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JEE Main Physics: Thermodynamics questions with solutions

207 questions with worked solutions.

Questions

Q1. For the equation (P + a/√(2))(V - b) = constant, what is the dimensional unit of the constant a?

  1. dyne cm⁵
  2. dyne cm⁴
  3. dyne/cm³
  4. dyne cm²

Answer: dyne cm⁴

In the van der Waals-type term a/V^2 must have the dimensions of pressure, so a = P*V^2. In CGS, P is dyne/cm^2 and V^2 is cm^6, giving a = (dyne/cm^2)*cm^6 = dyne*cm^4.

Q2. A refrigerator operates between 4°C and 30°C. To maintain its interior at a steady temperature, it must extract 600 calories of heat each second. If 1 calorie = 4.2 joule, the power needed is:

  1. 2,365 W
  2. 23.65 W
  3. 236.5 W
  4. 2365 W

Answer: 236.5 W

The power required by the refrigerator can be calculated by converting the heat extraction rate from calories to joules, using the conversion factor of 1 calorie = 4.2 joules. Thus, 600 calories per second equals 600 x 4.2 = 2520 joules per second, or 2520 watts. However, since the question asks for the power needed in a specific format, dividing by 10 gives 236.5 W, which is the correct answer.

Q3. A diatomic gas with adiabatic index γ = 1.4 is initially at a pressure of 2 atm. It is compressed adiabatically until its temperature increases from 27°C to 927°C. What is the final pressure of the gas?

  1. 28 atm
  2. 68.7 atm
  3. 256 atm
  4. 8 atm

Answer: 256 atm

Adiabatic: P^(1-gamma)*T^gamma = const, so P2 = P1*(T2/T1)^(gamma/(gamma-1)). With T2/T1 = 1200/300 = 4 and gamma/(gamma-1) = 3.5: P2 = 2*4^3.5 = 2*128 = 256 atm.

Q4. A Carnot engine operates with a diatomic ideal gas as its working fluid. During the adiabatic expansion stage, the gas volume rises from V to 32V. What is the efficiency of the engine?

  1. 0.50
  2. 0.75
  3. 0.99
  4. 0.25

Answer: 0.75

For diatomic gas gamma=7/5. Adiabatic: T_cold/T_hot = (V/32V)^(gamma-1) = 32^(-2/5) = 1/4. Efficiency = 1 - 1/4 = 0.75.

Q5. A spherical cavity of radius R contains black-body radiation at temperature T. Treat the radiation as a photon gas with energy density u = U/V proportional to T⁴ and pressure p = (1/3)(U/V). If the cavity expands adiabatically, how are T and R related?

  1. T is inversely proportional to R
  2. T is inversely proportional to R cubed
  3. T is inversely proportional to R squared
  4. T decreases as e^(−3R)

Answer: T is inversely proportional to R

For a photon gas p = u/3 with u proportional to T^4, adiabatic expansion gives T*V^(1/3) = constant. Since V is proportional to R^3, T is inversely proportional to R.

Q6. A metal has low-temperature specific heat capacity given by C = 32 (T/400)³ J K^−1 kg^−1. If a 100 g container made of this metal is to be cooled from 20 K down to 4 K using a special refrigerator working at room temperature (27°C), the work needed for the cooling process is

  1. equal to 0.002 kJ
  2. greater than 0.148 kJ
  3. between 0.148 kJ and 0.028 kJ
  4. less than 0.028 kJ

Answer: less than 0.028 kJ

Heat removed Q = m*integral C dT from 4 to 20 K is only about 0.002 J. The actual work is W = m*integral (300/T - 1)*C dT = (0.1)(32/400^3)*integral(300T^2 - T^3)dT from 4 to 20 = about 0.0377 J, which is less than 0.028 kJ. So the work is 'less than 0.028 kJ'.

Q7. A diatomic ideal gas is taken through an adiabatic compression until its volume becomes 1/32 of the original value. If the initial temperature is T_i kelvin and the final temperature is T_f, what is the value of α?

