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The ModelEccentricity

Eccentricity

Eccentricity measures how elliptical Earth’s orbit is. A value of 0 is a perfect circle; higher values mean a more elongated ellipse. Earth’s current eccentricity is 0.01671022 — a nearly circular orbit.


What Eccentricity Means in Practice

The eccentricity value represents the offset distance between the centre of Earth’s orbit and the Sun, as a fraction of the semi-major axis (1 AU).

MeasurementValue
1 AU (mean Earth-Sun distance)149,597,870.698828 km
Eccentricity (J2000)0.01671022
Offset distance2,499,813 km
Perihelion distance147,098,057 km
Aphelion distance152,097,684 km
Difference4,999,627 km
  • At perihelion (closest, ~January 3): Earth is 147,098,057 km from the Sun.
  • At aphelion (farthest, ~July 4): Earth is 152,097,684 km from the Sun.
  • Earth receives about 6.9% more solar energy at perihelion than at aphelion.

The ~20,957-Year Cycle

Earth’s eccentricity oscillates in a ~20,957-year cycle — not the ~100k and ~400k-year cycles predicted by Milankovitch theory.

Earth and PERIHELION-OF-EARTH orbiting in opposite directions

Two motions work in opposite directions:

MotionDirectionPeriod
Earth around EARTH-WOBBLE-CENTERClockwise~25,794 years
PERIHELION-OF-EARTH around SunCounter-clockwise~111,772 years

Because they move in opposite directions, they meet more frequently than either cycle alone:

Meeting frequency = 1/~25,794 + 1/~111,772 = 1/~20,957

They meet every ~20,957 years — the perihelion precession cycle.

Why alignment affects eccentricity. Earth’s perihelion point defines where Earth’s closest approach to the Sun occurs. Earth itself orbits its wobble center at a small radius (~202,847 km). When Earth and its perihelion point are on the same side of the wobble center, their distances add → maximum eccentricity (~0.0167). When on opposite sides, the distances partially cancel → minimum eccentricity (~0.0140).


Eccentricity Values

ParameterValueNotes
Current eccentricity (J2000)0.01671022Measured, NASA Planetary Fact Sheet
Base eccentricity0.015386Arithmetic midpoint of the cycle (closely-related geometric mean √(e²base + A²) = 0.0154456)
Maximum~0.0167At December-solstice perihelion alignment
Minimum~0.0140At June-solstice perihelion alignment
Variation amplitude±0.001356Half the range
Cycle period~20,957 years335,317 ÷ 16

The base value (0.015386) cannot be measured directly because we only have observations from recent centuries. It was derived from three constraints: minimum eccentricity occurred in ~9,233 BC when perihelion aligned with the June solstice; maximum occurred in 1246 AD when perihelion aligned with the December solstice; current eccentricity (0.01671022) is near the maximum and decreasing. The 3D simulation was calibrated to satisfy all three.


The Solstice Connection

Eccentricity extremes correlate with solstice alignments:

AlignmentEccentricityLast occurrenceNext occurrence
Perihelion at December solsticeMaximum (~0.0167)1246 AD~22,203 AD
Perihelion at June solsticeMinimum (~0.0140)~9,233 BC~11,725 AD

When perihelion aligns with the December solstice (Northern Hemisphere winter), Earth and its perihelion point are positioned such that their orbital offsets add. When aligned with the June solstice, they partially cancel.

Graph showing Earth's eccentricity oscillating between minimum and maximum over one eccentricity cycle, with maximum at December solstice alignment

We passed maximum eccentricity around 1246 AD. The current value (0.01671022) is decreasing toward the mean; it will reach minimum (~0.0140) around 11,725 AD and return to maximum around 22,203 AD.


Why Not Milankovitch’s 100k/400k Cycles?

Conventional Milankovitch theory proposes eccentricity cycles of ~100k and ~400k years. The model proposes a simpler ~20,957-year cycle instead. Five open questions in the conventional eccentricity theory:

QuestionDetails
1. The “~100k” simplificationMilankovitch’s calculations give ~95k and ~125k cycles. The commonly cited “~100k” is the combined quasi-periodic effect of these two components (and harmonics like ~99k from g₃−g₅), not a single physical cycle.
2. The 100,000-year problem Geological records show a dominant ~100k pattern but no clear ~400k periodicity — despite the ~400k eccentricity cycle being the strongest in theory. A recognised unsolved problem in paleoclimatology.
3. The energy problemEccentricity changes affect total annual insolation by only ~0.2%. How this small signal drives major glacial cycles remains debated — most proposals invoke amplification mechanisms (ice-albedo feedback, CO₂ feedbacks).
4. Modeled vs observedThe ~95k, ~125k, and ~405k cycles are derived from secular perturbation models — they are beat frequencies between planet-pair eigenmodes (95k = g₄−g₅; 125k = g₄−g₂; 405k = g₂−g₅), not directly measured in the geological record. The Mars/Venus/Jupiter labels on g_j are Berger’s convention; the Holistic model accepts the eigenmodes as math objects but does not endorse the single-planet attribution (see Eigenfrequencies).
5. Inclination precessionEarth’s orbital inclination precesses at ~67,063 years (vs ecliptic) or ~111,772 years (vs ICRF). This cycle was not part of Milankovitch’s original framework and is not included in standard eccentricity calculations, though it may contribute to the observed ~100k signal.

