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Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET PDF Download

Q1: Demonstrate that the internal energy U of the air in a room is independent of temperature provided the outside pressure p is constant. Calculate U, if p is equal to the normal atmospheric pressure and the room's volume is equal to V = 40 m3

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Internal energy of air, treating as an ideal gas

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET   (1)

Using  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Thus at constant pressure U = constant, because the volume of the room is a constant.

Putting the value of p = Patm and V in Eq. (1), we get U = 10 MJ.

Q2: A thermally insulated vessel containing a gas whose molar mass is equal to M and the ratio of specific heats Cp/Cv  = γ  moves with a velocity v. Find the gas temperature increment resulting from the sudden stoppage of the vessel. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: From energy conservation

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET       (1)

But from   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET (from the previous problem)     (2)

Hence from Eqs. (1) and (2).

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q3: Two thermally insulated vessels 1 and 2 are filled with air and connected by a short tube equipped with a valve. The volumes of the vessels, the pressures and temperatures of air in them are known (V1, p1, T1 and V2, p2, T2). Find the air temperature and pressure established after the opening of the valve. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: On opening the valve, the air will flow from the vessel at higher pressure to the vessel at lower pressure till both vessels have the same air pressure. If this air pressure is p, the total volume of the air in the two vessels will be (V1 + V2). Also if v1 and v2 be the number of moles of air initially in the two vessels, we have

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET    (1)

After the air is mixed up, the total number of moles are (v1 + v2) and the mixture is at temperature T.

Hence  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET     (2)

Let us look at the two portions of air as one single system. Since this system is contained in a thermally insulated vessel, no heat exchange is involved in the process. That is, total heat transfer for the combined system Q = 0

Moreover, this combined system does not perform mechanical work either. The walls of the containers are rigid and there are no pistons etc. to be pushed, looking at the total system, we know A = 0.

Hence, internal energy of the combined system docs not change in the process. Initially energy of the combined system is equal to the sum of internal energies of the two portions of air :

 Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET    (3)

Final internal energy of (n1 + n2) moles of air at temperature T is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET    (4)

Therefore, Ui = Uf implies :

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

From (2), therefore, final pressure is given by :

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

This process in an example of free adiabatic expansion of ideal gas.

Q4: Gaseous hydrogen contained initially under standard conditions in a sealed vessel of volume V = 5.0 l was cooled by ΔT = 55 K . Find how much the internal energy of the gas will change and what amount of heat will be lost by the gas.

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: By the first law of thermodynamics,

Q = ΔU + A

Here A = 0, as the volume remains constant,

So,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

From gas law,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence amount of heat lost  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q5: What amount of heat is to be transferred to nitrogen in the isobaric heating process for that gas to perform the work A = 2.0 J? 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: By the first law of thermodynamics  Q = ΔU + A

But   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q6: As a result of the isobaric heating by ΔT = 72 K one mole of a certain ideal gas obtains an amount of heat Q = 1.60 kJ. Find the work performed by the gas, the increment of its internal energy, and the value of γ = Cp/Cv.

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Under isobaric process Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

From the first law of thermodynamics 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Again increment in internal energy  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Thus  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q7: Two moles of a certain ideal gas at a temperature T0 = 300 K were cooled isochorically so that the gas pressure reduced n = 2.0 times. Then, as a result of the isobaric process, the gas expanded till its temperature got back to the initial value. Find the total amount of heat absorbed by the gas in this process. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Let v = 2 moles of the gas. In the first phase, under isochoric process, A1 = 0, therefore from gas law if pressure is reduced n times so that temperature i.e. new temperature becomes T0/n. 

