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Irodov Solutions: The First Law of Thermodynamics, Heat Capacity

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

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. 

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. 

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.

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? 

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.

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. 

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. 

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. 

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. 

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? 

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. 

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. 

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. 

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.

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.

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.

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. 

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. 

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? 

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.

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

 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.

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

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? 

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. 

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

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.

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

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. 

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. 

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. 

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. 

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. 

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. 

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. 

The document Irodov Solutions: The First Law of Thermodynamics, Heat Capacity is a part of the NEET Course Physics Class 11.
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FAQs on Irodov Solutions: The First Law of Thermodynamics, Heat Capacity

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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