The 100-kyr cycle in ice cores is a multi-planet eigenmode-beat signal, not direct eccentricity forcing. Empirical analysis on LR04 places the energy-weighted centroid at the s₁ − s₄ nodal eigenmode beat at n = 25 = 107.3 kyr, with adjacent contributions at n = 28 = 95.8 kyr (g₄ − g₅ eccentricity, Berger’s 95-kyr peak) and n = 22 = 121.9 kyr (s₂ − s₄ nodal). The 405-kyr g₂−g₅ term is essentially absent in post-MPT LR04 (amplitude ratio 0.12); bispectral analysis finds no significant 95k+125k phase coupling. Earth’s own H/3 inclination precession (n = 24) is a real cycle on the 8H lattice but does not directly drive climate — the L1 fit places near-zero amplitude there. Full empirical case: Climate Formula.


Comparison with Standard Formulas

The model’s eccentricity predictions are compared with polynomial formulas from Newcomb (1898), Harkness (1891), and Meeus (1998). All four converge at J2000 (e = 0.01671022). Standard polynomials predict continued decrease toward ~0.01 by 20,000 AD; the model predicts bounded oscillation within ~0.0140~0.0167 with minimum at ~11,725 AD followed by increase.

Eccentricity predictions compared: this model (purple) versus Newcomb (1898, blue), Harkness (1891, red), and Meeus (1998, green). All converge at J2000.

The graph below shows both predictions over 300,000 years. The model’s ~20,957-year cycle (blue) oscillates within a narrow bounded range of ~0.0140~0.0167 around a base value of 0.015386 (red). Standard Milankovitch eccentricity (grey) varies over much larger amplitudes (up to ~0.06) on ~100k and ~400k-year timescales.

Graph comparing the model's bounded eccentricity cycle (blue) against the standard Milankovitch eccentricity variation (grey) over several hundred thousand years

The two predictions diverge significantly: the model predicts eccentricity never leaves its narrow band; standard theory predicts it has varied by a factor of ~4 over the past 200,000 years. Since direct measurements only cover recent centuries, neither prediction can be verified for deep time — but they offer testable, fundamentally different forecasts.

Saturn coupling — an additional effect

The eccentricity curve above reflects only Earth’s own ~20,957-year perihelion cycle. Saturn’s eccentricity is independently predicted by Law 5 — the global eccentricity balance equation determines Saturn’s value from the other seven planets to 0.27%. The two predictions are not independent: Saturn participates in the same balance system that includes Earth, so changes in Earth’s eccentricity feed into Saturn’s via Law 5.

The physical Earth–Saturn coupling comes from Saturn being the only planet whose precession formula requires Earth’s time-varying obliquity and eccentricity as inputs (GROUP 15 terms; see Formulas), and from Saturn’s perihelion cycle (−8H/65 = 41,270 years, ecliptic-retrograde) coinciding with Jupiter’s ICRF perihelion — the gas-giant lock that drives Earth’s obliquity (Law 6). Saturn’s axial precession (~1.8 Myr, driven by a spin-orbit resonance with Neptune; Saillenfest et al. 2021) is unrelated.

Both the model’s predictions and standard Milankovitch predictions for ancient or future eccentricity are theoretical. Neither can be directly verified for times before ~1900 AD.

Numerical comparison: Model vs La2004

YearLa2004ModelDifference
5,000 AD0.015340.016020.00068
11,725 AD0.01156~0.0140 (minimum)0.00247
27,000 AD0.00263 (near min)0.015620.01299

These differences are significant but require geological timescales to verify directly. See Climate Formula: eccentricity attribution headwinds for the three discriminating empirical tests (405-kyr absence, bispectrum, wrong-family centroid).


Climate Implications

Eccentricity affects Earth’s climate through two mechanisms:

Total annual energy. Higher eccentricity gives Earth slightly more total annual solar energy. Orbit-averaged flux scales as 1/√(1−e²); perihelion’s intense, close-range flux more than compensates for the longer time spent near aphelion.

EccentricityEffect on annual insolation
Maximum (~0.0167)~0.014% more than circular
Minimum (~0.0140)~0.010% more than circular
Difference~0.004%

This effect is small — too small alone to cause ice ages.

Seasonal contrast. The more important effect is when perihelion occurs relative to seasons:

Perihelion timingNorthern Hemisphere effect
January (current)Milder winters, cooler summers
June (~11,725 AD)Hotter summers, colder winters

Eccentricity Cycles for Other Planets

The same two-counter-rotating-motion principle applies to every planet. Each planet has its own wobble period — the meeting frequency of its axial precession and ICRF perihelion precession — the period over which its eccentricity completes one full oscillation:

PlanetWobble periodH expression
Mercury31,935 yr2H/21
Venus141,186 yr8H/19
Earth~20,957 yrH/16
Mars51,587 yr8H/52
Jupiter60,967 yr8H/44
Saturn16,457 yr8H/163
Uranus33,532 yr≈H/10
Neptune26,825 yr≈2H/25

For Earth the wobble period coincides with the perihelion precession period (H/16) because axial precession (H/13) and ICRF perihelion precession (H/3) meet at this rate (13 + 3 = 16). For other planets the two component periods are different, so the wobble period is a derived beat frequency.

The wobble period (eccentricity cycle) is NOT the same as the perihelion ecliptic period. For Earth they coincide; for other planets they differ. The 3D simulation’s Solar System Resonance Cycle panel shows all six cycle types per planet (axial, perihelion ecliptic, ICRF, ascending node, obliquity, eccentricity) — each as an integer divisor of 8H.


Calculate Eccentricity at Any Year

See Formulas for the complete formulas.


Summary

AspectValue
Current eccentricity0.01671022 (decreasing)
Cycle period~20,957 years (H/16)
Range~0.0140 to ~0.0167
Maximum alignmentPerihelion at December solstice
Minimum alignmentPerihelion at June solstice
Last maximum1246 AD
Next minimum~11,725 AD
Climate connection100-kyr cycle is multi-planet eigenmode beats, not direct eccentricity — see Climate Formula

Continue to Days & Years to learn how these cycles affect the length of our days and years.

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