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Gas at a pressure P(0) in contained as a...

Gas at a pressure `P_(0)` in contained as a vessel. If the masses of all the molecules are halved and their speeds are doubles. The resulting pressure P will be equal to

A

`4 P_(0)`

B

`2 P_(0)`

C

`P_(0)`

D

`P_(0)//2`

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The correct Answer is:
To solve the problem, we need to understand how pressure is related to the mass of gas molecules and their speeds. The pressure of a gas can be expressed using the kinetic theory of gases, which states: \[ P = \frac{1}{3} \frac{mN \bar{v}^2}{V} \] where: - \( P \) is the pressure, - \( m \) is the mass of a single molecule, - \( N \) is the number of molecules, - \( \bar{v} \) is the root mean square speed of the molecules, - \( V \) is the volume of the gas. ### Step-by-step Solution: 1. **Initial Pressure Calculation**: The initial pressure \( P_0 \) is given by: \[ P_0 = \frac{1}{3} \frac{m N v^2}{V} \] where \( m \) is the initial mass of the molecules, \( N \) is the number of molecules, \( v \) is the initial speed of the molecules, and \( V \) is the volume. 2. **Change in Mass and Speed**: According to the problem, the mass of the molecules is halved: \[ m' = \frac{m}{2} \] and the speed of the molecules is doubled: \[ v' = 2v \] 3. **New Pressure Calculation**: We now calculate the new pressure \( P \) with the modified mass and speed: \[ P = \frac{1}{3} \frac{m' N (v')^2}{V} \] Substituting the new values: \[ P = \frac{1}{3} \frac{\left(\frac{m}{2}\right) N (2v)^2}{V} \] Simplifying this: \[ P = \frac{1}{3} \frac{\left(\frac{m}{2}\right) N (4v^2)}{V} \] \[ P = \frac{1}{3} \frac{2m N v^2}{V} \] \[ P = 2 \left(\frac{1}{3} \frac{m N v^2}{V}\right) \] \[ P = 2 P_0 \] 4. **Final Result**: Therefore, the resulting pressure \( P \) is: \[ P = 2 P_0 \] ### Conclusion: The resulting pressure after halving the mass of the molecules and doubling their speeds is \( 2 P_0 \).

To solve the problem, we need to understand how pressure is related to the mass of gas molecules and their speeds. The pressure of a gas can be expressed using the kinetic theory of gases, which states: \[ P = \frac{1}{3} \frac{mN \bar{v}^2}{V} \] where: - \( P \) is the pressure, - \( m \) is the mass of a single molecule, - \( N \) is the number of molecules, ...
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