concept

boltzmann entropy

Statistical definition of entropy relating to the number of microstates of a system.
18 related articles

Description

Boltzmann entropy is a statistical mechanics definition of entropy that quantifies the number of microscopic configurations (microstates) consistent with a given macroscopic state (macrostate). It is expressed as S = k_B ln W, where k_B is Boltzmann's constant and W is the number of microstates. This definition provides a probabilistic foundation for the second law of thermodynamics, explaining why entropy tends to increase: systems naturally evolve toward macrostates with the largest number of microstates.

History

Ludwig Boltzmann introduced this statistical interpretation of entropy in the 1870s, building on the work of James Clerk Maxwell. His ideas were controversial at the time but became foundational for statistical mechanics.

How it works

The entropy is computed by counting all possible arrangements of particles (positions, momenta, spins, etc.) that yield the same macroscopic properties like temperature, pressure, and volume. The logarithm of this count, multiplied by Boltzmann's constant, gives the entropy. This approach connects the microscopic laws of physics to macroscopic thermodynamic behavior, and it underlies the concept of equilibrium as the most probable state.

In practice

It is used in computational physics to simulate thermodynamic systems, in information theory to define entropy, and in cosmology to discuss the arrow of time and the initial low-entropy state of the universe.

Fun fact

Boltzmann's entropy formula is engraved on his tombstone in Vienna, a testament to its central role in physics.

Concept graph →

Related articles · 18

Living Particles Form Swarms Without a Leader
A cluster of glowing dots drifts through the darkness, now compressing into islands, now spreading out in waves. These are not fish or birds: this is a mathematical model of active matter, where each particle spends its own energy on movement, and also is born, dies, and competes with neighbors for space.
Entropic Tuning Fork of Evolution: Proteins and Notes of Complexity
Biological complexity has long eluded us: you can count genes, cells too, but how do you grasp the organization of the proteome itself — a multi-thousand ensemble of proteins woven from carbon, oxygen, and hydrogen?
HEP Phenomenology2026-06-132 minarXiv:2606.15364express
Spin-1 Fluid: A Universal Recipe for Motion
Picture a pot of boiling soup, but every grain in it is not just a point but a tiny top spinning around its own axis. That's the world of spin-1 particles. For example, some short-lived mesons born in accelerator collisions.
HEP Theory2026-05-312 minarXiv:2606.01296express
Wormholes Between Theories: How to Compare Quantum Worlds
Every quantum system (whether an atom, a crystal, or the entire Universe) has its own set of allowed energies, like the steps of a ladder. The hotter the system, the more readily particles climb to higher rungs.
General Relativity2026-05-281 minarXiv:2605.30405express
Universe as a Precise Mechanism: No 'Boltzmann Brains'
An eternal Universe where the measure of disorder (энтропия) grows is, for most of its time, a homogeneous void. In it, complex structures occasionally assemble by chance, such as fleeting consciousnesses — ‘мозги Больцмана’.
General Relativity2026-05-211 minarXiv:2605.22172express
How to Measure the Chaos of Spacetime Itself
Spacetime isn't a flat sheet, but a crumpled fabric: stars and planets leave creases on it. Information is written into every crease, and to erase it, heat would have to be released — that's how Landauer's principle works. Thus, the 'crumpledness' of space can be measured through entropy — the universal measure of disorder.
Quantum Physics2026-05-151 minarXiv:2605.16148express
How Internal Noise Destroys Quantum Magic
In a football stadium, the crowd's emotions arise from the chatter of individual fans. If mood could be both joyful and sorrowful at once, you'd have a quantum superposition. But the murmur of thousands of voices instantly forces that blend into a single definite state.
Statistical Mech2026-04-212 minarXiv:2604.19244express
How a Leaderless Rearrangement Points to Hidden Order
An orchestra without a conductor is playing, and suddenly, without any visible cue, the violins grow louder and the woodwinds shift slightly in time. From the outside, nothing seems to have changed, but inside the ensemble, a regrouping has occurred. This is roughly how small physical systems behave during so-called third-order pseudotransitions.
HEP Phenomenology2026-04-141 minarXiv:2604.12691express
How a quantum proton becomes a hot liquid
At the Large Hadron Collider, not only nuclei but also individual protons collide. Even in such small systems, collective behavior resembling the flow of a liquid is observed. But the proton is a quantum object; its state is described by a wave function, not by temperature and pressure.
Dynamical Systems2026-04-111 minarXiv:2604.10225express
Which Phases of Matter Are Real, and Which Are a Mirage
Water can be ice, liquid, or steam. Physicists call these states phases. In theory, each phase has its own measure — a way to describe how likely it is. But not every measure you can imagine occurs in nature. Some phases are real, while others are just mathematical illusions. Scientists have found a simple criterion that separates reality from mirage.
Statistical Mech2026-04-031 minarXiv:2604.02662express
Busting Myths About Bose–Einstein Condensate
In an orchestra where every musician plays the same note, the sound merges into a powerful unison. This is how a Bose–Einstein condensate is born: many boson particles at extremely low temperatures behave as a single entity.
Math Physics2026-02-171 minarXiv:2602.15943express
Light, Sorted into Shelves
A charged particle spiraling in a magnetic field doesn't stay silent: it emits light. This light is called synchrotron radiation, and it shows up everywhere — from distant galaxies to laboratory accelerators.
Plasma Physics2026-01-311 minarXiv:2602.00600express
Dancing Chaos: How to Measure the Complexity of Turbulence
Hot plasma in a future fusion reactor is like a packed dance floor: billions of particles whirl in a complex rhythm, colliding and changing speed. Figuring out how tangled this dance is — no easy task. Scientists have found a way to measure its complexity without watching every move.
Quantum Physics2026-01-092 minarXiv:2601.05514express
A Wire Heats Up from Knowledge
Run a current through a wire, and the wire heats up. Anyone who has ever touched a phone charger knows this. Physicists call this heating Joule heating, after James Joule, who in the mid-19th century measured how much heat electricity produces. Since then, the formula has been simple: the greater the resistance and the current, the hotter the wire.
Quantum Gases2026-01-031 minarXiv:2601.01039express
How quantum fog tests the laws of gravity
An ultracold atomic cloud, resembling fog, hints that gravity might not work as Newton said. On the outskirts of galaxies stars move faster than expected, and MOND theory tweaks the law of gravitation over large distances, removing the need for dark matter.
Quantum Gases2025-12-091 minarXiv:2512.08739express
Supersolidity Is Born at the Liquid Boundary
A supersolid is ice that flows. Think of a pond with a frozen crust, but beneath it, a liquid depth without friction. Usually, creating that crust means changing the liquid's properties throughout its entire volume.
The Eraser That Erases the Past: How Quantum Information Creates Irreversibility
A wave rolls onto the sand, leaving a pattern of foam and shells. A moment later it recedes, but the traces are no longer the same: the sand is smoothed, the shells are flipped over. Something similar happens in the quantum world when a system moves from a nonequilibrium state toward equilibrium.
Symphony of Imaginary Frequencies: Quantum Decay of the Inverted Well
At the hilltop of classical physics, a particle is frozen in unstable equilibrium. The slightest nudge — and it rolls down with increasing speed. In the quantum universe, no nudge is needed: the uncertainty principle itself acts as an all-pervading wind, blowing the particle off the peak.