L57 Reiner Gamma

A bright, swirling smear of high-albedo material with no shadow at any lighting angle, sitting atop one of the strongest localized magnetic anomalies on the Moon — likely a case of magnetic shielding preserving unweathered soil in place.

Coordinates7.4°N, 59.0°W
Optimal ViewingHigh/Full Sun (~Day 14–15); no terminator needed
Target TypeLunar Swirl / Magnetic Anomaly
Extent~30 × 60 km (bright core)

Source: IAU/Gazetteer & Sky & Telescope Lunar 100 (Wood, 2004)

L57 Reiner Gamma-lunar-100-map-coordinates

L57 Reiner Gamma

Oceanus Procellarum · Lunar Swirl

📉 Vital Statistics

Feature Type Lunar swirl / crustal magnetic anomaly
Core Extent ~30 × 60 km bright core, with tendrils reaching further
Coordinates ~7.4°N, 59°W (301°E)
Magnetic Field ~15 nT at 28 km altitude — one of the strongest on the Moon
Named For Nearby crater Reiner (Vincentio Reinieri)
Origin Bright swirl likely from magnetic shielding; the anomaly’s own origin is debated
L100 Distinction The Moon’s most famous swirl and one of its strongest localized magnetic anomalies

🔭 Field Notes

Reiner Gamma is a bright, swirling smear of high-albedo material sitting in the dark basalt of western Oceanus Procellarum, near the small crater Reiner. It’s one of the most visible lunar swirls from Earth, easily picked out in almost any backyard telescope — but what makes it strange is what you won’t see: no rim, no bowl, no shadow at any lighting angle. Early observers initially mistook it for a highland patch or even a crater, until it became clear the feature casts no shadow whatsoever, meaning it has no topography of its own. It’s pure brightness contrast laid flat across the mare, tied to one of the strongest local magnetic fields anywhere on the Moon.

  • A Feature With No Relief: Unlike nearly everything else in the Lunar 100, Reiner Gamma is identified purely by albedo, not shape. Its bright, concentric, swirling pattern shows no corresponding rise, depression, or ridge under any illumination — a genuine oddity among lunar surface features, most of which reveal themselves through shadow and relief.
  • Two Competing Origin Stories: The bright swirl itself is most likely explained by magnetic shielding: a strong local magnetic field deflects the solar wind, reducing the space weathering that normally darkens exposed lunar soil over time, leaving the shielded surface optically brighter than its surroundings. What remains genuinely debated is the origin of the underlying magnetic anomaly — proposed sources include remanent magnetization tied to an ancient impact, buried intrusive rock bodies, or other deep crustal structures. One older, less favored hypothesis proposed that a cometary impact both disturbed the surface and generated or enhanced the local magnetization directly, but this is now a minority view rather than a serious competitor to the shielding model.
  • One of the Strongest Anomalies on the Moon: Reiner Gamma’s magnetic field, measured at roughly 15 nanotesla from an altitude of 28 km, is among the strongest localized crustal magnetic signatures found anywhere on the Moon. It was first mapped from orbit by Apollo-era subsatellite magnetometers, which found the anomaly correlated almost exactly with the visible bright marking — a rare, clean link between a surface albedo feature and a specific magnetic source that still isn’t fully explained.

📍 Nearby L100 Targets

  • L42 Marius Hills: The Moon’s densest concentration of volcanic domes and cones, roughly 280 km northeast, spread across a plateau in the same stretch of Oceanus Procellarum. The pairing makes a striking contrast in the same wide field of view: one target defined entirely by subtle relief under low sun, the other showing no relief at all under any light.
  • L36 Grimaldi Basin: An ancient, heavily degraded impact basin roughly 480 km southwest, with one of the darkest floors on the Moon. Grimaldi and Reiner Gamma sit at opposite ends of the same albedo spectrum — the darkest major surface nearby paired with one of the brightest — both within easy reach of the same observing session.
  • L68 Flamsteed P: A large, mostly buried ghost crater roughly 560 km southeast, its ring reduced to scattered ridges by mare flooding, best known as the landing site of Surveyor 1 in 1966. Its geological history involves extensive volcanic flooding and modification, a debate that echoes the same open questions surrounding Reiner Gamma’s own formation.

