1. A Carnot engine operates between reservoirs at 610 and 315 K. If the engine absorbs 75J per cycle at the hot reservoir. Calculate (a) The efficiency, e, of the engine e= (b) The work output per cycle W. = per cycle
1. A Carnot engine operates between reservoirs at 610 and 315 K. If the engine absorbs 75J per cycle at the hot reservoir. Calculate (a) The efficiency, e, of the engine e= (b) The work output per cycle W. = per cycle
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Author:Raymond A. Serway, Chris Vuille
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![Certainly! Here is the transcription of the provided image text along with an explanation suited for an educational website:
---
### Carnot Engine Thermodynamics
1. A Carnot engine operates between reservoirs at 610 K and 315 K. If the engine absorbs 75 J per cycle at the hot reservoir.
Calculate:
(a) **The efficiency, \( e \), of the engine:**
\[ e = \ \] [Input Box]
(b) **The work output per cycle:**
\[ W_{\text{per cycle}} = \ \] [Input Box] J
---
The image provided shows a problem related to a Carnot engine, a theoretical thermodynamic cycle proposed by Nicolas Léonard Sadi Carnot. According to Carnot's theorem, no engine operating between two heat reservoirs can be more efficient than a Carnot engine operating between the same reservoirs.
- **Efficiency (\( e \)):** The efficiency of a Carnot engine is determined by the temperatures of the hot (\( T_H \)) and cold (\( T_C \)) reservoirs. It is given by the formula:
\[
e = 1 - \frac{T_C}{T_H}
\]
where \( T_H \) is the absolute temperature of the hot reservoir, and \( T_C \) is the absolute temperature of the cold reservoir.
- **Work output per cycle:** The work output (\( W_{\text{per cycle}} \)) is related to the engine efficiency and the heat absorbed from the hot reservoir (\( Q_H \)). It can be calculated using:
\[
W_{\text{per cycle}} = e \times Q_H
\]
where \( Q_H \) is the heat absorbed per cycle at the hot reservoir.
Here, the temperatures and the heat absorbed are provided:
- \( T_H = 610 \) K
- \( T_C = 315 \) K
- \( Q_H = 75 \) J
You can calculate the values by plugging in the numbers into the formulas provided.
This exercise helps understand the fundamental principles of thermodynamics and the efficiency limits of heat engines.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Fd88a7a9a-3f1e-4a05-9f09-8e85dfb857a6%2F41002165-4d2a-4e40-98ab-47e967cea9aa%2F5zt2llj_processed.png&w=3840&q=75)
Transcribed Image Text:Certainly! Here is the transcription of the provided image text along with an explanation suited for an educational website:
---
### Carnot Engine Thermodynamics
1. A Carnot engine operates between reservoirs at 610 K and 315 K. If the engine absorbs 75 J per cycle at the hot reservoir.
Calculate:
(a) **The efficiency, \( e \), of the engine:**
\[ e = \ \] [Input Box]
(b) **The work output per cycle:**
\[ W_{\text{per cycle}} = \ \] [Input Box] J
---
The image provided shows a problem related to a Carnot engine, a theoretical thermodynamic cycle proposed by Nicolas Léonard Sadi Carnot. According to Carnot's theorem, no engine operating between two heat reservoirs can be more efficient than a Carnot engine operating between the same reservoirs.
- **Efficiency (\( e \)):** The efficiency of a Carnot engine is determined by the temperatures of the hot (\( T_H \)) and cold (\( T_C \)) reservoirs. It is given by the formula:
\[
e = 1 - \frac{T_C}{T_H}
\]
where \( T_H \) is the absolute temperature of the hot reservoir, and \( T_C \) is the absolute temperature of the cold reservoir.
- **Work output per cycle:** The work output (\( W_{\text{per cycle}} \)) is related to the engine efficiency and the heat absorbed from the hot reservoir (\( Q_H \)). It can be calculated using:
\[
W_{\text{per cycle}} = e \times Q_H
\]
where \( Q_H \) is the heat absorbed per cycle at the hot reservoir.
Here, the temperatures and the heat absorbed are provided:
- \( T_H = 610 \) K
- \( T_C = 315 \) K
- \( Q_H = 75 \) J
You can calculate the values by plugging in the numbers into the formulas provided.
This exercise helps understand the fundamental principles of thermodynamics and the efficiency limits of heat engines.
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