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One mole of an ideal monatomic gas is used as the working substance of engine that operates on the cycle shown in Fig. 24-20. Calculate (a) the work done by the engine per cycle. (b) the heat added per cycle during the expansion stroke abc, and (c) the engine efficiency. (d) What is the cannot efficiency of an engine operating between the highest and lowest temperature present in the cycle? How does this compare to the efficiency calculated in (c)? Assume that p1 = 2p0, V1 = 2v0, p0 = 1.01 × 105 Pa, and V0 = 0.0225 m3,
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Shane Macguire , 10 Years ago
Grade upto college level
anser 1 Answers
Askiitians Tutor Team

To tackle this problem, we need to analyze the thermodynamic cycle of the engine and apply the relevant equations for work, heat, and efficiency. Let's break it down step by step, addressing each part of your question systematically.

Work Done by the Engine per Cycle

The work done by the gas during a thermodynamic cycle can be calculated using the area enclosed by the cycle on a pressure-volume (P-V) diagram. For a monatomic ideal gas, the work done during an isothermal or adiabatic process can be derived from the equations of state and the specific processes involved.

In this case, we need to identify the points of the cycle and the nature of the processes (isothermal, isochoric, isobaric, or adiabatic). Assuming the cycle consists of two isothermal processes and two adiabatic processes, we can calculate the work done during the expansion and compression phases.

  • During the expansion stroke (from point a to b), the work done (Wab) can be calculated using the formula for work done during an isothermal expansion:
  • Wab = nRT ln(Vb/Va)
  • During the compression stroke (from point c to d), the work done (Wcd) can be calculated similarly, but it will be negative since work is done on the gas:
  • Wcd = -nRT ln(Vd/Vc)

By summing these two contributions, we can find the total work done per cycle:

Wcycle = Wab + Wcd

Heat Added per Cycle During Expansion Stroke

To find the heat added during the expansion stroke (abc), we can use the first law of thermodynamics, which states that the change in internal energy (ΔU) is equal to the heat added (Q) minus the work done (W):

ΔU = Q - W

For an ideal monatomic gas, the change in internal energy during an isothermal process is zero, so:

Qab = Wab

Calculating Engine Efficiency

Engine efficiency (η) is defined as the ratio of the work output to the heat input. Thus, we can express it as:

η = Wcycle / Qin

Where Qin is the heat added during the expansion stroke. We can substitute our previous results into this equation to find the efficiency of the engine.

Carnot Efficiency Calculation

The Carnot efficiency (ηCarnot) is given by the formula:

ηCarnot = 1 - (Tlow / Thigh)

To find the temperatures, we can use the ideal gas law and the given pressures and volumes to determine the temperatures at the highest and lowest points in the cycle. Once we have Thigh and Tlow, we can calculate the Carnot efficiency.

Comparison of Efficiencies

Finally, we can compare the calculated efficiency from part (c) with the Carnot efficiency from part (d). The Carnot efficiency sets an upper limit on the efficiency of any heat engine operating between two temperatures, and it will always be greater than or equal to the efficiency of real engines.

By following these steps and performing the necessary calculations, you will arrive at the answers for each part of the question. If you have specific values for the pressures and volumes, we can plug those into the equations to find numerical results. Let me know if you need help with that!

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