I don't really agree, by the way. Call it intuition. I think it will turn out that most planets in the "terrestroid" class, which includes Venus and Earth, do not have moons at all. Earth is weird because of the Theia collision (if you don't know about that, look it up; it's very interesting and generally accepted now as correct). Captures like Phobos and Deimos (Mars's moons) don't count because they are tiny and don't actually last for billions of years; they get perturbed or crash into the planet. Same with impact ejecta "moonlets" that may survive for a while but aren't real moons. And my "rule of thumb," even if correct, might not include a common class of planet that doesn't actually exist in the Solar System at all, Superearths.*Your proposed "rule of thumb" is pointing in a reasonable direction, but it needs two big caveats: (1) we still have essentially zero direct observational leverage on moons of terrestrial exoplanets, and (2) our own Solar System is a tiny sample, and it's "selection-biased" in the sense that we're sitting on the one terrestrial planet with a conspicuously large moon.
On the observational side: as of early 2026, no exomoon has been unambiguously confirmed, despite several candidates and a lot of effort. That matters because it means we cannot yet say, from data, whether "most rocky planets have no moons" is true in the broader galaxy. The non-detections so far are not very informative for terrestrial planets in particular, because the methods are strongly biased toward large moons around large planets on favorable orbits—exactly the regime where "if moons are there, they're easiest to see."
From theory and Solar System context, though, you can make a defensible, more careful statement:
Most terrestrial planets probably do not have large, Earth–Moon-scale moons.
That's different from "no moons at all." Tiny moons, temporary captures, quasi-moons, and small-body satellites may be common; what's probably uncommon is a big, dynamically important, long-lived satellite like ours.
The main pathways to moons don't favor big moons around rocky planets.Why that's a plausible generalization:
For terrestrial planets, the "obvious" way to get a large moon is a giant impact that leaves a debris disk which re-accretes into one (or a few) moons. Earth's Moon is the archetype. But giant impacts are chaotic: you need the right impact geometry, the right mass ratio, and the right angular momentum budget, and then you need the resulting satellite to survive long-term tidal evolution. In other words, it's a real channel, but it's not guaranteed.
Giant impacts are common in late-stage terrestrial formation, but "Moon-making" outcomes may be a subset.
Numerical work emphasizes that late terrestrial planet growth is dominated by giant impacts. That supports the idea that "Earth-like systems" might often get whacked hard. But "often hit hard" doesn't automatically translate into "often end up with a big moon"; many impacts will lead to accretion without a substantial long-lived satellite, or to multiple small remnants, or to outcomes that later get destabilized.
Our Solar System's terrestrial sample does lean toward 'moon-poor.'
Mercury and Venus have none; Earth has one large one; Mars has two tiny ones that are widely treated as captured or otherwise non-Earthlike in origin (your point). If you restrict the discussion to "major moons of the four terrestrial planets," you end up with basically one clear success case: Earth. That makes it tempting to say "Earth is the anomaly." It probably is an anomaly in moon-to-planet mass ratio, even if "impact-born moons" in general aren't vanishingly rare.So what I'd say, in plain terms, is this:
It's quite plausible that the typical terrestrial planet has either no moons or only small moons, and that large moons like ours are not the default outcome. But it is not yet something we can claim as an empirical rule across the universe, because (so far) exomoon detections are still unconfirmed and heavily biased toward big-planet systems rather than Earth analogs.
If you want a sharper prediction that's still honest, it would be: "Large moons around rocky planets exist, but are probably uncommon; small moons may be common." That's the version that fits both the Solar System pattern and what formation theory tends to suggest, without overclaiming beyond what we can currently observe.
*For those who actually find this stuff fascinating, here's some more on Superearths (usually spelled with a hyphen)(Also from Chat GPT), starting with a definition:
A planet more massive than Earth but substantially less massive than the Solar System's ice giants (Uranus and Neptune).
Quantitatively
Mass: ~1 to ~10 Earth masses (M⊕)The commonly used ranges are:
(Many researchers narrow this to ~1–5 M⊕.)
Radius: roughly ~1 to ~1.8 Earth radii (R⊕), though radius-based definitions vary.Above about 1.6–1.8 Earth radii, many planets are no longer likely to be predominantly rocky; they tend to retain significant volatile envelopes (H/He or thick water layers). That transition is sometimes called the "radius valley" or "Fulton gap."
Rocky super-Earths (≈1–1.6 R⊕, ≲5 M⊕)So in practice, people often distinguish:
Mini-Neptunes (≈1.6–3 R⊕, often with thick atmospheres)The boundary is fuzzy and observationally driven rather than conceptually clean.
It does not mean "Earth-like."What a super-Earth is not
It does not imply plate tectonics, oceans, or life.
It does not imply similar composition—some may be iron-rich, some water-rich, some gas-enveloped.Why the term exists
We don't have any super-Earths in our Solar System. The terrestrial planets top out at 1 M⊕ (Earth), and then there's a large jump to Uranus and Neptune (~14–17 M⊕). Exoplanet surveys revealed that planets in the 1–5 M⊕ range are extremely common—probably the most common type of planet in the galaxy.
So the term "super-Earth" arose simply to describe this very common mass regime that our own Solar System happens not to contain.
Super-Earths may form differently from Earth (for example, via inward migration in dense inner disks), which means the moon-formation story could be quite different from the Earth–Moon giant-impact scenario. That's still an open theoretical question rather than a settled rule.
where
e is the elementary charge (~1.602×10−19 C);
h is the Planck constant (~6.626×10−34 J⋅Hz−1);
ℏ is the reduced Planck constant, (h/2π (~1.055×10−34 J⋅s);
c is the speed of light in a vacuum(~300Km⋅s−1);
ε0 is the electrical permittivity of space (~8.854×10−12 F⋅m−1);
μ0 is the magnetic permeability of space (~1.2567×10−6 N⋅A−2).
As far as anyone knows, having no reason to suspect otherwise, this is and always has been and always will be true everywhere in the universe, but no one really knows why, if there is a why, this number has the value it does.

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