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A monoatomic ideal gas, initially at tem...

A monoatomic ideal gas, initially at temperature `T_1,` is enclosed in a cylinder fitted with a friction less piston. The gas is allowed to expand adiabatically to a temperature `T_2` by releasing the piston suddenly. If `L_1 and L_2` are the length of the gas column before expansion respectively, then `(T_1)/(T_2)` is given by

A

`((L_1)/(L_2))^(2//3)`

B

`L_1/L_2`

C

`L_2/L_1`

D

`((L_2)/(L_1))^(2//3)`

Text Solution

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The correct Answer is:
To solve the problem, we need to find the ratio \( \frac{T_1}{T_2} \) for a monoatomic ideal gas that expands adiabatically. Here’s the step-by-step solution: ### Step 1: Understand the Adiabatic Process In an adiabatic process, the relationship between temperature and volume for an ideal gas is given by the equation: \[ T V^{\gamma - 1} = \text{constant} \] where \( \gamma \) is the adiabatic index. ### Step 2: Determine the Value of \( \gamma \) For a monoatomic ideal gas, the degree of freedom \( f \) is 3. The adiabatic index \( \gamma \) is given by: \[ \gamma = \frac{f + 2}{f} = \frac{3 + 2}{3} = \frac{5}{3} \] ### Step 3: Express Initial and Final States Let: - \( T_1 \) = initial temperature - \( T_2 \) = final temperature - \( L_1 \) = initial length of the gas column (related to initial volume) - \( L_2 \) = final length of the gas column (related to final volume) The volumes can be expressed in terms of the lengths: \[ V_1 \propto L_1 \quad \text{and} \quad V_2 \propto L_2 \] ### Step 4: Apply the Adiabatic Condition Using the adiabatic condition for the initial and final states: \[ T_1 V_1^{\gamma - 1} = T_2 V_2^{\gamma - 1} \] Substituting the expressions for volume: \[ T_1 (L_1)^{\gamma - 1} = T_2 (L_2)^{\gamma - 1} \] ### Step 5: Substitute \( \gamma \) Value Substituting \( \gamma = \frac{5}{3} \): \[ T_1 (L_1)^{\frac{5}{3} - 1} = T_2 (L_2)^{\frac{5}{3} - 1} \] This simplifies to: \[ T_1 (L_1)^{\frac{2}{3}} = T_2 (L_2)^{\frac{2}{3}} \] ### Step 6: Rearranging to Find the Ratio Rearranging the equation to find \( \frac{T_1}{T_2} \): \[ \frac{T_1}{T_2} = \frac{(L_2)^{\frac{2}{3}}}{(L_1)^{\frac{2}{3}}} \] This can be rewritten as: \[ \frac{T_1}{T_2} = \left(\frac{L_2}{L_1}\right)^{\frac{2}{3}} \] ### Final Answer Thus, the ratio \( \frac{T_1}{T_2} \) is: \[ \frac{T_1}{T_2} = \left(\frac{L_2}{L_1}\right)^{\frac{2}{3}} \] ---

To solve the problem, we need to find the ratio \( \frac{T_1}{T_2} \) for a monoatomic ideal gas that expands adiabatically. Here’s the step-by-step solution: ### Step 1: Understand the Adiabatic Process In an adiabatic process, the relationship between temperature and volume for an ideal gas is given by the equation: \[ T V^{\gamma - 1} = \text{constant} \] where \( \gamma \) is the adiabatic index. ...
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VMC MODULES ENGLISH-GASEOUS STATE & THERMODYNAMICS-JEE ADVANCED (ARCHIVE )
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