Sign in
12thPass logo
New chatPYQ LibraryDoubtsRank report
Sign in to see Recents

Your guest activity stays on this device

Sign in to save progress →
Sign in

Heat and Thermodynamics question

2024 · 5 Apr · Shift 2 · Q65
Guest · filters and generic practice availableBrowsing as a guest · PYQ filters and generic practice are available. Sign in only for personalised features and saved progress.
  1. PYQ Library
  2. /JEE Main
  3. /Physics
  4. /Heat and Thermodynamics
  5. /2024 · 5 Apr · Shift 2 · Q65

Heat and Thermodynamics question

2024 · 5 Apr · Shift 2 · Q65

JEE MainPhysicsHeat and ThermodynamicsMCQ+4 / −1
During an adiabatic process, if the pressure of a gas is found to be proportional to the cube of its absolute temperature, then the ratio of CPCV\frac{\mathrm{C}_{\mathrm{P}}}{\mathrm{C}_{\mathrm{V}}}CV​CP​​ for the gas is :
  1. A
    53\frac{5}{3}35​
  2. B
    32\frac{3}{2}23​
  3. C
    75\frac{7}{5}57​
  4. D
    97\frac{9}{7}79​
View written solutionFree

Correct answer: B

  1. Use the adiabatic relation

For an ideal gas undergoing an adiabatic process, PVγ=constantPV^{\gamma}=\text{constant}PVγ=constant where γ=CPCV.\gamma=\frac{C_P}{C_V}.γ=CV​CP​​.

Also, from the ideal gas equation, PV=nRT⇒P=nRTV.PV=nRT \quad \Rightarrow \quad P=\frac{nRT}{V}. PV=nRT⇒P=VnRT​.

  1. Express PPP in terms of TTT during the adiabatic process

From PVγ=K,PV^{\gamma}=K,PVγ=K, we get P=KVγ.P=\frac{K}{V^{\gamma}}.P=VγK​.

Using the ideal gas law, T∝PV.T \propto PV.T∝PV. Substitute P∝V−γP \propto V^{-\gamma}P∝V−γ: T∝V−γ⋅V=V1−γ.T \propto V^{-\gamma} \cdot V = V^{1-\gamma}.T∝V−γ⋅V=V1−γ.

So, V∝T11−γ.V \propto T^{\frac{1}{1-\gamma}}.V∝T1−γ1​.

Now,

= T^{-\frac{\gamma}{1-\gamma}} = T^{\frac{\gamma}{\gamma-1}}.$$ Hence, for an adiabatic process, $$P \propto T^{\frac{\gamma}{\gamma-1}}.$$ 3. **Compare with the given condition** It is given that $$P \propto T^3.$$ Therefore, $$\frac{\gamma}{\gamma-1}=3.$$ 4. **Solve for $\gamma$** $$\gamma = 3(\gamma-1)$$ $$\gamma = 3\gamma - 3$$ $$2\gamma = 3$$ $$\gamma = \frac{3}{2}.$$ Thus, $$\frac{C_P}{C_V}=\frac{3}{2}.$$ 5. **Check options** - A: $\frac{5}{3}$ ❌ - B: $\frac{3}{2}$ ✅ - C: $\frac{7}{5}$ ❌ - D: $\frac{9}{7}$ ❌ So the correct option is **B**.
PreviousNext

More from Heat and Thermodynamics

  • If n is the number density and d is the diameter of the molecule, then the average distance covered by a molecule between two successive collisions (i.e. mean free path) is represented by :2024 · MCQ
  • The specific heat at constant pressure of a real gas obeying PV2=RT equation is:2024 · MCQ
  • A sample contains mixture of helium and oxygen gas. The ratio of root mean square speed of helium and oxygen in the sample, is :2024 · MCQ
  • Given below are two statements: Statement (I) : Dimensions of specific heat is [L2 T−2 K−1]. Statement (II) : Dimensions of gas constant is [ML2 T−1 K−1]…2024 · MCQ
  • Energy of 10 non rigid diatomic molecules at temperature T is :2024 · MCQ
  • A total of 48 J heat is given to one mole of helium kept in a cylinder. The temperature of helium increases by 2∘C. The work done by the gas is: Given, R=8.3 J K−1 mol−1…2024 · MCQ
  • A mixture of one mole of monoatomic gas and one mole of a diatomic gas (rigid) are kept at room temperature (27∘C). The ratio of specific heat of gases at constant volume respectively is:2024 · MCQ
  • Two different adiabatic paths for the same gas intersect two isothermal curves as shown in P-V diagram. The relation between the ratio Vd​Va​​ and the ratio Vc​Vb​​ is: Includes diagram2024 · MCQ