🚀 Mission Log

Apollo Subsatellite Magnetometers, including PFS-2 (NASA, 1971–1972) Magnetometer-equipped subsatellites released from the Apollo 15 and 16 command modules, including Apollo 16’s PFS-2, provided among the first orbital measurements directly mapping the strong crustal magnetic anomaly correlating with Reiner Gamma’s bright surface marking.
Clementine (NASA/BMDO, 1994) Multispectral imaging documented the swirl’s distinctive high-albedo, optically immature surface in detail, providing key data for later studies comparing its brightness pattern against the magnetic field maps built from orbital and subsatellite measurements.
Lunar Reconnaissance Orbiter (NASA, 2009–present) NAC-controlled mosaics have mapped Reiner Gamma’s swirl pattern down to meter-scale detail, revealing tendrils extending hundreds of kilometers beyond the bright core and informing planning for future close-up study of the anomaly.
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Target Acquisition

1

Find the crater Reiner, then look just west

Start at Reiner, a sharp 30 km bowl crater in western Oceanus Procellarum, easy to pick out against the dark mare basalt. Look just to its west for a bright, swirling smear with no rim, no bowl, and no shadow at any lighting angle — that’s Reiner Gamma, named simply for its neighboring crater.

2

Skip the terminator — this target wants direct sunlight

Reiner Gamma is one of the rare Lunar 100 targets that doesn’t depend on a low, raking terminator. Since it’s a pure albedo marking with no topography of its own, it actually shows up best under high or full Sun, when direct illumination maximizes the brightness contrast between the swirl and the surrounding mare. A low terminator won’t hide it, but it won’t help either — this is one case where waiting for more direct light pays off rather than working against you.

3

Work up in power to trace the tendrils beyond the bright core

At 100x–150x, look past the swirl’s dense central knot for the fainter tendrils and loops that extend further out into the mare. Check carefully for any shadow at all along the swirl’s edges — you won’t find one, and that absence is the whole point. It’s one of the few Lunar 100 targets identified largely by the total lack of the shadow-and-relief cues you’d use almost everywhere else in this guide.

4

Pair it with the domes, the basin, and the ghost crater nearby

Roughly 280 km northeast, the Marius Hills (L42) pack the Moon’s densest cluster of volcanic domes into the same stretch of Oceanus Procellarum — a striking contrast between subtle relief under low sun and Reiner Gamma’s complete lack of relief under any light. Roughly 480 km southwest, Grimaldi Basin (L36) sits at the opposite end of the same albedo spectrum, one of the darkest floors on the Moon paired here with one of its brightest markings. And roughly 560 km southeast, Flamsteed P (L68), the mostly buried ghost crater where Surveyor 1 touched down in 1966, has a geological history shaped by extensive volcanic flooding — a fitting neighbor for a feature whose own origin is still being worked out.

💡 Observer’s Tip: Early observers initially mistook Reiner Gamma for a highland patch or even a crater, until it became clear the feature casts no shadow whatsoever under any illumination. Apollo-era subsatellite magnetometers later found the swirl sits atop one of the strongest localized magnetic anomalies on the Moon — a correlation thought to be the leading explanation for why the surface stays bright here, since a strong local field can shield the ground from the slow darkening caused by the solar wind.

📝 Observation Log — L57 Reiner Gamma

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Is Reiner Gamma visible tonight?

Reiner Gamma sits in western Oceanus Procellarum at 7.4°N, 59.0°W, just west of the crater Reiner. Best viewing is around Waxing Gibbous to Full Moon (roughly Day 12–15) — unusually for this list, this target wants high or full Sun rather than a low terminator, since it’s a pure albedo marking with no shadow-casting relief at any lighting angle. Libration is not a meaningful factor at this longitude.

