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The speed of sound in a particular gas a...

The speed of sound in a particular gas at a temperature `27""^(@)C` is 340 m/s. Then, the speed of sound in the same gas at a temperature `90""^(@)C` is:

A

340 m/s

B

357 m/s

C

374 m/s

D

411.4 m/s

Text Solution

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The correct Answer is:
To find the speed of sound in a gas at a different temperature, we can use the relationship between the speed of sound and temperature. The speed of sound in a gas is given by the formula: \[ V = \sqrt{\frac{\gamma RT}{M}} \] Where: - \( V \) is the speed of sound - \( \gamma \) is the adiabatic constant (which remains constant for the same gas) - \( R \) is the gas constant (which also remains constant) - \( T \) is the absolute temperature in Kelvin - \( M \) is the molecular mass of the gas (which remains constant) ### Step-by-Step Solution 1. **Identify the initial conditions**: - Given temperature \( T_1 = 27^\circ C \) - Speed of sound at \( T_1 \), \( V_1 = 340 \, \text{m/s} \) 2. **Convert the initial temperature to Kelvin**: \[ T_1 = 27 + 273 = 300 \, \text{K} \] 3. **Identify the final temperature**: - Given temperature \( T_2 = 90^\circ C \) 4. **Convert the final temperature to Kelvin**: \[ T_2 = 90 + 273 = 363 \, \text{K} \] 5. **Use the relationship between the speeds and temperatures**: Since \( V \) is directly proportional to the square root of \( T \), we can write: \[ \frac{V_2}{V_1} = \sqrt{\frac{T_2}{T_1}} \] 6. **Substitute the known values**: \[ \frac{V_2}{340} = \sqrt{\frac{363}{300}} \] 7. **Calculate \( \sqrt{\frac{363}{300}} \)**: \[ \sqrt{\frac{363}{300}} = \sqrt{1.21} \] 8. **Calculate \( \sqrt{1.21} \)**: \[ \sqrt{1.21} \approx 1.1 \] 9. **Substitute back to find \( V_2 \)**: \[ V_2 = 340 \times 1.1 = 374 \, \text{m/s} \] ### Final Answer The speed of sound in the gas at \( 90^\circ C \) is approximately \( 374 \, \text{m/s} \). ---

To find the speed of sound in a gas at a different temperature, we can use the relationship between the speed of sound and temperature. The speed of sound in a gas is given by the formula: \[ V = \sqrt{\frac{\gamma RT}{M}} \] Where: - \( V \) is the speed of sound - \( \gamma \) is the adiabatic constant (which remains constant for the same gas) - \( R \) is the gas constant (which also remains constant) ...
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