Kelvin's Statement & Efficiency of a Heat Engine
Detailed explanation of Kelvin's statement of the Second Law of Thermodynamics, essentials and working principle of heat engines, and step-by-step derivation of thermal efficiency (η).
1. Kelvin's Statement of 2nd Law of Thermodynamics
"It is impossible to construct an engine, operating continuously in a cycle, that can take heat from a source and convert it completely into work."
Explanation: When converting heat into mechanical work, a cyclic engine cannot convert 100% of the input heat energy into work. A fraction of the absorbed heat must always be rejected to a lower-temperature reservoir (the exhaust/sink). Thus, even though the First Law of Thermodynamics is fully satisfied, it is impossible to build an engine with an efficiency of 100%.
2. Heat Engines & Their Working Principle
Definition: Any device that transforms thermal energy (heat) into mechanical energy (work) is called a heat engine.
Essentials of a Heat Engine: Every heat engine consists of three essential components:
- Hot Reservoir (Source): Maintains a high temperature (T1) and supplies heat energy (Q1).
- Working Substance: The material (such as gas or steam) inside the engine that absorbs heat and performs mechanical work.
- Cold Reservoir (Sink): Maintains a lower temperature (T2) and absorbs waste heat (Q2).
Working Mechanism
All cyclic heat engines function through a repeating thermodynamic process:
- The working substance absorbs heat Q1 from the high-temperature source (T1).
- It expands and performs net mechanical work W on the surroundings.
- It discards the remaining waste heat Q2 to the low-temperature sink (T2) through exhaust or cooling systems to return to its initial state.
From energy conservation, the net mechanical work done W in one complete cycle is:
3. Thermal Efficiency of a Heat Engine
The effectiveness of a heat engine is measured by its **thermal efficiency** (η).
Mathematically:
Derivation of Formula
Substituting W = Q1 − Q2 into the efficiency expression:
η = Q1 − Q2Q1 &implies; η = 1 − Q2Q1
In percentage form:
In terms of absolute temperatures of the source (T1) and sink (T2):
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