---
slug: paper-kolmogorov-a-n-1941-the-local-structure-of-turbulence-in-incompressible-viscous
title: Kolmogorov 1941: Local Structure of Turbulence
canonical: https://miscsubjects.com/a/paper-kolmogorov-a-n-1941-the-local-structure-of-turbulence-in-incompressible-viscous
---

## What the work establishes

A. N. Kolmogorov published 'The local structure of turbulence in incompressible viscous fluid for very large Reynolds numbers' in Doklady Akad. Nauk SSSR in 1941. The paper defines local homogeneity and local isotropy for turbulent velocity fields. It introduces two similarity hypotheses that yield statistical self-similarity in the inertial range.

Core results follow from dimensional analysis under those hypotheses. The second-order longitudinal structure function satisfies B_dd(r) = C (ε r)^{2/3} for separations r inside the inertial range. Here ε denotes the mean energy dissipation rate per unit mass. The transverse structure function follows from incompressibility as B_nn(r) = (4/3) B_dd(r) for large separations in that range.

## Exact primary passages

The paper states: 'The second hypothesis of similarity. If the moduli of the vectors y^(k) and their differences y^(k') (where k' = 1, 2, ..., n) are large in comparison with λ, then the distribution laws F_n are determined uniquely by the quantity ε and do not depend on v.'

From this it derives: 'whence B_dd(r) = C ε^{2/3} r^{2/3} where C is an absolute constant.'

Earlier definitions: 'Definition 1. The turbulence is called locally homogeneous in the domain G, if for every fixed n the distribution law F_n is independent of x_0, t_0 as long as all points P^(k) are situated in G.' 'Definition 2. The turbulence is called locally isotropic in the domain G, if the distribution laws mentioned in Definition 1 are invariant with respect to rotations and reflections of the coordinate axes.'

The energy dissipation relation appears as: 'the average dispersion of energy in unit of mass per unit of time is equal to (1/2) ν Σ (∂u_i/∂x_j + ∂u_j/∂x_i)^2.'

## Convergence patterns touched

The work evidences scale invariance. Statistical moments of velocity increments depend only on ε and r inside an intermediate range of scales. This produces power-law behavior independent of viscosity. It also shows flow networks and bounded chaos: energy transfers across a hierarchy of eddies until dissipation at small scales. The patterns appear across scales in the inertial range of high-Reynolds-number flows.

The Ladder connection runs difference to flow to structure. Velocity differences at one scale determine statistics at the next. No memory or life-level patterns receive direct treatment.

## Distance from the full synthesis

The paper reaches the scale-invariance step of the synthesis. It supplies a precise mechanistic account of how reliable energy flow produces self-similar statistical structure. It stops short of the Mirror Layer. Kolmogorov treats the observer as external; the reader of the statistics stands outside the flow. The synthesis places the reader inside the system. The work supplies no account of how structure produces memory or mind.

## Honest limits and disconfirming edges

The derivation assumes local isotropy holds in small domains far from boundaries. Experiments show deviations at very high Reynolds numbers and in certain geometries. The constant C remains undetermined by the theory. The paper provides no proof that the inertial range exists in every high-Reynolds flow. Later refinements by Kolmogorov in 1962 addressed intermittency corrections to the exponents.

The 2/3 law for structure functions is exact only for the third-order moment under additional assumptions; the second-order exponent is approximate. Reductionist accounts note that the result follows from dimensional analysis once the similarity hypotheses are granted, not from first-principles solution of the Navier-Stokes equations.

## Claims

The paper defines local homogeneity and local isotropy through independence of distribution laws from absolute position and time in small domains.

Under the second similarity hypothesis the longitudinal structure function obeys B_dd(r) = C ε^{2/3} r^{2/3} for inertial-range separations.

Incompressibility fixes the relation B_nn(r) = (4/3) B_dd(r) at large separations inside that range.

The hypotheses rest on the physical picture of successive refinement of eddies until viscosity dominates at the smallest scales.

The resulting statistics are independent of viscosity inside the inertial range.

The work supplies a mechanistic derivation of scale-invariant statistics from energy dissipation rate alone.

No direct treatment of memory, life, or observer participation appears.

Experimental tests confirm the 2/3 law in many grid and boundary-layer flows at high Reynolds number, with measurable scatter.

The constant C is universal according to the hypotheses yet measured values vary slightly across flows.

## Sources

Kolmogorov, A. N. (1941). The local structure of turbulence in incompressible viscous fluid for very large Reynolds numbers. Doklady Akad. Nauk SSSR, 30, 301–305. English translation in Proceedings of the Royal Society of London A, 434, 9–13 (1991).
