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Entropy

physical science Maturity 13-18 Next article →

Entropy is a fundamental scientific concept used to describe states of disorder, randomness, or uncertainty. It is a central idea in many different fields of study. You can find it in classical thermodynamics, which studies heat and energy. It is also used in statistical physics to describe the tiny world of atoms. Beyond physics, entropy is important in information theory, chemistry, biology, and even economics.

system boundary
system boundary

At its core, entropy measures how energy is distributed within a system. We describe energy as having "low" or "high" entropy. Low entropy means that energy is highly ordered or concentrated in one place. High entropy means that energy has become disordered or dispersed across a system. This concept is vital to the second law of thermodynamics. This law states that the entropy of an isolated system cannot decrease over time as it evolves spontaneously. Instead, these systems move toward thermodynamic equilibrium, which is the state where entropy is at its highest.

Temperature-entropy chart for steam, imperial units
Temperature-entropy chart for steam, imperial units

Scientists use two main ways to look at entropy. The first is the macroscopic perspective of classical thermodynamics. This approach uses measurable physical properties like volume, pressure, mass, and temperature to define a system's state. The second is the microscopic description found in statistical mechanics. This method looks at the motions of tiny individual particles, such as atoms or molecules. While these two views seem different, they actually provide a unified understanding of the same physical phenomenon.

First law open system
First law open system

The history of entropy began with early studies of heat engines. In 1824, Sadi Carnot published work on the motive power of fire. He used an analogy of a water wheel to explain how heat produces work. He noticed that work could be produced when heat falls through a temperature difference. Later, in 1850, William Rankine referred to this idea as heat-potential. In 1865, the German physicist Rudolf Clausius provided a formal mathematical definition. He defined entropy as the quotient of an infinitesimal amount of heat divided by the instantaneous temperature.

Clausius
Clausius

Clausius is also responsible for the name we use today. He originally called the concept "transformation-content" or *Verwandlungsinhalt*. He eventually chose the word "entropy" from a Greek word meaning transformation. He wanted the name to sound similar to the word "energy." He believed the two terms were analogous in their physical significance. This helped scientists see the relationship between the two quantities.

Clausius
Clausius

Another major breakthrough came from Ludwig Boltzmann. He introduced the concept of statistical disorder into thermodynamics. Boltzmann explained that entropy is a measure of the number of possible microscopic arrangements, or microstates, that a system can occupy. These arrangements must all match the macroscopic conditions of the system. He linked microscopic interactions to observable behavior using a logarithmic law. This work introduced the Boltzmann constant, which is now a defining universal constant in the International System of Units.

First law open system
First law open system

One of the most important consequences of entropy is irreversibility. Many natural processes only happen in one direction. For example, if a glass cup smashes on a concrete floor, it goes from an ordered state to a disordered state.

The pieces will not spontaneously jump back together to form a cup. This happens because the total entropy of the system and its surroundings increases. In contrast, a reversible process is one that happens so slowly that it stays in equilibrium. In a perfectly reversible cycle, like the Carnot cycle, the total change in entropy can be zero.

Temperature-entropy chart for steam, imperial units
Temperature-entropy chart for steam, imperial units

Entropy also helps us understand how materials change through physical processes. You can see a version of this in industrial settings. For instance, when standardized paper sheets are cut into many different small pieces, the entropy of the system increases. The organized sheets become a collection of heterogeneous offcuts.

NewOne-Mixed paper offcuts illustrating material entropy02
NewOne-Mixed paper offcuts illustrating material entropy02

This transition from an ordered state to a disordered state is a clear example of increasing entropy in a production system.

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system boundary.svg
File:Temperature-entropy chart for steam, imperial units.svg
Temperature-entropy chart for steam,...
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First law open system.svg
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