos⁡[(1320π s−1)t](0.5 \text{ cm}) \sin[(6\pi \text{ cm}^{-1})x] \cos[(1320\pi \text{ s}^{-1})t]

Correct answer

A. (0.5 cm)sin⁡[(0.06π cm−1)x]cos⁡[(1320π s−1)t](0.5 \text{ cm}) \sin[(0.06\pi \text{ cm}^{-1})x] \cos[(1320\pi \text{ s}^{-1})t]

Step-by-step solution

Given frequency f=660 Hzf = 660 \text{ Hz} and wave speed v=220 m s−1=22000 cm s−1v = 220 \text{ m s}^{-1} = 22000 \text{ cm s}^{-1}.

Angular frequency ω=2πf=2π×660=1320π rad s−1\omega = 2\pi f = 2\pi \times 660 = 1320\pi \text{ rad s}^{-1}.

Wave number k=ωv=1320π22000=0.06π cm−1k = \dfrac{\omega}{v} = \dfrac{1320\pi}{22000} = 0.06\pi \text{ cm}^{-1}.

Since the string is clamped at both ends, the displacement at x=0x = 0 must be zero at all times. Therefore, the spatial part of the standing wave equation must be a sine function, sin⁡(kx)\sin(kx).

The maximum amplitude of the standing wave is given as A=0.5 cmA = 0.5 \text{ cm}.

The equation of the standing wave is of the form y(x,t)=Asin⁡(kx)cos⁡(ωt)y(x,t) = A \sin(kx) \cos(\omega t).

Substituting the values, we get:

y(x,t)=(0.5 cm)sin⁡[(0.06π cm−1)x]cos⁡[(1320π s−1)t]y(x,t) = (0.5 \text{ cm}) \sin[(0.06\pi \text{ cm}^{-1})x] \cos[(1320\pi \text{ s}^{-1})t]
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