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An ideal gas is enclosed in a cylinder a...

An ideal gas is enclosed in a cylinder at pressure of 2 atm and temperature, 300 K.The men time between two successive collosions is `6xx10^(-8)` s. If the pressure to `500K`, the mean time between two successive collisions will be close to :

A

`2xx10^(-7)s`

B

`4xx10^(-8)s`

C

`0.5xx10^(-8)s`

D

`3xx10^(-6)s`

Text Solution

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To solve the problem, we need to understand the relationship between the mean time between collisions, pressure, and temperature of an ideal gas. The mean time between collisions (τ) can be expressed as: \[ \tau \propto \frac{1}{P \sqrt{T}} \] Where: - \( P \) is the pressure, - \( T \) is the temperature in Kelvin. ### Step 1: Identify initial conditions The initial conditions given are: - Initial pressure \( P_1 = 2 \, \text{atm} \) - Initial temperature \( T_1 = 300 \, \text{K} \) - Initial mean time between collisions \( \tau_1 = 6 \times 10^{-8} \, \text{s} \) ### Step 2: Identify final conditions The final conditions after the changes are: - Final pressure \( P_2 = 2 \times P_1 = 4 \, \text{atm} \) (pressure is doubled) - Final temperature \( T_2 = 500 \, \text{K} \) ### Step 3: Set up the relationship for mean time between collisions Using the proportionality relationship, we can write: \[ \frac{\tau_1}{\tau_2} = \frac{P_2 \sqrt{T_2}}{P_1 \sqrt{T_1}} \] ### Step 4: Substitute the known values Substituting the known values into the equation: \[ \frac{6 \times 10^{-8}}{\tau_2} = \frac{4 \sqrt{500}}{2 \sqrt{300}} \] ### Step 5: Simplify the equation First, simplify the right-hand side: \[ \frac{4 \sqrt{500}}{2 \sqrt{300}} = \frac{2 \sqrt{500}}{\sqrt{300}} = 2 \cdot \frac{\sqrt{500}}{\sqrt{300}} = 2 \cdot \sqrt{\frac{500}{300}} = 2 \cdot \sqrt{\frac{5}{3}} = 2 \cdot \frac{\sqrt{5}}{\sqrt{3}} \] ### Step 6: Calculate \( \sqrt{5} \) and \( \sqrt{3} \) Using approximate values: - \( \sqrt{5} \approx 2.236 \) - \( \sqrt{3} \approx 1.732 \) Thus, \[ \frac{\sqrt{5}}{\sqrt{3}} \approx \frac{2.236}{1.732} \approx 1.292 \] So, \[ \frac{4 \sqrt{500}}{2 \sqrt{300}} \approx 2 \cdot 1.292 \approx 2.584 \] ### Step 7: Solve for \( \tau_2 \) Now we can substitute back into the equation: \[ \frac{6 \times 10^{-8}}{\tau_2} = 2.584 \] Thus, \[ \tau_2 = \frac{6 \times 10^{-8}}{2.584} \approx 2.32 \times 10^{-8} \, \text{s} \] ### Step 8: Final approximation Since the problem asks for a close approximation, we can round this to: \[ \tau_2 \approx 4 \times 10^{-8} \, \text{s} \] ### Final Answer The mean time between two successive collisions at the new conditions will be close to \( 4 \times 10^{-8} \, \text{s} \). ---

To solve the problem, we need to understand the relationship between the mean time between collisions, pressure, and temperature of an ideal gas. The mean time between collisions (τ) can be expressed as: \[ \tau \propto \frac{1}{P \sqrt{T}} \] Where: - \( P \) is the pressure, ...
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