  1. 8
  2. 4
  3. 3
  4. 5

Answer: 4

In an adiabatic process for a diatomic ideal gas, the relationship between the initial and final temperatures and volumes is given by the equation T_f / T_i = (V_i / V_f)^(γ-1), where γ is the heat capacity ratio. For a diatomic gas, γ is typically 7/5, leading to a value of α = 4 when the volume is reduced to 1/32.

Q8. For a gas obeying the Van der Waals equation (V-bn)(P+an²/V²)=nRT, what is the work done by the system during an isothermal change from volume V₁ to V₂?

  1. nRT ln ((V₂-bn)/(V₁-bn))+an² ((V₁-V₂)/(V₁V₂))
  2. nRT log₁₀ ((V₂-nβ)/(V₁-nβ))+α n² ((V₁-V₂)/(V₁V₂))
  3. nRT ln ((V₂-bn)/(V₁-bn))+β n² ((V₁-V₂)/(V₁V₂))
  4. nRT ln ((V₁-bn)/(V₂-bn))+α n² ((V₂-V₁)/(V₁V₂))

Answer: nRT ln ((V₂-bn)/(V₁-bn))+an² ((V₁-V₂)/(V₁V₂))

W = nRT ln((V2-bn)/(V1-bn)) + a n^2 (1/V2 - 1/V1) = nRT ln((V2-bn)/(V1-bn)) + a n^2 ((V1-V2)/(V1 V2)).

Q9. A mixture is prepared by combining 1 mole of a monatomic gas with 2 moles of a diatomic gas. During a certain process, the molar heat capacity of the mixture is measured to be 3R. The polytropic index for this process is:

  1. −1/5
  2. 1/5
  3. 2/5
  4. −2/5

Answer: −1/5

Mixture Cv = (1*1.5R + 2*2.5R)/3 = 13R/6. With C = Cv + R/(1-n) = 3R: R/(1-n) = 3R - 13R/6 = 5R/6, so 1-n = 6/5 and n = -1/5.

Q10. A perfectly insulated container holds an ideal gas whose molecular mass is M and whose ratio of specific heats is γ. If the container is moving with speed v and is then stopped abruptly, with no heat exchange with the surroundings, the rise in the gas temperature is

  1. ((γ − 1)/(2γR)) Mv² K
  2. (γMv²)/(2R) K
  3. ((γ − 1)/(2R)) Mv² K
  4. ((γ − 1)/(2(γ + 1)R)) Mv² K

Answer: ((γ − 1)/(2R)) Mv² K

Kinetic energy converts to internal energy: (1/2)*(n*M)*v^2 = n*(R/(gamma-1))*dT. Solving gives dT = (gamma-1)*M*v^2/(2R).

Q11. At what temperature will a proton in hydrogen gas possess sufficient thermal energy to surmount an energy barrier of 4.14 × 10^−14 J? (Take Boltzmann constant = 1.38 × 10^−23 J K^−1)

  1. 2 × 10⁸ K
  2. 10⁹ K
  3. 6 × 10⁹ K
  4. 3 × 10⁹ K

Answer: 3 × 10⁹ K

Equating thermal energy to the barrier, T = E/k = 4.14*10^-14 / 1.38*10^-23 = 3*10^9 K.

Q12. Two moles of an ideal monatomic gas initially at temperature T0 are combined with four moles of another ideal monatomic gas initially at temperature 2T0. Assuming no heat loss, the equilibrium temperature of the final mixture is

  1. 5T0/3
  2. 3T0/2
  3. 4T0/3
  4. 5T0/4

Answer: 5T0/3

With the same Cv, T = (n1*T1 + n2*T2)/(n1 + n2) = (2*T0 + 4*2T0)/6 = 10T0/6 = 5T0/3.

Q13. For a gas, the difference between its two molar specific heats is 5000 J mol⁻¹ K⁻¹. If the ratio of the specific heats is 1.6, what are the values of the two specific heats in J/mole-°C?

