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Question: Equations of a stationary wave and a travelling wave are \(y_1 = a\;sin(kx)cos(\omega t)\) and \(y_2...

Equations of a stationary wave and a travelling wave are y1=a  sin(kx)cos(ωt)y_1 = a\;sin(kx)cos(\omega t) and y2=a  sin(ωtkx)y_2 = a\;sin(\omega t-kx). The phase difference between two points x1=π3kx_1 = \dfrac{\pi}{3k} and x2=3π2kx_2 =\dfrac{3\pi}{2k} is ϕ1\phi_1 for the first wave and ϕ2\phi_2 for the second wave. The ratio ϕ1ϕ2\dfrac{\phi_1}{\phi_2} is:
A. 1
B. 56\dfrac{5}{6}
C. 34\dfrac{3}{4}
D. 67\dfrac{6}{7}

Explanation

Solution

Begin by first finding the number of nodes that lie between the two points in a stationary wave. From this you can deduce the phase difference of the stationary wave by looking at which node region lies across both the points. After this determine the phase difference between the two points in the travelling wave by calculating the difference between the two positions. Then divide the two to get the final ratio.

Formula Used: For a travelling wave, phase difference between two points: ϕ=kΔx\phi = k\Delta x, where k is the wave vector and Δx\Delta x is the difference between the position of two points.
For a stationary wave, phase difference between two points: ϕ=nπ\phi = n\pi, where n is the number of nodes.

Complete answer:
Let us first consider the stationary wave whose equation is given by y1=a  sin(kx)cos(ωt)y_1 = a\;sin(kx)cos(\omega t).
Now, we know that successive nodes in a stationary wave are found at nπn\pi phase difference.
This means that, at node points : sin(kx)=nπx=nπksin(kx) = n\pi \Rightarrow x = \dfrac{n\pi}{k}, where n= 0,1,2, so on.
Therefore, the nodes are found at πk\dfrac{\pi}{k}, 2πk\dfrac{2\pi}{k}, 3πk\dfrac{3\pi}{k}, and so on.
Now, the two points are given as x1=π3kx_1 = \dfrac{\pi}{3k} and x2=3π2kx_2 =\dfrac{3\pi}{2k}.
We see that x1=π3kx_1 = \dfrac{\pi}{3k}<πk\dfrac{\pi}{k}, and πk\dfrac{\pi}{k} < x2=3π2kx_2 = \dfrac{3\pi}{2k}<2πk\dfrac{2\pi}{k}
This means that there is only one node between the two points, given by
Now, from kx=nπk(πk)=nπn=1kx = n\pi \Rightarrow k\left(\dfrac{\pi}{k}\right) = n\pi \Rightarrow n = 1
The, kx=πx=πkkx = \pi \Rightarrow x = \dfrac{\pi}{k}
And this gives a phase difference
ϕ1=kx=k(πk)ϕ1=π\phi_1 = kx = k\left(\dfrac{\pi}{k}\right) \Rightarrow \phi_1 = \pi for the stationary wave.
For the travelling wave, the phase difference ϕ2\phi_2 is given as:
ϕ2=k(x2)k(x1)=k(x2x1)=k(3π2kπ3k)=3π2π3=9π2π6ϕ2=7π6\phi_2 = k(x_2)-k(x_1) = k(x_2-x_1) = k\left(\dfrac{3\pi}{2k}-\dfrac{\pi}{3k}\right) = \dfrac{3\pi}{2} - \dfrac{\pi}{3} = \dfrac{9\pi-2\pi}{6} \Rightarrow \phi_2 = \dfrac{7\pi}{6}
Therefore, the ratio of the two phase differences:
ϕ1ϕ2=π(7π6)=6π7π=67\dfrac{\phi_1}{\phi_2} = \dfrac{\pi}{\left(\dfrac{7\pi}{6}\right)} = \dfrac{6\pi}{7\pi} = \dfrac{6}{7}

Therefore, the correct answer will be D. 67\dfrac{6}{7}.

Note:
It is important to determine the number of nodes that lie between the two points on the stationary wave as this is the way to ultimately find the phase difference depending on whether the points are present in successive loops of the wave or not. Note that the two points do not have any nodes at their position since the nodes are formed at π\pi, 2π2\pi, and so on. However, x2x_2 lies at an antinodes lie at π2\dfrac{\pi}{2}, 3π2\dfrac{3\pi}{2} and so on.