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Two waves of slightly different frequenc...

Two waves of slightly different frequencies `f_(1) and f_(2) (f_(1) gt f_(2))` with zero phase difference , same amplitudes ,travelling in the same direction superimpose .

A

Phenomenon of beats is always observed by human ear.

B

Intensity of resultant wave is a constant.

C

Intensity of resultant wave varies periodically with time with maximum intensity `4 a^(2)` and minimum intensity zero.

D

A maxima appears at a time `1//[2 (f_(1) - f_(2))]` later ( or earlier ) than a minima appears .

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To solve the problem of two waves of slightly different frequencies \( f_1 \) and \( f_2 \) (where \( f_1 > f_2 \)), with zero phase difference and the same amplitudes, we will analyze the situation step by step. ### Step-by-Step Solution: 1. **Understanding Wave Properties**: - We have two waves described by the following equations: \[ y_1 = A \sin(2\pi f_1 t) \] \[ y_2 = A \sin(2\pi f_2 t) \] where \( A \) is the amplitude of the waves. 2. **Superposition of Waves**: - When these two waves superimpose, the resultant wave \( y \) can be expressed as: \[ y = y_1 + y_2 = A \sin(2\pi f_1 t) + A \sin(2\pi f_2 t) \] 3. **Using the Trigonometric Identity**: - We can use the trigonometric identity for the sum of sines: \[ \sin a + \sin b = 2 \sin\left(\frac{a+b}{2}\right) \cos\left(\frac{a-b}{2}\right) \] - Applying this identity, we get: \[ y = 2A \sin\left(\pi (f_1 + f_2) t\right) \cos\left(\pi (f_1 - f_2) t\right) \] 4. **Resultant Amplitude and Intensity**: - The amplitude of the resultant wave varies with time and is given by: \[ A_{resultant} = 2A \cos\left(\pi (f_1 - f_2) t\right) \] - The intensity \( I \) of the wave is proportional to the square of the amplitude: \[ I \propto A_{resultant}^2 = (2A \cos(\pi (f_1 - f_2) t))^2 = 4A^2 \cos^2(\pi (f_1 - f_2) t) \] - This indicates that the intensity varies periodically with time, reaching a maximum of \( 4A^2 \) and a minimum of \( 0 \). 5. **Beat Frequency**: - The beat frequency \( f_{beat} \) is given by the difference in frequencies: \[ f_{beat} = f_1 - f_2 \] - The time period of the beats \( T_{beat} \) is: \[ T_{beat} = \frac{1}{f_{beat}} = \frac{1}{f_1 - f_2} \] 6. **Time Difference Between Maxima and Minima**: - Maxima occur at times \( t = \frac{n}{f_{beat}} \) (where \( n \) is an integer). - Minima occur at times \( t = \frac{(2n + 1)}{2f_{beat}} \). - The time difference between a maximum and the nearest minimum is: \[ \Delta t = \frac{1}{2f_{beat}} = \frac{1}{2(f_1 - f_2)} \] ### Conclusion: - The correct options based on the analysis are: - The intensity of the resultant wave varies periodically with time (correct). - A maxima appears at a time \( \frac{1}{2(f_1 - f_2)} \) later or earlier than a minima appears (correct).

To solve the problem of two waves of slightly different frequencies \( f_1 \) and \( f_2 \) (where \( f_1 > f_2 \)), with zero phase difference and the same amplitudes, we will analyze the situation step by step. ### Step-by-Step Solution: 1. **Understanding Wave Properties**: - We have two waves described by the following equations: \[ y_1 = A \sin(2\pi f_1 t) ...
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