Thermodynamics Efficiency
Efficiency in thermodynamics represents how effectively a machine converts input energy into useful work. No engine is
1
0
0
%
efficient because some energy is always lost as heat.
Question in Mechanical Engineering
1
)
A heat engine receives
5
0
0
0
J of heat energy and produces
1
4
0
0
J of useful work. Calculate the efficiency of the engine and heat rejected to the surroundings.
Question:
Thermodynamics Efficiency
Efficiency in thermodynamics represents how effectively a machine converts input energy into useful work. No engine is
1
0
0
%
efficient because some energy is always lost as heat.
Question in Mechanical Engineering
1
)
A heat engine receives
5
0
0
0
J of heat energy and produces
1
4
0
0
J of useful work. Calculate the efficiency of the engine and heat rejected to the surroundings.
This is AI generated Response.
Asked by: Sam
Created at: 2025-11-17 00:25:02
Final Answer:
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# Thermodynamic Efficiency: Example Problem
## Problem Statement
A heat engine receives \( 500 \) J of energy (\( Q_{in} \)) and produces \( \) J of useful work (\( W \)).
Calculate:
- The efficiency (\( \eta \)) of the engine.
- The heat rejected (\( Q_{out} \)) to the surroundings.
---
## 1. Efficiency Calculation
**Efficiency (\( \eta \))** is defined as:
\[
\eta = \frac{\text{Useful Work Output}}{\text{Heat Input}} \times 100\%
\]
Plug in the given values:
\[
\eta = \frac{140\ \text{J}}{500\ \text{J}} \times 100\% = 28\%
\]
---
## 2. Heat Rejected Calculation
The **first law of thermodynamics** gives:
\[
Q_{in} = W + Q_{out}
\]
\[
Q_{out} = Q_{in} - W
\]
\[
Q_{out} = 500\ \text{J} - 140\ \text{J} = 360\ \text{J}
\]
---
## 3. Summary Table
| Quantity | Value |
|------------------|-------------|
| Heat Input (\( Q_{in} \)) | 500 J |
| Useful Work (\( W \)) | 140 J |
| Efficiency (\( \eta \)) | 28% |
| Heat Rejected (\( Q_{out} \)) | 360 J |
---
## 4. Key Points
- No real engine is 100% efficient because some energy is always lost as heat.
- The efficiency is always less than 100%.
---
**Image Example:**

*Heat engine schematic: \( Q_{in} \) enters, \( W \) exits as work, \( Q_{out} \) is rejected heat*
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