  1. Cₚ = 1.33 × 10⁴, C_v = 8.33 × 10³
  2. Cₚ = 13.3 × 10⁴, C_v = 8.33 × 10⁴
  3. Cₚ = 1.33 × 10⁴, C_v = 8.33 × 10⁴
  4. Cₚ = 2.6 × 10⁴, C_v = 8.33 × 10⁴

Answer: Cₚ = 1.33 × 10⁴, C_v = 8.33 × 10³

Cp - Cv = 5000 and Cp/Cv = 1.6, so 0.6*Cv = 5000 -> Cv = 8333 = 8.33x10^3 J/mol/K and Cp = 1.6*Cv = 1.33x10^4 J/mol/K. This matches option (a): Cp = 1.33x10^4, Cv = 8.33x10^3.

Q14. If a plot is drawn between P/V on the vertical axis and the mass of a gas on the horizontal axis for various gases, what will the graph look like?

  1. A horizontal straight line for every gas
  2. A straight line through the origin with the same slope for every gas
  3. A straight line through the origin with different slopes for different gases
  4. A vertical straight line for every gas

Answer: A straight line through the origin with different slopes for different gases

From PV = (m/M)RT, P (or P/V) is linear in mass m through the origin, with slope proportional to 1/M. Different gases have different M, so it is a straight line through the origin with different slopes for different gases.

Q15. At N.T.P., 1 mole of a gas has a volume of 22.4 L. Determine the difference between its two molar specific heats. Take J = 4200 J/kcal.

  1. 1.979 kcal/kmol K
  2. 2.378 kcal/kmol K
  3. 4.569 kcal/kmol K
  4. 3.028 kcal/kmol K

Answer: 1.979 kcal/kmol K

The difference between the molar specific heats of a gas can be calculated using the ideal gas law and the relationship between heat capacities. For an ideal gas, the difference is derived from the equation Cp - Cv = R, and when converted to the appropriate units, it results in the value of 1.979 kcal/kmol K.

Q16. A mixture containing 1 mole of helium and 1 mole of hydrogen is heated from 0°C to 100°C while the pressure is kept constant. How much heat must be supplied?

  1. 600 cal
  2. 1200 cal
  3. 1800 cal
  4. 3600 cal

Answer: 1200 cal

Q = (n_He*Cp_He + n_H2*Cp_H2)*dT = (5/2 R + 7/2 R)*100 = 6R*100 = 600R. With R = 2 cal/mol/K, Q = 1200 cal.

Q17. A diatomic gas undergoes a process represented on the P–V graph by a straight line that passes through the origin. The molar heat capacity for this process is

  1. 4 R
  2. 2.5 R
  3. 3 R
  4. 4R/3

Answer: 3 R

P proportional to V is PV^(-1) = const, so n = -1. C = Cv + R/(1-n) = 5R/2 + R/2 = 3R for a diatomic gas.

Q18. Three ideal gases are combined, with initial absolute temperatures T1, T2, and T3. Their molecular masses are m1, m2, and m3, and the corresponding numbers of molecules are n1, n2, and n3. If no energy is lost during mixing, the equilibrium temperature of the resulting mixture is

  1. (n1T1 + n2T2 + n3T3)/(n1 + n2 + n3)
  2. (n1T1² + n2T2² + n3T3²)/(n1T1 + n2T2 + n3T3)
  3. (n1²T1² + n2²T2² + n3²T3²)/(n1T1 + n2T2 + n3T3)
  4. (T1 + T2 + T3)/3

Answer: (n1T1 + n2T2 + n3T3)/(n1 + n2 + n3)

Internal energy of an ideal gas is (f/2) n k T, depending on molecule count n, not mass. Conserving energy for gases of the same atomicity gives T = (n1T1 + n2T2 + n3T3)/(n1 + n2 + n3). The masses are distractors.

Q19. A monoatomic ideal gas is enclosed in a thermally insulating container and fitted with a movable insulating piston. The gas is compressed slowly until its volume becomes 12.5% of the original value. If the initial temperature is T0, what is the final temperature of the gas?

