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A monatomic gas is expanded adiabaticall...

A monatomic gas is expanded adiabatically and due to expansion volume becomes 8 times, then

A

a.Pressure becomes `(1)/(32)` times

B

b.Total K.E. of gas molecules becomes `(1)/(4)` times

C

c.Ratio of translational and roational kinetic energy changes with variation in temperature

D

d.None of These

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To solve the problem step by step, we need to analyze the adiabatic expansion of a monatomic gas where the volume becomes 8 times its initial value. We will use the principles of thermodynamics, particularly the equations governing adiabatic processes. ### Step 1: Understand the adiabatic process In an adiabatic process, there is no heat exchange with the surroundings. For a monatomic ideal gas, the relationship between pressure (P), volume (V), and temperature (T) is given by: \[ PV^\gamma = \text{constant} \] where \(\gamma\) (gamma) for a monatomic gas is \(\frac{5}{3}\). ### Step 2: Set up the initial and final states Let: - Initial pressure = \(P_1\) - Initial volume = \(V_1\) - Final pressure = \(P_2\) - Final volume = \(V_2 = 8V_1\) Using the adiabatic condition: \[ P_1 V_1^\gamma = P_2 V_2^\gamma \] ### Step 3: Substitute the final volume Substituting \(V_2 = 8V_1\) into the equation: \[ P_1 V_1^{\frac{5}{3}} = P_2 (8V_1)^{\frac{5}{3}} \] ### Step 4: Simplify the equation This simplifies to: \[ P_1 V_1^{\frac{5}{3}} = P_2 \cdot 8^{\frac{5}{3}} V_1^{\frac{5}{3}} \] Cancelling \(V_1^{\frac{5}{3}}\) from both sides gives: \[ P_1 = P_2 \cdot 8^{\frac{5}{3}} \] ### Step 5: Calculate \(8^{\frac{5}{3}}\) Calculating \(8^{\frac{5}{3}}\): \[ 8^{\frac{5}{3}} = (2^3)^{\frac{5}{3}} = 2^5 = 32 \] ### Step 6: Relate the pressures Thus, we have: \[ P_1 = 32 P_2 \] Rearranging gives: \[ P_2 = \frac{P_1}{32} \] ### Step 7: Analyze the kinetic energy The total kinetic energy of the gas is related to its temperature. The kinetic energy of a monatomic ideal gas is given by: \[ KE = \frac{3}{2} nRT \] Since \(PV = nRT\), we can express temperature in terms of pressure and volume: \[ T = \frac{PV}{nR} \] ### Step 8: Find the temperature ratio Using the initial and final states: \[ \frac{T_2}{T_1} = \frac{P_2 V_2}{P_1 V_1} \] Substituting \(P_2 = \frac{P_1}{32}\) and \(V_2 = 8V_1\): \[ \frac{T_2}{T_1} = \frac{\left(\frac{P_1}{32}\right)(8V_1)}{P_1 V_1} = \frac{8}{32} = \frac{1}{4} \] ### Step 9: Relate kinetic energy to temperature Since kinetic energy is proportional to temperature: \[ KE_2 = \frac{3}{2} nR T_2 = \frac{3}{2} nR \left(\frac{1}{4} T_1\right) = \frac{1}{4} KE_1 \] ### Conclusion From the analysis: - The final pressure \(P_2\) is \(\frac{P_1}{32}\). - The total kinetic energy of the gas molecules becomes \(\frac{1}{4}\) of the initial kinetic energy. ### Final Answers 1. Pressure becomes \(\frac{1}{32}\) times the initial pressure. 2. Kinetic energy of the gas molecules becomes \(\frac{1}{4}\) times the initial kinetic energy. 3. The ratio of translational and rotational kinetic energy does not change with temperature.
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