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Physics · Ch 11 — Thermodynamics

Second Law of Thermodynamics

11.9

Second Law of Thermodynamics

The Second Law of Thermodynamics

The first law of thermodynamics tells us that energy is conserved in every process. But it says nothing about which processes can actually happen. Many processes that conserve energy are never observed in nature. For example, a hot cup of coffee left on a table cools down spontaneously — the heat flows from the coffee into the surrounding air. The reverse process — the coffee getting hotter while the air around it gets colder — would also conserve energy, but it never happens. Why?

The second law of thermodynamics answers this question. It identifies the direction in which natural processes occur and places a fundamental restriction on what is possible, even when energy is conserved.

The Kelvin–Planck Statement

One way to state the second law focuses on heat engines. A heat engine takes heat Q1Q_1 from a hot reservoir, does work WW, and rejects the remaining heat Q2Q_2 to a cold reservoir. The first law requires Q1=W+Q2Q_1 = W + Q_2. Could we build an engine that converts all the heat it absorbs into work, so that Q2=0Q_2 = 0? Such a device would be a perfect heat engine — 100% efficient.

The Kelvin–Planck statement says this is impossible:

Important

Kelvin–Planck statement: It is impossible to construct a heat engine that, operating in a cycle, produces no effect other than the absorption of heat from a single reservoir and the performance of an equal amount of work.

In other words, no cyclic process can convert heat completely into work. Some heat must always be rejected to a colder reservoir. This is why the efficiency of any real heat engine is always less than 1.

The Clausius Statement

Another way to state the second law focuses on the flow of heat. We know that heat flows spontaneously from a hot body to a cold body, never the other way. Could we build a device that transfers heat from a cold body to a hot body without any other change? Such a device would be a perfect refrigerator — it would cool something without needing any work input.

The Clausius statement says this is impossible:

Important

Clausius statement: It is impossible to construct a refrigerator that, operating in a cycle, produces no effect other than the transfer of heat from a colder body to a hotter body.

A real refrigerator requires work input to move heat from cold to hot. The Clausius statement simply says that heat cannot, by itself, flow from a colder to a hotter body.

Equivalence of the Two Statements

Though they sound different, the Kelvin–Planck and Clausius statements are logically equivalent. If you could violate one, you could build a device that violates the other. The proof goes like this:

›Proof

Proof of equivalence

Part 1: Suppose a device violates the Kelvin–Planck statement — a heat engine that takes heat QQ from a hot reservoir and converts it entirely into work W=QW = Q, with no heat rejected. Use this work to drive a perfect refrigerator that takes heat Q2Q_2 from a cold reservoir and delivers heat Q1=Q2+WQ_1 = Q_2 + W to the hot reservoir. The net effect on the hot reservoir is zero (the engine takes QQ, the refrigerator returns Q2+W=Q2+QQ_2 + W = Q_2 + Q), but heat Q2Q_2 has been transferred from cold to hot with no other change — a violation of the Clausius statement.

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