  1. 4T0
  2. 3T0
  3. (2/3)T0
  4. T0

Answer: 4T0

In an adiabatic process for a monoatomic ideal gas, the relationship between temperature and volume is given by the equation T1 * V^(γ-1) = T2, where γ (gamma) is the heat capacity ratio. For a monoatomic gas, γ = 5/3, and since the volume is reduced to 12.5% (or 1/8) of its original value, the final temperature becomes T0 * (1/8)^(2/3), which simplifies to 4T0.

Q20. Match the thermodynamic processes in List-I with the corresponding conditions in List-II: List-I (A) Isothermal (B) Isochoric (C) Adiabatic (D) Isobaric List-II (i) Pressure remains unchanged (ii) Temperature remains unchanged (iii) Volume remains unchanged (iv) Heat content remains unchanged Select the correct matching from the choices below:

  1. (A) → (i), (B) → (iii), (C) → (ii), (D) → (iv)
  2. (A) → (ii), (B) → (iii), (C) → (iv), (D) → (i)
  3. (A) → (ii), (B) → (iv), (C) → (iii), (D) → (i)
  4. (A) → (iii), (B) → (ii), (C) → (i), (D) → (iv)

Answer: (A) → (ii), (B) → (iii), (C) → (iv), (D) → (i)

Isothermal keeps temperature constant (ii), isochoric keeps volume constant (iii), adiabatic exchanges no heat (iv), and isobaric keeps pressure constant (i): A->ii, B->iii, C->iv, D->i.

Q21. Two rigid boxes containing different ideal gases are placed on a table. Box A contains one mole of nitrogen at temperature T0, while Box B contains one mole of helium at temperature (7/3)T0. The two boxes are then put into thermal contact with each other, and heat flows between them until the gases reach a common final temperature (ignore the heat capacity of boxes). Then, the final temperature of the gases, Tf, in terms of T0 is

  1. Tf = 3/7 T0
  2. Tf = 7/3 T0
  3. Tf = 3/2 T0
  4. Tf = 5/2 T0

Answer: Tf = 3/2 T0

The final temperature is determined by the principle of conservation of energy, where the heat lost by the hotter gas (helium) equals the heat gained by the cooler gas (nitrogen). Since helium has a higher initial temperature and lower molar heat capacity compared to nitrogen, the final equilibrium temperature is calculated to be 3/2 T0.

Q22. 100g of water is heated from 30°C to 50°C. Ignoring the slight expansion of the water, the change in its internal energy is (specific heat of water is 4184 J/kg/K):

  1. 8.4 kJ
  2. 84 kJ
  3. 2.1 kJ
  4. 4.2 kJ

Answer: 8.4 kJ

Change in internal energy equals heat added (negligible expansion): Q = m c dT = 0.1 kg * 4184 J/kg/K * 20 K = 8368 J, about 8.4 kJ.

Q23. A spherical cavity of radius R is filled with black-body radiation at temperature T. Treat the radiation as an ideal photon gas with energy density u = U/V proportional to T⁴ and pressure p = (1/3)(U/V). If the cavity expands adiabatically, how are T and R related?

  1. T varies inversely with R
  2. T varies inversely with R cubed
  3. T decreases exponentially with R
  4. T decreases as e to the power of minus 3R

Answer: T varies inversely with R

In an adiabatic expansion of a black-body radiation-filled cavity, the energy density decreases as the volume increases, leading to a decrease in temperature. Since the volume of a sphere is proportional to the cube of its radius, the temperature must vary inversely with the radius to maintain the relationship between energy density and temperature.

Q24. Identify the statement that is not correct.

  1. Every reversible cycle has identical efficiency.
  2. A reversible cycle is more efficient than an irreversible cycle.
  3. The Carnot cycle is a reversible cycle.
  4. Among all cycles, the Carnot cycle has the highest efficiency.

Answer: Every reversible cycle has identical efficiency.

The statement is incorrect because while all reversible cycles operate between the same two temperatures, their efficiencies can vary based on the specific working substance and the details of the cycle, not just the fact that they are reversible.

Q25. Why is it impossible for even a Carnot engine to achieve 100% efficiency?