Now from first law of thermodynamics

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

During the second phase (under isobaric process),

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Thus from first law of thermodynamics :

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence the total amount of heat absorbed

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q8: Calculate the value of γ = Cp/Cv  for a gaseous mixture consisting of v1  = 2.0 moles of oxygen and v2 = 3.0 moles of carbon dioxide. The gases are assumed to be ideal. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Total no. of moles of the mixture v = v1 + v2

At a certain temperature,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Thus   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Similarly   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Thus  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q9: Find the specific heat capacities cv and cp for a gaseous mixture consisting of 7.0 g of nitrogen and 20 g of argon. The gases are assumed to be ideal. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

and    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Now molar mass of the mixture  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q10: One mole of a certain ideal gas is contained under a weightless piston of a vertical cylinder at a temperature T. The space over the piston opens into the atmosphere. What work has to be performed in order to increase isothermally the gas volume under the piston it times by slowly raising the piston? The friction of the piston against the cylinder walls is negligibly small. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Let 5 be the area of the piston and F be the force exerted by the external agent Then, F + p S - p0S (Fig.) at an arbitrary instant of time. Here p is the pressure at the instant the volume is V. (Initially the pressure inside is p0)

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET
Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET
Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q11: A piston can freely move inside a horizontal cylinder closed from both ends. Initially, the piston separates the inside space of the cylinder into two equal parts each of volume V0, in which an ideal gas is contained under the same pressure P0  and at the same temperature. What work has to be performed in order to increase isothermally the volume of one part of gas η times compared to that of the other by slowly moving the piston? 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Let the agent move the piston to the right by x. In equilibrium position,

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Work done by the agent in an infinitesmal change dx is

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

By applying PV = constant, for the two parts,

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,      Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

When the volume of the left end is η times the volume of the right end

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q12: Three moles of an ideal gas being initially at a temperature T0 = 273 K were isothermally expanded n = 5.0 times its initial volume and then isochorically heated so that the pressure in the final state became equal to that in the initial state. The total amount of heat transferred to the gas during the process equals Q = 80 kJ. Find the ratio γ = Cp/Cv for this gas. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: In the isothermal process, heat transfer to the gas is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

In the isochoric process, A = 0

Thus heat transfer to the gas is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

But   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Thus, net heat transfer to the gas

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q13: Draw the approximate plots of isochoric, isobaric, isothermal, and adiabatic processes for the case of an ideal gas, using the following variables:

(a) p, T; (b) V, T. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: (a) From ideal gas law Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

For isochoric process, obviously k = constant, thus p = kT, represents a straight line passing through the origin and its slope becomes k.
For isobaric process p = constant, thus on p - T curve, it is a horizontal straight line parallel to T - axis, if T is along horizontal (or x - axis)

For isothermal process, T = constant, thus on p - T curve, it represents a vertical straight line if T is taken along horizontal (or x - axis)

For adiabatic process Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

After diffrentiating, we get Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

The approximate plots of isochoric, isobaric, isothermal, and adiabatic processes are drawn in the answer sheet.

(b) As p is not considered as variable, we have from ideal gas law

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

On V - T co-ordinate system let us, take T along x - axis.
For isochoric process V = constant, thus k' = constant and V = k'T obviously represents a straight line passing through the origin of the co-ordinate system and k' is its slope.
For isothermal process T = constant. Thus on the stated co- ordinate system it represents a straight line parallel to the V - axis.
For adiabatic process Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

After differentiating, we get Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

The approximate plots of isochoric, isobaric, isothermal and adiabatic processes are drawn in the answer sheet.

Q14: One mole of oxygen being initially at a temperature T0 = 290 K is adiabatically compressed to increase its pressure η = 10.0 times. Find:
 (a) the gas temperature after the compression;
 (b) the work that has been performed on the gas. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: According to T - p relation in adiabatic process, Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET (where k = constant)

and   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b) Using the solution of part (a), sought work done

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q15: A certain mass of nitrogen was compressed η = 5.0 times (in terms of volume), first adiabatically, and then isothermally. In both cases the initial state of the gas was the same. Find the ratio of the respective works expended in each compression.

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Let (p0, V0,T0) be the initial state of the gas.

We know  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

But from the equation  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Thus    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

On the other hand, we know  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET (work done by the gas)

Thus  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q16: A heat-conducting piston can freely move inside a closed thermally insulated cylinder with an ideal gas. In equilibrium the piston divides the cylinder into two equal parts, the gas temperature being equal to T0 . The piston is slowly displaced. Find the gas temperature as a function of the ratio η of the volumes of the greater and smaller sections. The adiabatic exponent of the gas is equal to γ.

