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).
| Measurement | Value |
|---|---|
| 1 AU (mean Earth-Sun distance) | 149,597,870.698828 km |
| Eccentricity (J2000) | 0.01671022 |
| Offset distance | 2,499,813 km |
| Perihelion distance | 147,098,057 km |
| Aphelion distance | 152,097,684 km |
| Difference | 4,999,627 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.
Two motions work in opposite directions:
| Motion | Direction | Period |
|---|---|---|
| Earth around EARTH-WOBBLE-CENTER | Clockwise | ~25,794 years |
| PERIHELION-OF-EARTH around Sun | Counter-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
| Parameter | Value | Notes |
|---|---|---|
| Current eccentricity (J2000) | 0.01671022 | Measured, NASA Planetary Fact Sheet |
| Base eccentricity | 0.015386 | Arithmetic midpoint of the cycle (closely-related geometric mean √(e²base + A²) = 0.0154456) |
| Maximum | ~0.0167 | At December-solstice perihelion alignment |
| Minimum | ~0.0140 | At June-solstice perihelion alignment |
| Variation amplitude | ±0.001356 | Half the range |
| Cycle period | ~20,957 years | 335,317 ÷ 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:
| Alignment | Eccentricity | Last occurrence | Next occurrence |
|---|---|---|---|
| Perihelion at December solstice | Maximum (~0.0167) | 1246 AD | ~22,203 AD |
| Perihelion at June solstice | Minimum (~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.
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:
| Question | Details |
|---|---|
| 1. The “~100k” simplification | Milankovitch’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 problem | Eccentricity 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 observed | The ~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 precession | Earth’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.
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.
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
| Year | La2004 | Model | Difference |
|---|---|---|---|
| 5,000 AD | 0.01534 | 0.01602 | 0.00068 |
| 11,725 AD | 0.01156 | ~0.0140 (minimum) | 0.00247 |
| 27,000 AD | 0.00263 (near min) | 0.01562 | 0.01299 |
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.
| Eccentricity | Effect 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 timing | Northern 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:
| Planet | Wobble period | H expression |
|---|---|---|
| Mercury | 31,935 yr | 2H/21 |
| Venus | 141,186 yr | 8H/19 |
| Earth | ~20,957 yr | H/16 |
| Mars | 51,587 yr | 8H/52 |
| Jupiter | 60,967 yr | 8H/44 |
| Saturn | 16,457 yr | 8H/163 |
| Uranus | 33,532 yr | ≈H/10 |
| Neptune | 26,825 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
| Aspect | Value |
|---|---|
| Current eccentricity | 0.01671022 (decreasing) |
| Cycle period | ~20,957 years (H/16) |
| Range | ~0.0140 to ~0.0167 |
| Maximum alignment | Perihelion at December solstice |
| Minimum alignment | Perihelion at June solstice |
| Last maximum | 1246 AD |
| Next minimum | ~11,725 AD |
| Climate connection | 100-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.