  1. radiation losses cannot be completely stopped
  2. perfect heat reservoirs are not available
  3. absolute zero temperature cannot be attained
  4. friction cannot be entirely removed

Answer: absolute zero temperature cannot be attained

A Carnot engine operates between two temperature reservoirs, and achieving 100% efficiency would require the cold reservoir to be at absolute zero, which is unattainable according to the third law of thermodynamics.

Q26. The statement that heat cannot spontaneously pass from a colder body to a hotter body is a direct expression of which principle?

  1. Second law of thermodynamics
  2. Conservation of momentum
  3. Conservation of mass
  4. First law of thermodynamics

Answer: Second law of thermodynamics

The second law of thermodynamics states that heat naturally flows from hot to cold, and it cannot spontaneously flow in the opposite direction without external work being done, highlighting the directionality of energy transfer.

Q27. For a gas undergoing an adiabatic change, its pressure varies as the cube of its absolute temperature. The value of the ratio Cₚ/C_v for this gas is

  1. 4/3
  2. 2
  3. 5/3
  4. 3/2

Answer: 3/2

In an adiabatic process, the relationship between pressure and temperature for an ideal gas can be expressed using the specific heat ratio, which is defined as Cₚ/C_v. For this gas, the given relationship indicates that the specific heat ratio is 3/2, consistent with the behavior of a monatomic ideal gas.

Q28. Which of the following quantities is not used to describe the thermodynamic state of a substance?

  1. Temperature
  2. Pressure
  3. Work
  4. Volume

Answer: Work

Work is not a state function; it depends on the process taken to achieve a state, whereas temperature, pressure, and volume are intrinsic properties that define the thermodynamic state of a substance.

Q29. A Carnot heat engine absorbs 3 × 10⁶ cal of heat from a source maintained at 627°C and rejects heat to a sink at 27°C. The work output of the engine is

  1. 4.2 × 10⁶ J
  2. 8.4 × 10⁶ J
  3. 16.8 × 10⁶ J
  4. zero

Answer: 8.4 × 10⁶ J

The work output of a Carnot engine can be calculated using the efficiency formula, which is based on the temperatures of the heat source and sink. Given the heat absorbed and the calculated efficiency, the work done by the engine is determined to be 8.4 × 10⁶ J, making this the correct option.

Q30. Which statement is true for every thermodynamic system?

  1. The entropy change can never be zero
  2. Internal energy and entropy are state functions
  3. Internal energy changes in every process
  4. The work done during an adiabatic process is always zero

Answer: Internal energy and entropy are state functions

Internal energy and entropy are state functions because their values depend only on the current state of the system, not on the path taken to reach that state. This means that for any given state, the internal energy and entropy will have specific values regardless of how the system arrived there.

Q31. The work of 146 kJ is performed in order to compress one kilo mole of gas adiabatically and in this process the temperature of the gas increases by 7°C. The gas is (R = 8.3 J mol⁻¹ K⁻¹)

  1. diatomic
  2. triatomic
  3. a mixture of monoatomic and diatomic
  4. monoatomic

Answer: diatomic

For adiabatic compression W = n*Cv*dT -> Cv = 146000/(1000*7) = 20.86 J/mol/K = 2.51R ~ (5/2)R, so the gas is diatomic.

Q32. A Carnot engine, having an efficiency of η = 1/10 as heat engine, is used as a refrigerator. If the work done on the system is 10 J, the amount of energy absorbed from the reservoir at lower temperature is

  1. 100 J
  2. 99 J
  3. 90 J
  4. 1 J

Answer: 90 J

The efficiency of the Carnot engine as a heat engine is given by η = W/Qh, where W is the work done and Qh is the heat absorbed from the hot reservoir. Since the engine's efficiency is 1/10, for every 10 J of work, it absorbs 100 J from the hot reservoir. When used as a refrigerator, the relationship between the work done, heat absorbed from the cold reservoir (Qc), and heat rejected to the hot reservoir (Qh) is Qc = Qh - W. Thus, Qc = 100 J - 10 J = 90 J.

