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Heat and Thermodynamics question

2008 · Shift 1 · Q51
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Heat and Thermodynamics question

2008 · Shift 1 · Q51

JEE AdvancedPhysicsHeat and ThermodynamicsMCQ+3 / −1
An ideal gas is expanding such that PT 2^22 = constant. The coefficient of volume expansion of the gas is
  1. A
    1T\frac{1}{\mathrm{T}}T1​
  2. B
    2T\frac{2}{\mathrm{T}}T2​
  3. C
    3T\frac{3}{\mathrm{T}}T3​
  4. D
    4T\frac{4}{\mathrm{T}}T4​
View written solutionFree

Correct answer: C

Step-by-step Solution:

  1. Understand the Goal: We need to find the coefficient of volume expansion (gamma\\gammagamma) for an ideal gas undergoing a specific process described by the equation PT2=textconstantPT^2 = \\text{constant}PT2=textconstant.

  2. Definition of Coefficient of Volume Expansion: The coefficient of volume expansion for a specific process is defined as the fractional change in volume per unit change in temperature. Mathematically, it is expressed as: γ=1VdVdT\gamma = \frac{1}{V} \frac{dV}{dT}γ=V1​dTdV​ While the standard definition is for an isobaric (constant pressure) process, when a specific process is given, we calculate this value for that process.

  3. Use the Ideal Gas Law: For an ideal gas, the equation of state is: PV=nRTPV = nRTPV=nRT where PPP is pressure, VVV is volume, TTT is temperature, nnn is the number of moles, and RRR is the universal gas constant. We can express the pressure PPP from this equation as: P=nRTVP = \frac{nRT}{V}P=VnRT​

  4. Combine the Process Equation and the Ideal Gas Law: The given process is PT2=KPT^2 = KPT2=K, where KKK is a constant. Substitute the expression for PPP from the ideal gas law into this process equation to establish a relationship between volume VVV and temperature TTT: (nRTV)T2=K\left( \frac{nRT}{V} \right) T^2 = K(VnRT​)T2=K nRT3V=K\frac{nRT^3}{V} = KVnRT3​=K

  5. Express Volume as a Function of Temperature: Rearrange the equation from the previous step to solve for VVV: V=(nRK)T3V = \left( \frac{nR}{K} \right) T^3V=(KnR​)T3 Since nnn, RRR, and KKK are all constants, we can let C=nRKC = \frac{nR}{K}C=KnR​. The relationship simplifies to: V=CT3V = CT^3V=CT3 This shows that for this particular process, the volume of the gas is proportional to the cube of its absolute temperature.

  6. Calculate the Derivative dVdT\frac{dV}{dT}dTdV​: Differentiate the expression for VVV with respect to TTT: dVdT=ddT(CT3)=C⋅(3T2)=3CT2\frac{dV}{dT} = \frac{d}{dT}(CT^3) = C \cdot (3T^2) = 3CT^2dTdV​=dTd​(CT3)=C⋅(3T2)=3CT2

  7. Calculate the Coefficient of Volume Expansion: Now, substitute the expressions for VVV and dVdT\frac{dV}{dT}dTdV​ into the formula for gamma\\gammagamma: γ=1VdVdT=1CT3(3CT2)\gamma = \frac{1}{V} \frac{dV}{dT} = \frac{1}{CT^3} (3CT^2)γ=V1​dTdV​=CT31​(3CT2) The constant CCC and the term T2T^2T2 cancel out: γ=3T\gamma = \frac{3}{T}γ=T3​

  8. Conclusion: The coefficient of volume expansion for the gas undergoing the process PT2=textconstantPT^2 = \\text{constant}PT2=textconstant is 3T\frac{3}{T}T3​. This matches option C.

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