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Since here the piston is conducting and it is moved slowly the temperature on the two sides increases and maintained at the same value.
Elementary work done by the agent = Work done in compression - Work done in expansion 

i.e. dA - p2 dV - p1 dV = (p2 - P1) dV

where p1 and p2 are pressures at any instant of the gas on expansion and compression side respectively.

From the gas law  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET for each section

(x is the displacement of the piston towards section 2)

So,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Also, from the first law of thermodynamics 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So, work done on the gas  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

On integrating 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q17: Find the rate v with which helium flows out of a thermally insulated vessel into vacuum through a small hole. The flow rate of the gas inside the vessel is assumed to be negligible under these conditions. The temperature of helium in the vessel is T = 1,000 K.

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: From energy conservation as in the derivation of Bernoulli theorem it reads

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET    (1)

In the Eq. (1) u is the internal energy per unit mass and in this case is the thermal eneigy per unit mass of the gas. As the gas vessel is thermally insulated Qd = 0, also in our case.

Just inside the vessel Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET Inside the vessel v = 0 also. Just outside p = 0, and u = 0. Ingeneral gz is not very significant for gases.

Thus applying Eq. (1) just inside and outside the hole, we get

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Note : The velocity here is the velocity of hydrodynamic flow of the gas into vacuum. This requires that the diameter of the hole is not too small (D > mean free path l). In the opposite case (D < < l) the flow is called effusion. Then the above result does not apply and kinetic theory methods are needed.

Q18: The volume of one mole of an ideal gas with the adiabatic exponent γ is varied according to the law V = a/T, where a is a constant. Find the amount of heat obtained by the gas in this process if the gas temperature increased by ΔT. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: The differential work done by the gas

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

From the Grst law of thermodynamics  

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q19: Demonstrate that the process in which the work performed by an ideal gas is proportional to the corresponding increment of its internal energy is described by the equation pVn = const, where n is a constant. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: According to the problem : A α U or dA = aU (where a is proportionality constant)

or,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET                             (1)

From ideal gas law, pV= v R T, on differentiating

p dV + V dp = v RdT                      (2)

Thus from (1) and (2) 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Dividing both the sides by pV

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

On integrating n In V + In p = In C (where C is constant) 

or, Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q20: Find the molar heat capacity of an ideal gas in a polytropic process pVn = const if the adiabatic exponent of the gas is equal to γ. At what values of the polytropic constant n will the heat capacity of the gas be negative? 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: In the polytropic process work done by the gas

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(where Ti and Tf are initial and final temperature of the gas like in adiabatic process)

and    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

By the first law of thermodynamics Q = ΔU + A 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

According to definition of molar heat capacity when number of moles v = 1 and ΔT = 1 then Q = Molar heat capacity.

Here,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q21: In a certain polytropic process the volume of argon was increased α = 4.0 times. Simultaneously, the pressure decreased β = 8.0 times. Find the molar heat capacity of argon in this process, assuming the gas to be ideal.

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Let the process be polytropic according to the law pVn = constant

Thus,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

In the polytropic process molar heat capacity is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q22: One mole of argon is expanded polytropically, the polytropic constant being n = 1.50. In the process, the gas temperature changes by ΔT = — 26 K. Find:
 (a) the amount of heat obtained by the gas;
 (b) the work performed by the gas

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: (a) Increment of internal energy for ΔT, becomes

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

From first law of thermodynamics

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b) Sought work done,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

 Q23: An ideal gas whose adiabatic exponent equals y is expanded according to the law p = αV , where a is a constant. The initial volume of the gas is equal to V0. As a result of expansion the volume increases η times. Find:
 (a) the increment of the internal energy of the gas;
 (b) the work performed by the gas;
 (c) the molar heat capacity of the gas in the process.

