Two sound waves emerging from a source reach a point simultaneously along two paths. When the path difference is `12 cm ` or `36 cm`, then there is a silence at that point. If the speed of sound in air be `330 m//s`, then calculate maximum possible frequency of the source.
Two sound waves emerging from a source reach a point simultaneously along two paths. When the path difference is `12 cm ` or `36 cm`, then there is a silence at that point. If the speed of sound in air be `330 m//s`, then calculate maximum possible frequency of the source.
Text Solution
AI Generated Solution
The correct Answer is:
To solve the problem, we need to find the maximum possible frequency of the sound source given the conditions of path difference and the speed of sound. Let's break down the solution step by step.
### Step 1: Understand the condition for silence
When two sound waves interfere destructively, they create silence at a point. This occurs when the path difference between the two waves is an odd multiple of half wavelengths. Mathematically, this can be expressed as:
\[
\Delta x = \left(n + \frac{1}{2}\right) \lambda
\]
where \( n \) is an integer (0, 1, 2, ...).
### Step 2: Identify the path differences
Given path differences are:
- \( \Delta x_1 = 12 \, \text{cm} = 0.12 \, \text{m} \)
- \( \Delta x_2 = 36 \, \text{cm} = 0.36 \, \text{m} \)
### Step 3: Set up the equations
For both path differences, we can set up the equations:
1. For \( \Delta x_1 = 0.12 \, \text{m} \):
\[
0.12 = \left(n_1 + \frac{1}{2}\right) \lambda
\]
2. For \( \Delta x_2 = 0.36 \, \text{m} \):
\[
0.36 = \left(n_2 + \frac{1}{2}\right) \lambda
\]
### Step 4: Find the wavelength
From the two equations, we can express the wavelength \( \lambda \) in terms of \( n_1 \) and \( n_2 \):
\[
\lambda = \frac{0.12}{n_1 + \frac{1}{2}} = \frac{0.36}{n_2 + \frac{1}{2}}
\]
### Step 5: Solve for \( n_1 \) and \( n_2 \)
We can rearrange the equations to find a relationship between \( n_1 \) and \( n_2 \):
\[
0.12(n_2 + \frac{1}{2}) = 0.36(n_1 + \frac{1}{2})
\]
Expanding and simplifying gives:
\[
0.12n_2 + 0.06 = 0.36n_1 + 0.18
\]
\[
0.12n_2 - 0.36n_1 = 0.12
\]
\[
n_2 = 3n_1 + 1
\]
### Step 6: Substitute values
To find the maximum frequency, we need to find the maximum wavelength. The maximum occurs when \( n_1 \) is minimized (i.e., \( n_1 = 0 \)):
\[
n_2 = 1
\]
Substituting \( n_1 = 0 \) into the equation for \( \lambda \):
\[
\lambda = 0.12 \, \text{m}
\]
### Step 7: Calculate frequency
Using the speed of sound \( v = 330 \, \text{m/s} \) and the wavelength \( \lambda \):
\[
f = \frac{v}{\lambda} = \frac{330}{0.12}
\]
Calculating gives:
\[
f = 2750 \, \text{Hz}
\]
### Final Answer
The maximum possible frequency of the source is:
\[
\boxed{2750 \, \text{Hz}}
\]
To solve the problem, we need to find the maximum possible frequency of the sound source given the conditions of path difference and the speed of sound. Let's break down the solution step by step.
### Step 1: Understand the condition for silence
When two sound waves interfere destructively, they create silence at a point. This occurs when the path difference between the two waves is an odd multiple of half wavelengths. Mathematically, this can be expressed as:
\[
\Delta x = \left(n + \frac{1}{2}\right) \lambda
\]
where \( n \) is an integer (0, 1, 2, ...).
...
|
Topper's Solved these Questions
SOUND WAVES
DC PANDEY ENGLISH|Exercise Exercise 19.5|5 VideosView PlaylistSOUND WAVES
DC PANDEY ENGLISH|Exercise INTRODUCTORY EXERCISE|1 VideosView PlaylistSOUND WAVES
DC PANDEY ENGLISH|Exercise Exercise 19.3|4 VideosView PlaylistSOLVD PAPERS 2017 NEET, AIIMS & JIPMER
DC PANDEY ENGLISH|Exercise Solved paper 2018(JIPMER)|38 VideosView PlaylistSUPERPOSITION OF WAVES
DC PANDEY ENGLISH|Exercise Level 2 Subjective|8 VideosView Playlist
Similar Questions
Explore conceptually related problems
In a Quinck's experiment , the sound intensity being detected at an appropriate point , changes from minimum for the second time , when the slidable tube is drawn apart by 9.0 cm . If the speed of sound in air be 336 m//s , then what is the frequency of this sounding source ?
Watch solution
A sound wave starting from source S , follows two paths AOB and ACB to reach the detector D . If ABC is an equilateral traingle , of side l and there is silence at point D , the maximum wavelength (lambda) of sound wave must be
Watch solution
Calculate the frequency of fifth harmonic of a closed organ pipe of length 50cm, if the velocity of sound in air is 330 m/s.
Watch solution
Calculate the frequency of fifth harmonic of a closed organ pipe of length 50cm, if the velocity of sound in air is 330 m/s.
Watch solution
In an organ pipe the distance between the adjacent node is 4 cm . Find the frequency of source if speed of sound in air is 336 m//s .
Watch solution
Sound waves from a tuning fork placed at a point P reach another point Q , by two separate paths PRQ and PSQ . When PSQ is greater than PRQ by 11.5 cm , there is silence at Q . When the difference is 23 cm , the sound becomes loudest at Q , and when 34.5 cm , there is silence , and so on . Explain this effect and calculate the frequency of the fork if the velocity of sound is taken to be 331.2 m//s .
Watch solution
Light waves of wavelength 5460 A, emitted by two coherent sources, meet at a point after travelling different paths. The path difference between the two wave trains at that point is 2.1 mum . then phase difference will be ?
Watch solution
Sound waves of frequency 600 H_(Z) fall normally on perfectly reflecting wall. The distance from the wall at which the air particles have the maximum amplitude of vibration is (speed of sound in air = 330 m//s )
Watch solution
Sound waves of frequency 660 H_(Z) fall normally on perfectly reflecting wall. The distance from the wall at which the air particles have the maximum amplitude of vibration is (speed of sound in air = 330 m//s )
Watch solution
Calculate the minimum distance in air required between the source of sound and the obstacle to hear an echo. Take speed of sound in air = 350 m s^(-1)
Watch solution