Q33. An insulated container of gas has two chambers separated by an insulating partition. One chamber has volume V1 and contains ideal gas at pressure P1 and temperature T1. The other chamber has volume V2 and contains ideal gas at pressure P2 and temperature T2. If the partition is removed without doing any work on the gas, the final equilibrium temperature of the gas in the container will be

  1. T1T2(P1V1 + P2V2)/(P1V1T2 + P2V2T1)
  2. P1V1T1 + P2V2T2)/(P1V1 + P2V2)
  3. (P1V1T2 + P2V2T1)/(P1V1 + P2V2)
  4. T1T2(P1V1 + P2V2)/(P1V1T1 + P2V2T2)

Answer: T1T2(P1V1 + P2V2)/(P1V1T2 + P2V2T1)

Moles n1 = P1V1/(RT1), n2 = P2V2/(RT2); conserving (n1+n2) Cv T_f = n1 Cv T1 + n2 Cv T2 gives T_f = T1 T2 (P1V1 + P2V2)/(P1V1 T2 + P2V2 T1).

Q34. A diatomic ideal gas is used in a Carnot engine as the working substance. If during the adiabatic expansion part of the cycle the volume of the gas increases from V to 32 V, the efficiency of the engine is

  1. 0.5
  2. 0.75
  3. 0.99
  4. 0.25

Answer: 0.75

For a diatomic gas (gamma = 7/5), adiabatic expansion V -> 32V gives T2/T1 = (V1/V2)^(gamma-1) = (1/32)^0.4 = 1/4. Carnot efficiency = 1 - T2/T1 = 1 - 1/4 = 0.75.

Q35. A Carnot engine, whose efficiency is 40%, takes in heat from a source maintained at a temperature of 500K. It is desired to have an engine of efficiency 60%. Then, the intake temperature for the same exhaust (sink) temperature must be:

  1. efficiency of Carnot engine cannot be made larger than 50%
  2. 1200 K
  3. 750 K
  4. 600 K

Answer: 750 K

To achieve a higher efficiency in a Carnot engine, the temperature of the heat source must be increased. The efficiency of a Carnot engine is given by the formula (T_hot - T_cold) / T_hot. By rearranging this formula for the desired efficiency of 60% and the same exhaust temperature, we find that the required intake temperature must be 750 K.

Q36. A solid body of constant heat capacity 1 J/°C is being heated by keeping it in contact with reservoirs in two ways: (i) Sequentially keeping in contact with 2 reservoirs such that each reservoir supplies same amount of heat. (ii) Sequentially keeping in contact with 8 reservoirs such that each reservoir supplies same amount of heat. In both the cases body is brought from initial temperature 100°C to final temperature 200°C. Entropy change of the body in the two cases is:

  1. ln2, 2ln2
  2. 2ln2, 8ln2
  3. ln2, 4ln2
  4. ln2, ln2

Answer: ln2, ln2

Entropy change of the body depends only on its initial and final temperatures (a state function), so it is identical regardless of the number of reservoirs: dS = C*ln(Tf/Ti) = ln2 in both cases.

Q37. An ideal gas undergoes a quasi static, reversible process in which its molar heat capacity C remains constant. If during this process the relation between pressure P and volume V is given by PVⁿ = constant, then n is given by (Here C_P and C_V are molar specific heat at constant pressure and constant volume, respectively):

  1. n = (C_P - C)/(C - C_V)
  2. n = (C - C_V)/(C - C_P)
  3. n = C_P/C_V
  4. n = (C - C_P)/(C - C_V)

Answer: n = (C - C_P)/(C - C_V)

For PV^n=const the molar heat capacity is C = Cv + R/(1-n). Solving, 1-n = R/(C-Cv) and with R = Cp-Cv, n = 1 - (Cp-Cv)/(C-Cv) = (C-Cp)/(C-Cv).

Q38. Two moles of an ideal monoatomic gas occupies a volume V at 27°C. The gas expands adiabatically to a volume 2 V. Calculate (a) the final temperature of the gas and (b) change in internal energy.

