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QJEEM24Ph4a0f: JEE Main 2024 Physics - Class 11 JEEM24Ph4a0f Solution: A sample of 1 mole gas at temperature is adiabatically expanded …

A sample of 1 mole gas at temperature TT is adiabatically expanded to double its volume. If adiab constant for the gas is γ=32\gamma=\frac{3}{2} , then the work done by the gas in the process is :

Multiple Choice Options

  • A RT[2+2]\mathrm{R} \mathrm{T}[2+\sqrt{2}]
  • B RT[2−2]\mathrm{RT}[2-\sqrt{2}]
  • C RT[2−2]\frac{\mathrm{R}}{\mathrm{T}}[2-\sqrt{2}]
  • D TR[2+2]\frac{T}{R}[2+\sqrt{2}]

Step-by-Step Verified Solution

For an adiabatic process, the work done by the gas can be found using the formula:

W=P1V1−P2V2γ−1W = \frac{P_1 V_1 - P_2 V_2}{\gamma - 1}

Given that the volume is doubled ( V2=2V1V_2 = 2V_1 ) and the adiabatic constant γ=32\gamma = \frac{3}{2} , we can manipulate the ideal gas law and the adiabatic process relationship to find an expression for work done in terms of the initial conditions and γ\gamma .

Recall, for an adiabatic process, PVγ=constantPV^{\gamma} = \text{constant} , so we can write:

P1V1γ=P2V2γP_1V_1^{\gamma} = P_2V_2^{\gamma}

Using the fact that V2=2V1V_2 = 2V_1 , we can express P2P_2 in terms of P1P_1 and V1V_1 as follows:

P1V1γ=P2(2V1)γP_1V_1^{\gamma} = P_2(2V_1)^{\gamma}

P2=P1(V12V1)γP_2 = P_1 \left( \frac{V_1}{2V_1} \right)^{\gamma}

P2=P1(12)γP_2 = P_1 \left( \frac{1}{2} \right)^{\gamma}

The work done then becomes:

W=P1V1−P1(12)γ⋅2V1γ−1W = \frac{P_1 V_1 - P_1 \left( \frac{1}{2} \right)^{\gamma} \cdot 2V_1}{\gamma - 1}

W=P1V11−(12)γ⋅2γ−1W = P_1V_1 \frac{1 - \left( \frac{1}{2} \right)^{\gamma} \cdot 2}{\gamma - 1}

Plugging in γ=32\gamma = \frac{3}{2} , we get:

W=P1V11−(12)32⋅232−1W = P_1V_1 \frac{1 - \left( \frac{1}{2} \right)^{\frac{3}{2}} \cdot 2}{\frac{3}{2} - 1}

W=P1V11−12⋅212W = P_1V_1 \frac{1 - \sqrt{\frac{1}{2}} \cdot 2}{\frac{1}{2}}

W=2P1V1(1−12)W = 2P_1V_1 (1 - \sqrt{\frac{1}{2}})

Since P1V1=nRTP_1V_1 = nRT for 1 mole ( n=1n = 1 ) of gas at temperature TT , we can further simplify:

W=2RT(1−12)W = 2RT(1 - \sqrt{\frac{1}{2}})

W=2RT(1−12)W = 2RT(1 - \frac{1}{\sqrt{2}})

W=RT(2−2)W = RT(2 - \sqrt{2})

Therefore, the correct option is:

Option B RT[2−2]\mathrm{RT}[2-\sqrt{2}] .

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