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Question: A travelling wave represented by y(x, t) = a sin (kx – \(\omega\)t) is superimposed on another wave ...

A travelling wave represented by y(x, t) = a sin (kx – ω\omegat) is superimposed on another wave represented by y(x, t) = a sin (kx + ω\omegat). The resultant is a

A

Standing wave having nodes at x =(n+12)λ2;\left( n + \frac{1}{2} \right)\frac{\lambda}{2}; n = 0, 1, 2, ....

B

Standing wave having nodes at x = nλ2\frac{n\lambda}{2}; n = 0, 1, 2, ...

C

Wave travelling along + x direction

D

Wave travelling along – x direction

Answer

Standing wave having nodes at x = nλ2\frac{n\lambda}{2}; n = 0, 1, 2, ...

Explanation

Solution

According to the principle of superposition, the resultant wave is

y=asin(kxωt)+asin(kx+ωt)y = a\sin(kx - \omega t) + a\sin(kx + \omega t)

2asinkxcosωt2a\sin kx\cos\omega t …. (i)

It represent a standing wave. In the standing wave, there will be nodes (where amplitude is zero) and antinodes (where amplitude is largest).

For Eq. (i), the positions of nodes are given by

Sin k x = 0

kx=nπ;\Rightarrow kx = n\pi; n = 0,1,2, ……..

Or 2πλx=nπ,\frac{2\pi}{\lambda}x = n\pi, n=0,1,2,……..

Or x=nλ2;x = \frac{n\lambda}{2}; n= 0,1,2, ……….

In the same way,

From Eq. (i), the positions of antinodes are given by

sinkx=1\left| \sin kx \right| = 1

kx=(n+12)π;n=0,1,2,.......\Rightarrow kx = \left( n + \frac{1}{2} \right)\pi;n = 0,1,2,.......

Or 2πxλ=(n+12)π;n=0,1,2,.......\frac{2\pi x}{\lambda} = \left( n + \frac{1}{2} \right)\pi;n = 0,1,2,.......

Or x=(n+12)λ2;n=0,1,2,......x = \left( n + \frac{1}{2} \right)\frac{\lambda}{2};n = 0,1,2,......