JEE Challenger
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Velocity of Point on Transverse Sinusoidal Wave

A transverse sinusoidal wave moves along a string in the positive xx-direction at a speed of 10 cm/s10\text{ cm/s}. The wavelength of the wave is 0.5 m0.5\text{ m} and its amplitude is 10 cm10\text{ cm}. At a particular time tt, the snap-shot of the wave is shown in figure. The velocity of point P when its displacement is 5 cm5\text{ cm} is

Diagram 0

Options

A

3π50j^ m/s\frac{\sqrt{3}\pi}{50}\hat{j}\text{ m/s}

Correct
B

−3π50j^ m/s-\frac{\sqrt{3}\pi}{50}\hat{j}\text{ m/s}

C

3π50i^ m/s\frac{\sqrt{3}\pi}{50}\hat{i}\text{ m/s}

D

−3π50i^ m/s-\frac{\sqrt{3}\pi}{50}\hat{i}\text{ m/s}

Topics & Concepts

Step-by-Step Solution

To find the velocity of point PP on the string, we first determine the frequency, angular frequency, and magnitude of particle velocity, followed by its direction using the wave profile.

1. Calculation of Wave Parameters

Given:

  • Wave speed, v=10 cm/s=0.1 m/sv = 10\text{ cm/s} = 0.1\text{ m/s}
  • Wavelength, λ=0.5 m\lambda = 0.5\text{ m}
  • Amplitude, A=10 cm=0.1 mA = 10\text{ cm} = 0.1\text{ m}
  • Displacement at point PP, y=5 cm=0.05 my = 5\text{ cm} = 0.05\text{ m}

The angular frequency ω\omega of the wave is given by:
ω=2πf=2π(vλ)=2π(0.1 m/s0.5 m)=2π5 rad/s\omega = 2\pi f = 2\pi \left(\frac{v}{\lambda}\right) = 2\pi \left(\frac{0.1\text{ m/s}}{0.5\text{ m}}\right) = \frac{2\pi}{5}\text{ rad/s}

2. Magnitude of Particle Velocity

The speed of a particle performing Simple Harmonic Motion at displacement yy is given by:
∣vp∣=ωA2−y2|v_p| = \omega \sqrt{A^2 - y^2}

Substituting the given values:
∣vp∣=(2π5)(0.1)2−(0.05)2=(2π5)0.0075=(2π5)(320)=3π50 m/s|v_p| = \left(\frac{2\pi}{5}\right) \sqrt{(0.1)^2 - (0.05)^2} = \left(\frac{2\pi}{5}\right) \sqrt{0.0075} = \left(\frac{2\pi}{5}\right) \left(\frac{\sqrt{3}}{20}\right) = \frac{\sqrt{3}\pi}{50}\text{ m/s}

3. Direction of Velocity

The particle velocity vyv_y at any point on a transverse wave traveling in the positive xx-direction is related to the slope of the wave profile by:
vy=−v(∂y∂x)v_y = -v \left(\frac{\partial y}{\partial x}\right)

From the given snapshot of the wave:

  • At point PP, the string has a negative slope, i.e., ∂y∂x<0\frac{\partial y}{\partial x} < 0.
  • Since v>0v > 0 (wave travels along +x+x), the particle velocity is:
    vy=−(+v)(−slope)>0v_y = - (+v)(-\text{slope}) > 0

Thus, the particle at PP is moving upwards in the positive yy-direction (+j^+\hat{j}). Alternatively, as the wave shifts to the right, the crest approaches point PP, causing its displacement to increase upwards.

Conclusion

The velocity vector of point PP is:
v⃗P=3π50j^ m/s\vec{v}_P = \frac{\sqrt{3}\pi}{50}\hat{j}\text{ m/s}

Correct Answer: A