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Ch 21: Heat Engines and Refrigerators
Knight Calc - Physics for Scientists and Engineers 5th Edition
Knight Calc5th EditionPhysics for Scientists and EngineersISBN: 9780137344796Non è quello che usi tu?Cambia libro di testo
Capitolo 21, Problema 63b

The heat engine shown in FIGURE P21.63 uses 0.020 mol of a diatomic gas as the working substance. Make a table that shows ∆Eth, Ws, and Q for each of the three processes.

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Step 1: Identify the three processes in the heat engine cycle from the graph. The processes are: (1 → 2) adiabatic compression, (2 → 3) isobaric expansion, and (3 → 1) isochoric cooling.
Step 2: For each process, calculate the change in internal energy (∆Eth) using the formula ∆Eth = n * Cv * ∆T, where n is the number of moles, Cv is the molar specific heat at constant volume for a diatomic gas, and ∆T is the change in temperature. Use the ideal gas law (PV = nRT) to find temperatures at each state.
Step 3: Calculate the work done (Ws) for each process. For the adiabatic process (1 → 2), use the formula Ws = (P2 * V2 - P1 * V1) / (γ - 1), where γ = Cp/Cv. For the isobaric process (2 → 3), use Ws = P * ∆V. For the isochoric process (3 → 1), Ws = 0 since volume does not change.
Step 4: Calculate the heat transfer (Q) for each process using the first law of thermodynamics: Q = ∆Eth + Ws. For the adiabatic process (1 → 2), Q = 0 since no heat is exchanged. For the isobaric and isochoric processes, use the calculated values of ∆Eth and Ws.
Step 5: Organize the results into a table with columns for each process (1 → 2, 2 → 3, 3 → 1) and rows for ∆Eth, Ws, and Q. Ensure all values are consistent with the calculations and the graph provided.

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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 heat engine, this principle relates the change in internal energy (∆E_th) to the work done by the system (W_s) and the heat added to the system (Q) through the equation ∆E_th = Q - W_s.
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The First Law of Thermodynamics

Heat Transfer (Q)

Heat transfer (Q) refers to the energy exchanged between the system and its surroundings due to a temperature difference. In a heat engine, Q is the heat absorbed from the hot reservoir during the heating process, which is essential for performing work and changing the internal energy of the gas.
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Work Done by the System (W_s)

Work done by the system (W_s) is the energy transferred when the gas expands or compresses against an external pressure. In the context of the heat engine cycle shown in the diagram, W_s can be calculated during the expansion and compression processes, which are critical for understanding the engine's efficiency and performance.
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