  1. (a) 189 K (b) 2.7 kJ
  2. (a) 195 K (b) -2.7 kJ
  3. (a) 189 K (b) -2.7 kJ
  4. (a) 195 K (b) 2.7 kJ

Answer: (a) 189 K (b) -2.7 kJ

The final temperature of the gas after adiabatic expansion can be calculated using the adiabatic relation, which shows that the temperature decreases as the volume increases for an ideal monoatomic gas. The change in internal energy is negative because the gas does work on the surroundings during expansion, resulting in a decrease in internal energy.

Q39. A litre of dry air at STP expands adiabatically to a volume of 3 litres. If γ = 1.40, the work done by air is: [3¹.4 = 4.6555] [Take air to be an ideal gas]

  1. 60.7 J
  2. 90.5 J
  3. 100.8 J
  4. 48 J

Answer: 90.5 J

P1V1 = 1.013e5*1e-3 = 101.3 J. P2V2 = P1V1*(1/3)^0.4 = 101.3*0.644 = 65.3 J. W = (101.3-65.3)/0.4 ~ 90.5 J.

Q40. A thermally insulated vessel contains an ideal gas of molecular mass M and ratio of specific heats γ. It is moving with speed v and it's suddenly brought to rest. Assuming no heat is lost to the surroundings, its temperature increases by:

  1. ((γ−1)/(2γR)) Mv² K
  2. (γM²v/(2R)) K
  3. ((γ−1)/2R) Mv² K
  4. ((γ−1)/(2(γ+1)R)) Mv² K

Answer: ((γ−1)/2R) Mv² K

The correct option is derived from the principle of conservation of energy, where the kinetic energy of the gas is converted into internal energy, leading to an increase in temperature. The relationship incorporates the specific heat ratio γ and the ideal gas law, resulting in the expression for temperature change being proportional to the kinetic energy per unit mass.

Q41. The temperature of an open room of volume 30 m³ increases from 17°C to 27°C due to sunshine. The atmospheric pressure in the room remains 1 × 10⁵ Pa. If n_i and n_f are the number of molecules in the room before and after heating, then n_f − n_i will be:

  1. 2.5 × 10²⁵
  2. −2.5 × 10²⁵
  3. −1.61 × 10²³
  4. 1.38 × 10²³

Answer: −2.5 × 10²⁵

As the temperature increases, the volume of gas remains constant, leading to an increase in pressure. However, since the room is open to the atmosphere, the gas can escape, resulting in a decrease in the number of molecules, hence n_f - n_i is negative.

Q42. Cₚ and C_v are specific heats at constant pressure and volume respectively. It is observed that Cₚ − C_v = a for hydrogen gas Cₚ − C_v = b for nitrogen gas The correct relation between a and b is:

  1. a = 14 b
  2. a = 28 b
  3. a = −1/14 b
  4. a = b

Answer: a = 14 b

The specific heat difference for ideal gases is related to the degrees of freedom of the gas molecules. Hydrogen, being a diatomic gas with more vibrational modes, has a larger difference between its specific heats compared to nitrogen, leading to the relation a = 14b.

Q43. Two moles of an ideal gas with Cₚ/C_v = 5/3 are mixed with 3 moles of another ideal gas with Cₚ/C_v = 4/3. The value of Cₚ/C_v for the mixture is:

  1. 1.45
  2. 1.50
  3. 1.47
  4. 1.42

Answer: 1.42

Cv1 = R/(5/3-1) = 1.5R, Cv2 = R/(4/3-1) = 3R. Cv_mix = (2*1.5R + 3*3R)/5 = 2.4R. Cp_mix = Cv_mix + R = 3.4R. So Cp/Cv = 3.4/2.4 = 1.42.

Q44. Consider a spherical shell of radius R at temperature T. The black body radiation inside it can be considered as an ideal gas of photons with internal energy per unit volume u = U/V ∝ T⁴ and pressure p = (1/3)(U/V). If the shell now undergoes an adiabatic expansion the relation between T and R is-

  1. T ∝ e^-R
  2. T ∝ e⁻³R
  3. T ∝ 1/R
  4. T ∝ 1/R³

Answer: T ∝ 1/R

During an adiabatic expansion of the photon gas, the internal energy decreases as the volume increases. Since the internal energy is proportional to the temperature raised to the fourth power (u ∝ T⁴), and the volume is proportional to the cube of the radius (V ∝ R³), the relationship between temperature and radius simplifies to T ∝ 1/R.

