One mole of monatomic gas undergoes a Carnot cycle with TH = 350°C and TL = 210°C. The initial pressure is 8.8 atm. During the isothermal expansion, the volume doubles. Find the values of the pressure and volume at the points a, b, c, and d of Fig. 20–5.
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23. The Second Law of Thermodynamics
The Carnot Cycle
Problem 20b
Textbook Question
(III) One mole of monatomic gas undergoes a Carnot cycle with TH = 350°C and TL = 210°C. The initial pressure is 8.8 atm. During the isothermal expansion, the volume doubles. Determine Q, W, and ∆Eint for each segment of the cycle.

1
Step 1: Convert the temperatures from Celsius to Kelvin. The Carnot cycle operates with temperatures in Kelvin, so use the formula T(K) = T(°C) + 273. For TH = 350°C, T_H = 350 + 273 = 623 K. For TL = 210°C, T_L = 210 + 273 = 483 K.
Step 2: Understand the Carnot cycle. It consists of four processes: (1) isothermal expansion at T_H, (2) adiabatic expansion from T_H to T_L, (3) isothermal compression at T_L, and (4) adiabatic compression from T_L to T_H. Each segment involves specific calculations for heat transfer (Q), work done (W), and change in internal energy (∆E_int).
Step 3: For the isothermal expansion at T_H, use the ideal gas law and the formula for work done during isothermal processes: W = nRT_H ln(V_f/V_i), where n is the number of moles, R is the gas constant (8.314 J/mol·K), T_H is the high temperature, and V_f/V_i is the ratio of final to initial volume. Since the volume doubles, V_f/V_i = 2. Calculate Q using Q = W, as ∆E_int = 0 for isothermal processes.
Step 4: For the adiabatic expansion from T_H to T_L, use the adiabatic condition for a monatomic gas: TV^(γ-1) = constant, where γ = 5/3 for monatomic gases. Relate the initial and final states to find the work done (W) using the formula W = (P_iV_i - P_fV_f)/(γ - 1). Note that Q = 0 for adiabatic processes, and ∆E_int can be calculated using ∆E_int = -W.
Step 5: Repeat similar calculations for the isothermal compression at T_L and the adiabatic compression from T_L to T_H. For the isothermal compression, use W = nRT_L ln(V_f/V_i) and Q = W. For the adiabatic compression, use the same adiabatic relations as in Step 4. Sum up Q, W, and ∆E_int for each segment to analyze the entire cycle.

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Key Concepts
Here are the essential concepts you must grasp in order to answer the question correctly.
Carnot Cycle
The Carnot cycle is a theoretical thermodynamic cycle that provides the maximum possible efficiency for a heat engine operating between two temperature reservoirs. It consists of four reversible processes: two isothermal (constant temperature) and two adiabatic (no heat exchange). Understanding this cycle is crucial for analyzing the performance of real engines and calculating work and heat transfer in thermodynamic processes.
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First Law of Thermodynamics
The First Law of Thermodynamics states that energy cannot be created or destroyed, only transformed from one form to another. In the context of a thermodynamic cycle, it can be 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. This principle is essential for calculating the energy changes during each segment of the Carnot cycle.
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The First Law of Thermodynamics
Isothermal Process
An isothermal process occurs at a constant temperature, meaning that the internal energy of an ideal gas remains unchanged during this process. For an ideal monatomic gas, the work done during isothermal expansion can be calculated using the formula W = nRT ln(Vf/Vi), where Vf and Vi are the final and initial volumes, respectively. This concept is vital for determining the heat transfer and work done during the isothermal segments of the Carnot cycle.
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Entropy & Ideal Gas Processes
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