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Law of the process is p = α V or pV-1 = α
so the process is polytropic of index n = - 1
As p = αV so, Pi - αVand pf = α η V0

(a) Increment of the internal energy is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b) Work done by the gas is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(c) Molar heat capacity is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q24: An ideal gas whose adiabatic exponent equals γ is expanded so that the amount of heat transferred to the gas is equal to the decrease of its internal energy. Find:
 (a) the molar heat capacity of the gas in this process;
 (b) the equation of the process in the variables T, V;
(c) the work performed by one mole of the gas when its volume increases η times if the initial temperature of the gas is T0

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans:   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

where Cn is the molar heat capacity in the process. It is given that Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b) By the first law of thermodynamics, dQ - dU + dA,

or,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(c)   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

But from part (a), we have  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Thus   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

From part (b); we know  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So, Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET (where T is the final temperature)

Work done by the gas for one mole is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q25: One mole of an ideal gas whose adiabatic exponent equals y undergoes a process in which the gas pressure relates to the temperature as p = aTα, where a and α are constants. Find:
 (a) the work performed by the gas if its temperature gets an increment ΔT;
 (b) the molar heat capacity of the gas in this process; at what value of α will the heat capacity be negative? 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Given p = a Tα (for one mole of gas)

So,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Here polytropic exponent  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(a) In the poly tropic process for one mole of gas :

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b) Molar heat capacity is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q26: An ideal gas with the adiabatic exponent γ undergoes a process in which its internal energy relates to the volume as U = aVα, where a and α are constants. Find:
 (a) the work performed by the gas and the amount of heat to be transferred to this gas to increase its internal energy by ΔU;
 (b) the molar heat capacity of the gas in this process. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So polytropric index n = 1 - α

(a) Work done by the gas is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

By the first law of thermodynamics, Q = ΔU+A

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b) Molar heat capacity is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q27: An ideal gas has a molar heat capacity Cv at constant volume. Find the molar heat capacity of this gas as a function of its volume V, if the gas undergoes the following process: 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: By the first law .of thermodynamics

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Molar specific heat according to definition

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

We have   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

After differentiating, we get  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b)   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q28: One mole of an ideal gas whose adiabatic exponent equals γ undergoes a process p = p0 + α /V, w here P0 and α are positive constants. Find:
 (a) heat capacity of the gas as a function of its volume;
(b) the internal energy increment of the gas, the work performed by it, and the amount of heat transferred to the gas, if its volume increased from V1 to V2.

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Using 2.52

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET (for one mole of gas)

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEETIrodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Therefore   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b) Work done is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

By the first law of thermodynamics Q = ΔU +A

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q29: One mole of an ideal gas with heat capacity at constant pressure Cp undergoes the process T = T0 + αV, where T0 and α are constants. Find: 
 (a) heat capacity of the gas as a function of its volume;
(b) the amount of heat transferred to the gas, if its volume increased from V1 to V2

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: (a) Heat capacity is given by

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET   (see solution of 2.52)

We have  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

After differentiating, we get,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Hence   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b)  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET for one mole of gas

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Now  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

By the first law of thermodynamics Q = ΔU + A

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q30: For the case of an ideal gas find the equation of the process (in the variables T, V) in which the molar heat capacity varies as:
(a) C = Cv  + αT; (b) C = Cv + βV;  (c) C = Cv + ap, where α, β, and a are constants. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: Heat capacity is given by Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Integrating both sides, we get  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET is a constant.

Or,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

and  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Integrating both sides, we get   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEETIrodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or     Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  or V - a T = constant

Q31: An ideal gas has an adiabatic exponent γ. In some process its molar heat capacity varies as C = α/T, where α is a constant. Find:
(a) the work performed by one mole of the gas during its heating from the temperature T0 to the temperature η times higher; 
 (b) the equation of the process in the variables p, V. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: (a) By the first law of thermodynamics A = Q - ΔU

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Given    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b) Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Given   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Integrating both sides, we get

or, Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q32: Find the work performed by one mole of a Van der Waals gas during its isothermal expansion from the volume V1 to V2 at a temperature T. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: The work done is

