Step 1: The general equation of a stationary wave is: \[ y = A \sin(kx) \cos(\omega t) \] where:
- \( A \) is the amplitude,
- \( k \) is the wave number,
- \( x \) is the position,
- \( \omega \) is the angular frequency.
In the given equation, we have \( y = 5 \sin \frac{\pi}{2} \cos 10\pi t \).
Step 2: The wave number \( k \) is related to the wavelength \( \lambda \) by: \[ k = \frac{2\pi}{\lambda} \] From the given equation, \( k = \frac{\pi}{2} \), so the wavelength \( \lambda \) is: \[ \lambda = \frac{2\pi}{k} = \frac{2\pi}{\pi/2} = 4 \, {cm} \] Step 3: The distance between two consecutive nodes is half the wavelength: \[ {Distance between nodes} = \frac{\lambda}{2} = \frac{4}{2} = 2 \, {cm} \] Thus, the distance between two consecutive nodes is 2 cm.
Match List-I with List-II on the basis of two simple harmonic signals of the same frequency and various phase differences interacting with each other:
LIST-I (Lissajous Figure) | LIST-II (Phase Difference) | ||
---|---|---|---|
A. | Right handed elliptically polarized vibrations | I. | Phase difference = \( \frac{\pi}{4} \) |
B. | Left handed elliptically polarized vibrations | II. | Phase difference = \( \frac{3\pi}{4} \) |
C. | Circularly polarized vibrations | III. | No phase difference |
D. | Linearly polarized vibrations | IV. | Phase difference = \( \frac{\pi}{2} \) |
Choose the correct answer from the options given below: