To determine the temperature at which an organ pipe filled with nitrogen gas will resonate at the same frequency of 300 Hz as it did with oxygen gas at 47 °C, we need to understand how the speed of sound in a gas is affected by its temperature and molecular composition. The frequency of a sound wave in a pipe is related to the speed of sound in the gas and the length of the pipe.
Understanding the Basics
The fundamental frequency (first harmonic) of a pipe is given by the formula:
Where:
- f is the frequency (in Hz),
- v is the speed of sound in the gas (in m/s), and
- λ is the wavelength (in meters).
For a pipe open at both ends, the wavelength is related to the length of the pipe (L) by:
Thus, we can express the frequency in terms of the speed of sound and the length of the pipe:
Speed of Sound in Gases
The speed of sound in a gas can be calculated using the formula:
Where:
- γ is the adiabatic index (ratio of specific heats),
- R is the universal gas constant (approximately 8.314 J/(mol·K)),
- T is the absolute temperature in Kelvin, and
- M is the molar mass of the gas in kg/mol.
Calculating for Oxygen
For oxygen (O₂), the molar mass is about 0.032 kg/mol, and the adiabatic index (γ) is approximately 1.4. First, we convert the temperature from Celsius to Kelvin:
- T₁ = 47 °C + 273.15 = 320.15 K
Now we can calculate the speed of sound in oxygen:
- v₁ = √(1.4 × 8.314 × 320.15 / 0.032)
Calculating this gives:
Finding the Temperature for Nitrogen
Now, we need to find the temperature at which nitrogen (N₂) will produce the same frequency. The molar mass of nitrogen is about 0.028 kg/mol, and its adiabatic index is also approximately 1.4. We set the speed of sound in nitrogen equal to the speed of sound in oxygen:
Using the speed of sound formula for nitrogen:
- 316.5 = √(1.4 × 8.314 × T₂ / 0.028)
Squaring both sides gives:
- 100145.25 = (1.4 × 8.314 × T₂ / 0.028)
Now, solving for T₂:
- T₂ = (100145.25 × 0.028) / (1.4 × 8.314)
Calculating this yields:
Finally, converting this back to Celsius:
- T₂ = 120.6 K - 273.15 ≈ -152.55 °C
Summary
To resonate at the same frequency of 300 Hz in the fundamental mode, the organ pipe filled with nitrogen gas would need to be at approximately -152.55 °C. This significant drop in temperature highlights how the properties of gases can dramatically influence sound propagation.