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q33: One mole of oxygen is expanded from a volume V1 = 1.00 1 to V2 = 5.0 l at a constant temperature T = 280 K. Calculate:
 (a) the increment of the internal energy of the gas: 
 (b) the amount of the absorbed heat.
 The gas is assumed to be a Van der Waals gas. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: (a) The increment in the internal energy is

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

But from second law

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

On the other hand   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,    Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b) From the first law  

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q34: For a Van der Waals gas find:
 (a) the equation of the adiabatic curve in the variables T, V;
(b) the difference of the molar heat capacities Cp, — Cv  as a function of T and V. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: (a) From the first law for an adiabatic

dQ = dU + pd V = 0

From the previous problem

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

This equation can be integrated if we assume that Cv and b are constant then

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

(b)  We use  

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Now,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So along constant p, Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Thus  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

On differentiating,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

and   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Q35: Two thermally insulated vessels are interconnected by a tube equipped with a valve. One vessel of volume V1 =  10 l contains v = 2.5 moles of carbon dioxide. The other vessel of volume V2 = 100 l is evacuated. The valve having been opened, the gas adiabatically expanded. Assuming the gas to obey the Van der Waals equation, find its temperature change accompanying the expansion. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans: From the first law

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEETas the vessels are themally insulated.

As this is free expansion,   Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

But  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

So,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

or,  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

Substitution gives ΔT = - 3 K

Q36: What amount of heat has to be transferred to v = 3.0 moles of carbon dioxide to keep its temperature constant while it expands into vacuum from the volume V1 =  5.0 l to V2 = 10 l ? The gas is assumed to be a Van der Waals gas. 

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET  View Answer

Ans:  Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET (as A = 0 in free expansion).

So at constant temperature.

Irodov Solutions: The First Law of Thermodynamics, Heat Capacity | Physics Class 11 - NEET

= 0.33 kJ from the given data.

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FAQs on Irodov Solutions: The First Law of Thermodynamics, Heat Capacity - Physics Class 11 - NEET

1. What is the First Law of Thermodynamics and how does it relate to heat capacity?
Ans. The First Law of Thermodynamics states that energy cannot be created or destroyed, only transformed from one form to another. It is often expressed as ΔU = Q - W, where ΔU is the change in internal energy, Q is the heat added to the system, and W is the work done by the system. Heat capacity relates to this law as it defines the amount of heat required to change the temperature of a substance, indicating how much energy is absorbed or released during a temperature change.
2. How do we calculate heat capacity and what are its units?
Ans. Heat capacity (C) is calculated using the formula C = Q/ΔT, where Q is the heat added to or removed from the system and ΔT is the change in temperature. The units of heat capacity are typically expressed in joules per degree Celsius (J/°C) or joules per Kelvin (J/K), as the size of the temperature change is the same for both Celsius and Kelvin scales.
3. What is the difference between specific heat capacity and molar heat capacity?
Ans. Specific heat capacity (c) is defined as the amount of heat required to raise the temperature of one unit mass of a substance by one degree Celsius (or Kelvin). It is expressed in J/(kg·°C). Molar heat capacity (C_m) is the amount of heat required to raise the temperature of one mole of a substance by one degree Celsius (or Kelvin), expressed in J/(mol·°C). The key difference lies in the mass versus the amount of substance being considered.
4. Why is heat capacity important in thermodynamics and real-world applications?
Ans. Heat capacity is crucial in thermodynamics because it helps predict how a substance will respond to heat changes, which is essential for understanding energy transfer processes. In real-world applications, knowing the heat capacity of materials is vital for designing heating and cooling systems, cooking, climate control, and in various industrial processes where temperature regulation is critical.
5. How does heat capacity change with temperature and phase changes?
Ans. Heat capacity can vary with temperature because the amount of energy required to change the temperature of a substance may not be constant; it often increases with temperature due to increased molecular motion. Additionally, during phase changes (e.g., solid to liquid or liquid to gas), the heat capacity can differ significantly, as energy is used for breaking intermolecular bonds rather than increasing temperature, leading to a peak in heat capacity known as latent heat.
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