Question:

The displacement of a plane progressive wave in a medium, traveling towards the positive x-axis with velocity 4m/s at t=0 is given by \(y=3sin2\pi(-\frac{x}{3})\). Then the expression for the displacement at a later time t=4 sec will be

Updated On: Apr 2, 2025
  • \(y=3\,sin2\pi(-\frac{x-16}{3})\)
  • \(y=3\,sin2\pi(\frac{-x-16}{3})\)
  • \(y=3\,sin2\pi(\frac{-x+1}{3})\)
  • \(y=3\,sin2\pi(\frac{-x-1}{3})\)
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The Correct Option is A

Approach Solution - 1

The given wave equation is \(y=3sin(2π(−3x​))\), representing a plane progressive wave traveling towards the positive x-axis with a velocity of 4 m/s at t=0.
To justify the answer \(y=3sin(2π(−3x−16))\), we need to account for the wave's velocity. The general form of a plane wave equation is \(y=Asin(kx−ωt+ϕ)\), where k is the wave number, ω is the angular frequency, and ϕ is the phase angle.
Given that the wave's velocity is 4 m/s, we know that \(v=kω\)​, and in this case, v=4. By equating v with the phase velocity ​, we can find the relationship between ω and k. Then, we substitute these values into the general equation and adjust the phase angle ϕ to match the initial condition at t=0.
This process leads to the answer \(y=3sin(2π(−3x−16))\), which correctly represents the displacement of the wave as it travels towards the positive x-axis with the given velocity and initial condition.
The correct option is(A): \(y=3\,sin2\pi(-\frac{x-16}{3})\)

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Approach Solution -2

The general equation for a wave propagating in one dimension can be written as :
\(y=Asin(kx−ωt+ϕ)\), where \(A\) represents the amplitude, \(\omega\) is the angular frequency, \(k\) is the wave number, \(x\) denotes the position, \(t\) is the time, and \(\phi\) is the phase constant.
Given wave equation is \(y=3\sin2\pi(-\frac{x}{3})\). This can be rewritten as \(y=3\sin(-2\pi\frac{x}{3})\) which corresponds to the form \(y=A\sin(\omega t-kx)\) where \(\omega t\) is 0, i.e \(t = 0\)\(A=3\) and \(k\ \text{is}\ -\frac{2\pi}{3}\).
The negative sign of \(k\) indicates that the wave propagates in the negative \(x\)-direction, whereas the problem specifies that the wave moves in the positive \(x\)-direction.
Therefore, we should consider \(k\) as positive, i.e \(k=\frac{2\pi}{3}.\)
Speed of wave \(v\) is given by \(v=\frac{\omega}{k}\).
According to the information provided in the problem, \(v=4\ m/s\).
By substituting these values, we can determine \(\omega:4=\frac{\omega}{2\pi/3}\) which gives \(\omega=\frac{8\pi}{3}\).
Thus, the wave equation at any time \(t\) can be expressed as \(y=3\sin[\frac{8\pi}{3}t-\frac{2\pi}{3}x].\)
Next, we want to determine the wave equation at \(t = 4\) seconds.
Now, Substituting \(t=4\), into the equation gives \(y=3\sin[\frac{8\pi}{3}\times4-\frac{2\pi}{3}x].\)
Upon simplifying the argument of the sine function, we obtain
\(y=3\sin2\pi(\frac{-x+16}{3}).\)
Upon rearranging the argument of the sine function once more, we obtain
\(y=3\sin2\pi(-\frac{x+16}{3}).\)
So, the correct option is (A) : \(y=3\,sin2\pi(-\frac{x-16}{3})\)

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Concepts Used:

Electromagnetic waves

The waves that are produced when an electric field comes into contact with a magnetic field are known as Electromagnetic Waves or EM waves. The constitution of an oscillating magnetic field and electric fields gives rise to electromagnetic waves.

Types of Electromagnetic Waves:

Electromagnetic waves can be grouped according to the direction of disturbance in them and according to the range of their frequency. Recall that a wave transfers energy from one point to another point in space. That means there are two things going on: the disturbance that defines a wave, and the propagation of wave. In this context the waves are grouped into the following two categories:

  • Longitudinal waves: A wave is called a longitudinal wave when the disturbances in the wave are parallel to the direction of propagation of the wave. For example, sound waves are longitudinal waves because the change of pressure occurs parallel to the direction of wave propagation.
  • Transverse waves: A wave is called a transverse wave when the disturbances in the wave are perpendicular (at right angles) to the direction of propagation of the wave.