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Last updated July 30, 2025

The Nice Model: Towards an Explanation of the Late Heavy Bombardment

Simulation of the Nice model

A Dynamic Reorganization of the Solar System

At the beginning of the 21st century, a group of astrophysicists from the Observatory of the Côte d'Azur in Nice proposed a revolutionary scenario to explain the current distribution of the planets, the structure of the asteroid belt, and the origin of the late heavy bombardment (LHB): the Nice model.

This model postulates that after the dissipation of the protosolar gas disk, the giant planets (Jupiter, Saturn, Uranus, Neptune) migrated due to gravitational interactions with a vast population of small icy bodies, initially confined beyond Neptune's orbit.

The Initial Configuration of the Giant Planets

A more compact architecture of the solar system

In the initial version of the Nice model, the giant planets did not occupy the positions they have today. They were closer to each other, forming a compact and almost circular structure. Jupiter, Saturn, Uranus, and Neptune evolved in slightly eccentric orbits, with respective orbital radii of about 5.5 AU, 8 AU, 11 AU, and 14 AU from the Sun. This system was initially stable, without major cross-interactions.

A disk of planetesimals beyond Neptune

At that time, a massive disk of small bodies (icy planetesimals) extended beyond Neptune's orbit, between 15 and 35 astronomical units. This disk contained up to 30 Earth masses of material, representing a major dynamic source for gravitational interactions with the outer planets.

A system in precarious balance

Although seemingly stable, this configuration contained the seeds of instability. The slow but continuous gravitational interactions between the planets and the planetesimals gradually modified the orbital parameters of the planets. When Jupiter and Saturn approached an orbital resonance (2:1), a brutal reorganization began, initiating planetary migration and the events that followed. This slow orbital coupling would lead to a sudden dynamic shift: the planetary instability triggered by a mutual resonance.

This initial phase, which precedes the orbital upheaval, is crucial for understanding the subsequent events: planetary migration, the diffusion of small bodies, and the late heavy bombardment.

Evolution of the orbits of the giant planets in the Nice model

Evolution of the orbits of the giant planets in the Nice model

Dynamic Instability and Resonances

When Jupiter and Saturn reach a 2:1 orbital resonance (the ratio of their periods becomes 2 to 1), a major gravitational instability is triggered. This configuration strongly disrupts the orbits of Uranus and Neptune, which are then projected outwards. They cross the belt of planetesimals, causing the dispersion of billions of icy objects throughout the inner and outer Solar System.

The Late Heavy Bombardment (LHB)

This sudden displacement would have led to a period of massive collisions on the terrestrial planets, particularly the Moon, Mars, and Earth, about 700 million years after the formation of the Solar System. This phase, identified through radiometric dating of lunar rocks brought back by the Apollo missions, is known as the late heavy bombardment, dated around 3.9 billion years ago.

It is notably correlated with the creation of many lunar impact basins such as Imbrium or Orientale. This phenomenon could also have contributed to the late delivery of water and organic matter to Earth.

Extensions and Validations of the Model

Since its initial formulation in 2005, the Nice model has been refined (Nice II, Nice III) to integrate effects such as the gravitational friction of the residual gas disk, interactions between massive planetesimals, or the hypothesis of a fifth giant planet ejected.

Numerical simulations, correlated with observations of trans-Neptunian objects (TNOs), confirm the effectiveness of the model in explaining the eccentric and inclined orbits of many small planets, such as Sedna or Eris.

Comparative table of dynamic consequences

Dynamic effects of planetary migration
PhenomenonObserved consequenceGeological or orbital evidenceSource
Jupiter-Saturn resonanceGravitational instabilityNumerical model (res. 2:1)Morbidelli et al., 2005
Migration of Uranus and NeptuneRearrangement of the Kuiper BeltOrbital distribution of TNOsLevison et al., 2008
Dispersion of planetesimalsLate Heavy BombardmentDating of lunar rocksTera et al., 1974
Possible planetary ejectionInstability reduced to 4 giantsNumerical simulationsNesvorný, 2011
Capture of Trojan asteroidsPresence of co-orbital objects of JupiterL4 and L5 populations (asymmetries, sizes)Morbidelli et al., 2005
Inclination of trans-Neptunian disk objectsEccentric and inclined orbitsTNOs with high inclinations and periheliaGomes et al., 2005
Restructuring of the asteroid beltDepletion and orbital excitationCurrent low total massMinton & Malhotra, 2009
Stabilization of the inner solar systemFinal alignment of planetary orbitsCurrent stable architectureTsiganis et al., 2005

References: Morbidelli et al., Nature, 2005, Levison et al., Icarus, 2008, Tera et al., Science, 1974, Nesvorný, ApJ, 2011.

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