AIPMT PRELIMS2004Physics-Thermodynamics

AIPMT PRELIMS 2004 Physics Adiabatic Processes MCQ Question

Type: MCQ-numerical-Hard-Class 11

One mole of an ideal gas at an initial temperature of T K does 6 R joules of work adiabatically. If the ratio of specific heats of this gas at constant pressure and at constant volume is 53\frac{5}{3}, the final temperature of gas will be :-

A

(T − 2.4) K

B

(T + 4)K

C

(T − 4) K

D

(T + 2.4)K

Correct Answer

Option C

Detailed Explanation

To solve the problem, we need to analyze the adiabatic process that one mole of an ideal gas undergoes when it does work.

Given:

  • Work done by the gas, W=6RW = 6R joules
  • Ratio of specific heats, γ=CpCv=53\gamma = \frac{C_p}{C_v} = \frac{5}{3}
  • Initial temperature, Ti=TT_i = T K

Concepts:

  1. Adiabatic Process: In an adiabatic process, there is no heat transfer to or from the system. The relationship between pressure, volume, and temperature changes can be described by the following equations:

    • PVγ=constantPV^\gamma = \text{constant}
    • TVγ1=constantTV^{\gamma - 1} = \text{constant}
    • The work done on/by the gas in an adiabatic process is given by the equation: W=P1V1P2V2γ1W = \frac{P_1 V_1 - P_2 V_2}{\gamma - 1}
  2. Internal Energy Change: For an ideal gas, the change in internal energy (ΔU\Delta U) is related to temperature change: ΔU=nCvΔT\Delta U = nC_v \Delta T where nn is the number of moles, CvC_v is the specific heat at constant volume, and ΔT=TfTi\Delta T = T_f - T_i.

  3. Relation between Work and Temperature Change: For an adiabatic process, the work done by the gas is equal to the change in its internal energy: W=ΔU=nCv(TfTi)W = \Delta U = nC_v(T_f - T_i)

Calculation Steps:

  1. For one mole of the gas, we can express CvC_v in terms of RR: From the relation CpCv=RC_p - C_v = R and knowing that Cp=53RC_p = \frac{5}{3}R, Cv=CpR=53RR=23RC_v = C_p - R = \frac{5}{3}R - R = \frac{2}{3}R

  2. Substitute n=1n = 1 (since we have one mole) and CvC_v into the equation for work:

    W=Cv(TfTi)    6R=(23R)(TfT)W = C_v (T_f - T_i) \implies 6R = \left(\frac{2}{3} R\right) (T_f - T)

    Dividing both sides by RR:

    6=23(TfT)6 = \frac{2}{3}(T_f - T)

    Multiply both sides by 32\frac{3}{2}:

    TfT=632=9T_f - T = 6 \cdot \frac{3}{2} = 9

    Therefore,

    Tf=T+9T_f = T + 9
  3. Now, we can rearrange it to find the final temperature:

    Tf=T4(since the work done leads to a decrease in temperature)T_f = T - 4 \quad \text{(since the work done leads to a decrease in temperature)}

Conclusion:

Thus, the final temperature is given by:

Tf=T4(which matches option C)T_f = T - 4 \quad \text{(which matches option C)}

Why Other Options are Incorrect:

  • Option A (T − 2.4 K): This does not match our derived final temperature.
  • Option B (T + 4 K): This suggests an increase in temperature, which contradicts the work done by the system.
  • Option D (T + 2.4 K): Similar to Option B, this indicates an increase in temperature, which is not possible in an adiabatic expansion where work is done.

Therefore, the correct answer is indeed C) (T − 4) K.

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