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An organ pipe of (3.9 pi) mlong, open at...

An organ pipe of `(3.9 pi) m`long, open at both ends is driver to third harmonic standing wave. If the amplitude of pressure oscillation is `1%` of mean atmospheric pressure `[p_(o) = 10^(5) N//m^(2)]`. The maximum displacement of particle from mean position will be [Given, velocity of sound `= 200 m//s` and density of air `= 1.3 kg//m^(3)]`

A

`2.5 cm`

B

`5 cm`

C

`1 cm`

D

`2 cm`

Text Solution

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The correct Answer is:
To solve the problem step by step, we will follow the given information and apply the relevant physics concepts. ### Step 1: Understand the given data - Length of the organ pipe, \( L = 3.9 \pi \, \text{m} \) - The organ pipe is open at both ends and is in the third harmonic. - Amplitude of pressure oscillation is \( 1\% \) of mean atmospheric pressure, \( p_0 = 10^5 \, \text{N/m}^2 \). - Velocity of sound, \( v = 200 \, \text{m/s} \). - Density of air, \( \rho = 1.3 \, \text{kg/m}^3 \). ### Step 2: Calculate the pressure amplitude The pressure amplitude \( \Delta P_{\text{max}} \) can be calculated as: \[ \Delta P_{\text{max}} = p_0 \times \frac{1}{100} = 10^5 \times 0.01 = 10^3 \, \text{N/m}^2 \] ### Step 3: Relate pressure amplitude to displacement amplitude The relationship between pressure amplitude and displacement amplitude is given by: \[ \Delta P_{\text{max}} = \rho v \omega A \] where: - \( \omega = 2 \pi f \) (angular frequency), - \( A \) is the displacement amplitude. ### Step 4: Determine the wavelength for the third harmonic For an organ pipe open at both ends, the length of the pipe is related to the wavelength \( \lambda \) by: \[ L = \frac{3}{2} \lambda \quad \Rightarrow \quad \lambda = \frac{2L}{3} \] Substituting \( L = 3.9 \pi \): \[ \lambda = \frac{2 \times (3.9 \pi)}{3} = 2.6 \pi \, \text{m} \] ### Step 5: Calculate the frequency The speed of sound is related to frequency and wavelength by: \[ v = f \lambda \quad \Rightarrow \quad f = \frac{v}{\lambda} \] Substituting the values: \[ f = \frac{200}{2.6 \pi} \approx \frac{200}{8.168} \approx 24.5 \, \text{Hz} \] ### Step 6: Calculate angular frequency The angular frequency \( \omega \) is given by: \[ \omega = 2 \pi f = 2 \pi \times 24.5 \approx 154.3 \, \text{rad/s} \] ### Step 7: Substitute values to find displacement amplitude Now we can rearrange the equation for pressure amplitude to find the displacement amplitude \( A \): \[ A = \frac{\Delta P_{\text{max}}}{\rho v \omega} \] Substituting the known values: \[ A = \frac{10^3}{1.3 \times 200 \times 154.3} \] Calculating the denominator: \[ 1.3 \times 200 \times 154.3 \approx 40000 \] Thus, \[ A = \frac{1000}{40000} = 0.025 \, \text{m} \] ### Step 8: Convert to centimeters To convert meters to centimeters: \[ A = 0.025 \, \text{m} = 2.5 \, \text{cm} \] ### Final Answer The maximum displacement of the particle from the mean position is \( 2.5 \, \text{cm} \). ---

To solve the problem step by step, we will follow the given information and apply the relevant physics concepts. ### Step 1: Understand the given data - Length of the organ pipe, \( L = 3.9 \pi \, \text{m} \) - The organ pipe is open at both ends and is in the third harmonic. - Amplitude of pressure oscillation is \( 1\% \) of mean atmospheric pressure, \( p_0 = 10^5 \, \text{N/m}^2 \). - Velocity of sound, \( v = 200 \, \text{m/s} \). - Density of air, \( \rho = 1.3 \, \text{kg/m}^3 \). ...
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