---
slug: paper-poincar-h-1890-sur-le-probl-me-des-trois-corps-et-les-quations-de-la-dynamique-a
title: Poincaré 1890: Three-Body Problem and Bounded Chaos
canonical: https://miscsubjects.com/a/paper-poincar-h-1890-sur-le-probl-me-des-trois-corps-et-les-quations-de-la-dynamique-a
---

## What the work establishes
Henri Poincaré submitted his memoir to the 1889 King Oscar II prize competition. The revised version appeared in Acta Mathematica volume 13 in 1890. The paper examines the motion of three bodies under Newtonian gravity. It shows that no general analytic integral exists beyond the known energy and momentum integrals. It also demonstrates that certain orbits exhibit sensitive dependence on initial conditions. Small changes in starting positions or velocities produce trajectories that diverge exponentially over time while remaining bounded.

The memoir introduces qualitative methods. Poincaré studies periodic solutions and their stability. He identifies homoclinic orbits where a trajectory returns arbitrarily close to a saddle point after looping away. These tangles generate complex behavior that cannot be captured by convergent series expansions of the classical type.

## Exact primary work and verifiable passages
The primary source is Poincaré, H. (1890). Sur le problème des trois corps et les équations de la dynamique. Acta Mathematica, 13, 1-270. No page-specific verbatim excerpts from the original French text appear in publicly indexed secondary sources with verifiable pagination. Secondary accounts confirm the core claims: non-existence of additional analytic integrals and the presence of homoclinic tangles. June Barrow-Green's monograph provides the most detailed historical reconstruction.

A later popular formulation of sensitive dependence appears in Poincaré's Science and Hypothesis (1902), not in the 1890 memoir itself. That formulation states: "If we knew exactly the laws of nature and the situation of the universe at the initial moment, we could predict exactly the situation of that same universe at a succeeding moment. But even if it were the case that the natural laws had no longer any secret for us, we could still only know the initial situation approximately." The 1890 technical memoir supplies the mathematical mechanism behind the later statement.

## Convergence patterns evidenced
The memoir supplies the first rigorous mathematical demonstration of bounded chaos in a concrete physical system. Bounded chaos is one of the grain patterns listed in the OIP/GRAIN synthesis: energy flows produce narrow families of structural patterns that include bounded chaos. The three-body system generates flow networks of trajectories, symmetry breaking at saddle points, and scale-invariant features near homoclinic points. These patterns emerge from the deterministic equations without external imposition.

The work touches the Ladder at the level of difference to flow to structure. Initial differences in position and velocity flow through the nonlinear equations and generate persistent structural complexity. No memory or life is invoked; the patterns remain purely dynamical. The reader of the equations stands inside the same phase space that the equations describe, aligning with the Mirror Layer.

Sibling articles that carry related load appear at /a/oip-the-ladder and /a/oip-the-mirror-layer.

## Distance from the full synthesis
The memoir stays at the mechanistic tier of dynamical systems. It proves specific mathematical facts about integrals and orbit structure. It does not address memory formation, biological evolution, or mind. It therefore lies at moderate distance from the complete OIP/GRAIN synthesis. The synthesis uses the 1890 result as one concrete instance of bounded chaos that recurs across scales. Poincaré himself did not frame the result in those terms.

## Honest limits and disconfirming edges
The memoir does not solve the general three-body problem. It shows that certain series diverge and that qualitative behavior can be arbitrarily complex. Later work by Sundman (1912) produced a convergent series solution that is impractical for computation. Modern numerical methods confirm the existence of both chaotic and regular regions in phase space. The mathematical proofs rest on assumptions of analyticity and specific mass hierarchies; they do not extend automatically to every parameter regime. Reductionist objections in the style of Weinberg note that the complexity remains fully determined by the differential equations; no new ontological layer appears. The paper itself contains no empirical data from physical observations.

## Mechanistic claims
Claim c1 states that the memoir proves the non-existence of additional analytic first integrals for the general three-body problem. Tier: mechanistic. Source status: supported by secondary reconstructions.

Claim c2 states that the memoir identifies homoclinic tangles that produce sensitive dependence on initial conditions while keeping trajectories bounded. Tier: mechanistic.

Claim c3 states that these results constitute the first rigorous example of bounded chaos in a Newtonian gravitational system. Tier: mechanistic.

## What the evidence actually shows
The 1890 memoir supplies formal proofs within the framework of Hamiltonian dynamics. It does not contain numerical simulations or astronomical observations. Later numerical integrations of three-body systems reproduce the predicted sensitivity. The patterns remain confined to the mathematical model.

## What scientists say
Historians of mathematics credit the memoir with opening the qualitative theory of dynamical systems. Chenciner's review traces the development from the prize paper through the three volumes of Les méthodes nouvelles de la mécanique céleste. No scientist claims the work directly anticipates biological or cognitive patterns.

## What we do not know
The memoir leaves open the measure of the set of chaotic versus regular orbits for arbitrary masses. It provides no statement on the prevalence of these patterns in real solar-system dynamics beyond the restricted problem.

## Safety and limits
The work is a purely mathematical text. It carries no safety implications for physical systems or models. Its results remain valid only within the stated analytic and Hamiltonian assumptions.
