Example 1: Heat Engine
A steam power plant takes in heat from a boiler at 500°C and rejects heat to a condenser at 30°C. According to Kelvin–Planck, it cannot convert all the boiler heat into work; some must be rejected to the condenser.
This page provides a detailed, easy-to-understand explanation of the formal statements of the Second Law of Thermodynamics, their physical meaning, equivalence, and engineering implications.
The Second Law of Thermodynamics introduces the concept of directionality and feasibility of processes, complementing the First Law (energy conservation). It tells us which processes can occur spontaneously and sets limits on the conversion of heat into work.
Statement: “It is impossible to construct a device that operates in a cycle and produces no effect other than the extraction of heat from a single thermal reservoir and the performance of an equivalent amount of work.”
Meaning: No heat engine can have 100% thermal efficiency when operating between a single reservoir and producing only work. There must be heat rejection to a lower-temperature reservoir.
Implication: All practical heat engines must reject some heat; efficiency is always less than 1.
Statement: “It is impossible to construct a device that operates in a cycle and produces no effect other than the transfer of heat from a colder body to a hotter body without the input of external work.”
Meaning: Heat cannot spontaneously flow from cold to hot; to do so requires work input (as in refrigerators and heat pumps).
Implication: Refrigerators and heat pumps must consume work to move heat against the natural temperature gradient.
A steam power plant takes in heat from a boiler at 500°C and rejects heat to a condenser at 30°C. According to Kelvin–Planck, it cannot convert all the boiler heat into work; some must be rejected to the condenser.
A domestic refrigerator moves heat from the cold interior to the warmer kitchen air. According to Clausius, this requires electrical work input to the compressor.