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Statistical mechanics

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Statistical mechanics is a mathematical framework used in physics. It applies probability theory and statistical methods to large groups of microscopic entities. This field is also called statistical physics or statistical thermodynamics. Its main goal is to explain the properties of matter in aggregate. It does this by using the physical laws that govern atomic motion. This science is useful in many different areas. These include biology, neuroscience, computer science, information theory, and sociology.

In standard mechanics, scientists study two main types. These are classical mechanics and quantum mechanics. In classical mechanics, a system is described by a phase point. In quantum mechanics, it is described by a pure quantum state vector. Scientists use equations of motion to move these states forward in time. For classical systems, they use Hamilton's equations. For quantum systems, they use the Schrödinger equation. These equations allow us to calculate a state at any point in time. However, there is a disconnect between these laws and our daily experience. We cannot know the exact position and velocity of every single molecule during a chemical reaction.

Statistical mechanics bridges this gap by adding uncertainty. Instead of looking at one single state, it introduces a statistical ensemble. An ensemble is a large collection of virtual, independent copies of a system. It represents a probability distribution over all possible states. In classical statistical mechanics, this is a distribution over phase points. In quantum statistical mechanics, it is a distribution over pure states. This is often summarized as a density matrix. The ensemble evolves over time as virtual systems move from one state to another. This evolution is guided by the Liouville equation in classical mechanics. In quantum mechanics, the evolution follows the von Neumann equation.

Gibbs-Elementary principles in statistical mechanics
Gibbs-Elementary principles in statistical mechanics

There are different types of ensembles. Some are known as equilibrium ensembles. These do not evolve over time, and their condition is called statistical equilibrium. Statistical equilibrium does not mean the particles have stopped moving. It means the ensemble itself is not changing. In contrast, mechanical equilibrium is a state where forces are balanced and motion has ceased. Statistical mechanics also includes non-equilibrium statistical mechanics. This branch studies ensembles that change over time or belong to non-isolated systems. It helps model the speed of irreversible processes like heat flows or chemical reactions. The fluctuation–dissipation theorem is a key concept here. It studies the simplest non-equilibrium situation of steady state current flow.

Gibbs-Elementary principles in statistical mechanics
Gibbs-Elementary principles in statistical mechanics

The history of this field spans many years. In 1738, Swiss mathematician Daniel Bernoulli published Hydrodynamica. This work laid the basis for the kinetic theory of gases. He argued that gases consist of many molecules moving in all directions. He suggested that their impact on a surface causes gas pressure. He also proposed that heat is the kinetic energy of their motion.

In 1859, James Clerk Maxwell formulated the Maxwell distribution of molecular velocities. This gave the proportion of molecules with a specific velocity. This was the first statistical law in physics. Maxwell also showed that molecular collisions lead to an equalization of temperatures. In 1864, Ludwig Boltzmann began developing the subject further. Boltzmann developed the interpretation of entropy using microstates. He also introduced the concept of an equilibrium statistical ensemble. His work includes about 2,000 pages of papers on subjects like the H-theorem and thermal equilibrium.

Gibbs-Elementary principles in statistical mechanics
Gibbs-Elementary principles in statistical mechanics

The field was officially named by Josiah Willard Gibbs in 1884. Gibbs was an American mathematical physicist. In 1902, he published Elementary Principles in Statistical Mechanics. This book formalized the field as a general approach for all mechanical systems. His methods were originally derived from classical mechanics. However, they were general enough to adapt to quantum mechanics. This allows the field to remain a foundation for science today.

Gibbs-Elementary principles in statistical mechanics
Gibbs-Elementary principles in statistical mechanics

Statistical thermodynamics is a specific branch of this science. Its goal is to derive the classical thermodynamics of materials. It connects macroscopic properties to microscopic behaviors. One common idea used is the equal a priori probability postulate. This states that an isolated system can be found in any microstate with equal probability. This is often linked to the ergodic hypothesis. An ergodic system explores all accessible states over time. Another idea is the principle of indifference, which assigns equal probabilities when information is missing. There are also three main equilibrium ensembles used in statistical thermodynamics. These include the microcanonical ensemble, which describes systems with precise energy and composition. These ensembles all correspond to classical thermodynamics in the macroscopic limit.

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