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The root mean square velocity of helium ...

The root mean square velocity of helium gas becomes the same as that of methane molecule at `327^@C` , when the temperature is

A

300 K

B

450 K

C

150 K

D

1200 K

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The correct Answer is:
To solve the problem of finding the temperature at which the root mean square (rms) velocity of helium gas equals that of methane gas at 327°C, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the formula for root mean square velocity (vrms)**: The formula for the root mean square velocity of a gas is given by: \[ v_{rms} = \sqrt{\frac{3RT}{M}} \] where: - \( R \) is the universal gas constant, - \( T \) is the temperature in Kelvin, - \( M \) is the molar mass of the gas. 2. **Set up the equation for helium and methane**: We need to equate the rms velocities of helium and methane: \[ v_{rms, \text{He}} = v_{rms, \text{CH}_4} \] This gives us: \[ \sqrt{\frac{3RT_{He}}{M_{He}}} = \sqrt{\frac{3RT_{CH_4}}{M_{CH_4}}} \] 3. **Substitute known values**: - The molar mass of helium (\( M_{He} \)) is approximately 4 g/mol. - The molar mass of methane (\( M_{CH_4} \)) is approximately 16 g/mol. - The temperature for methane is given as 327°C, which we need to convert to Kelvin: \[ T_{CH_4} = 327 + 273 = 600 \, K \] 4. **Rewrite the equation**: Substituting the values into the equation, we have: \[ \sqrt{\frac{3RT_{He}}{4}} = \sqrt{\frac{3R \cdot 600}{16}} \] 5. **Square both sides to eliminate the square root**: \[ \frac{3RT_{He}}{4} = \frac{3R \cdot 600}{16} \] 6. **Cancel \( 3R \) from both sides**: \[ \frac{T_{He}}{4} = \frac{600}{16} \] 7. **Solve for \( T_{He} \)**: \[ T_{He} = 4 \cdot \frac{600}{16} \] Simplifying this: \[ T_{He} = 4 \cdot 37.5 = 150 \, K \] 8. **Convert Kelvin to Celsius** (if needed): Since the question asks for the temperature in Celsius, we convert: \[ T_{He} = 150 - 273 = -123 \, °C \] ### Final Answer: The temperature at which the root mean square velocity of helium gas becomes the same as that of methane at 327°C is **150 K** or **-123°C**.
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