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When to Observe Reiner Gamma

Reiner Gamma breaks nearly every rule this list otherwise follows. It has no topography of its own, so for once, you’re not waiting for a low terminator — you’re waiting for the opposite.

  • For the Swirl: You need high or full Sun. Reiner Gamma is a pure albedo marking with no shadow-casting relief at any lighting angle, so direct illumination maximizes the brightness contrast between the swirl and the surrounding mare. A low terminator won’t hide it, but it won’t help either.
  • For Orientation: Anchor on Reiner, a sharp 30 km bowl crater in western Oceanus Procellarum. Look just to its west for the bright, swirling marking with no rim and no bowl — Reiner Gamma, named simply for its neighboring crater.
  • Aperture and Seeing: Moderate power confirms the dense central knot; higher power and steady seeing help trace the fainter tendrils extending further out into the mare.

What to Look For

1 No Shadow at Any Lighting Angle

Check carefully around the swirl’s boundary for any shadow at all. You won’t find one, and that absence is the whole point — the swirl itself never produces shadows that define its shape, making it one of the few Lunar 100 targets identified largely by the total lack of the shadow-and-relief cues you’d use almost everywhere else in this guide.

Challenge: Revisit the same field under two very different lighting conditions and confirm for yourself that the swirl’s brightness contrast changes, but no shadow ever appears at either extreme.
2 Tendrils Beyond the Bright Core

Look past the swirl’s dense central knot for the fainter tendrils and loops that extend further out into the surrounding mare.

Challenge: See how far you can follow a single tendril before it fades into the mare — high-resolution orbital imagery has traced these loops for hundreds of kilometers beyond the core.
3 One of the Strongest Magnetic Anomalies on the Moon

Nothing at the eyepiece hints at this directly, but Reiner Gamma sits atop a crustal magnetic field measured at roughly 15 nanotesla from an altitude of 28 km — among the strongest localized magnetic signatures found anywhere on the Moon.

4 A Feature Early Observers Misread

Early observers initially mistook Reiner Gamma for a highland patch or even a crater, until later observations demonstrated the feature casts no shadow whatsoever under any illumination — a mistake that’s easy to understand once you’ve tried to find topography here yourself and come up empty.


The Science: A Bright Mark With No High Ground

Reiner Gamma is one of the Moon’s clearest cases of a surface feature explained not by geology in the usual sense, but by physics acting on geology — a magnetic field quietly protecting the ground beneath it from the slow processes that darken everything around it.

Magnetic Shielding From Space Weathering

The bright swirl itself is most likely explained by magnetic shielding: a strong local magnetic field deflects the solar wind, reducing the space weathering that normally darkens exposed lunar soil over time, leaving the shielded surface optically brighter than its surroundings. This is now the leading explanation for swirls like Reiner Gamma.

The Anomaly’s Own Origin Remains Debated

What’s genuinely unresolved is the source of the underlying magnetic anomaly itself. Proposed explanations include remanent magnetization tied to an ancient impact, buried intrusive rock bodies, or other deep crustal structures. Apollo subsatellite magnetometers provided among the first orbital measurements directly mapping the anomaly and confirming its close correlation with the visible bright marking.

What Hasn’t Been Resolved

A correlation this precise between a surface albedo feature and a specific magnetic source is rare, and it’s still not fully explained why the magnetic field maps so cleanly onto the swirl’s shape rather than a more diffuse or offset pattern. An older hypothesis proposing that a cometary impact both disturbed the surface and generated the local magnetization directly now receives relatively little support compared to the shielding model.

Most Lunar 100 targets show you their history through shape. Reiner Gamma shows you nothing but brightness, and asks you to accept that an invisible magnetic field, mapped only by spacecraft, is the reason a patch of mare basalt still looks freshly exposed after billions of years. Unlike bright ray systems, which trace back to an obvious source crater, Reiner Gamma has no central impact crater from which the bright material could have originated — one more reason it puzzled observers for as long as it did.

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