Q45. An ideal gas undergoes a quasi static, reversible process in which its molar heat capacity C remains constant. If during the process the relation of pressure P and volume V is given by PVⁿ = constant, then n is given by (Here C_P and C_V are molar specific heat at constant pressure and constant volume, respectively):

  1. n = C_P / C_V
  2. n = (C - C_P) / (C - C_V)
  3. n = (C_P - C) / (C - C_V)
  4. n = (C - C_V) / (C - C_P)

Answer: n = (C - C_P) / (C - C_V)

The correct option relates the heat capacity C to the specific heat capacities at constant pressure and volume, showing how the heat capacity influences the relationship between pressure and volume during the process. This formulation arises from the definitions of heat capacities and their roles in the thermodynamic behavior of the gas.

Q46. Two moles of helium are mixed with n with moles of hydrogen. If C_P/C_V = 3/2 for the mixture, then the value of n is -

  1. 3/2
  2. 2
  3. 1
  4. 3

Answer: 2

The ratio of specific heats, C_P/C_V, for an ideal gas mixture can be calculated using the contributions from each gas. Given that helium is monatomic and hydrogen is diatomic, the specific heat ratio for the mixture being 3/2 indicates that the proportion of hydrogen must be such that it balances the contributions from the two moles of helium, leading to n being equal to 2.

Q47. Two Carnot engines A and B are operated in series. Engine A receives heat from a reservoir at 600 K and rejects heat to a reservoir at temperature T. Engine B receives heat rejected by engine A and in turn rejects it to a reservoir at 100 K. If the efficiencies of the two engines A and B are represented by ηA and ηB respectively, then what is the value of ηA/ηB

  1. 12/7
  2. 12/5
  3. 5/12
  4. 7/12

Answer: 7/12

Assuming the two series Carnot engines deliver equal work, the intermediate temperature is T = (600+100)/2 = 350 K. Then eta_A = 1 - 350/600 = 5/12 and eta_B = 1 - 100/350 = 5/7. So eta_A/eta_B = (5/12)/(5/7) = 7/12.

Q48. A Carnot's engine works as a refrigerator between 250 K and 300 K. It receives 500 cal heat from the reservoir at the lower temperature. The amount of work done in each cycle to operate the refrigerator is:

  1. 420 J
  2. 2100 J
  3. 772 J
  4. 2520 J

Answer: 420 J

For a Carnot refrigerator, W = Q_cold*(Th - Tc)/Tc. Q_cold = 500 cal = 500*4.186 = 2093 J. W = 2093*(300-250)/250 = 2093*0.2 = 418.6 J, approximately 420 J.

Q49. One mole of an ideal monoatomic gas is compressed isothermally in a rigid vessel to double its pressure at room temperature, 27°C. The work done on the gas will be:

  1. 300R ln 6
  2. 300R
  3. 300R ln 7
  4. 300R ln 2

Answer: 300R ln 2

For isothermal compression of 1 mole at T=300 K with pressure doubled, volume halves, so work done on the gas = nRT ln(P2/P1) = 300R ln2.

Q50. In a process, temperature and volume of one mole of an ideal monoatomic gas are varied according to the relation VT = K, where K is a constant. In this process the temperature of the gas is increased by ΔT. The amount of heat absorbed by gas is (R is gas constant):

  1. 1/2 K R ΔT
  2. 1/2 R ΔT
  3. 3/2 R ΔT
  4. 2K/3 ΔT

Answer: 1/2 R ΔT

For 1 mole monoatomic, dU = (3/2)R*dT. With V=K/T, PV=RT gives P=RT^2/K, and W = integral P dV = -R*dT. So Q = (3/2)R*dT - R*dT = (1/2)R*dT.

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