Oct. 25, 1671: Iapetus is discovered

In 1669, French-Italian astronomer Giovanni Cassini arrived at the still-under-construction Paris Observatory as its new director. He quickly talked Louis XIV’s minister of finance into buying a 34-foot Campani refractor for the observatory, and on Oct. 25, 1671, used that refractor to discover Saturn’s moon Iapetus. The second saturnian moon discovered, after Christaan Huygens’ 1655 Titan find, Iapetus appeared brighter at some parts of its orbit and darker at others. Cassini also noted that he could only see the moon on the west side of Saturn; from that information, he was able to correctly deduce that Iapetus has one side with a far dark albedo than the other, and that the moon is tidally locked with Saturn. Scientists speculate that one face of Iapetus is murkier in color because eruptions of hydrocarbons at the surface, or because it may be picking up detritus from darker moon Phoebe.

Cassini had a long and productive astronomical career, during which he improved instruments and discovered, observed, and measured many new celestial bodies. Among these were not just Iapetus, but also the third, fourth, and fifth moons of Saturn: Rhea, Dione, and Tethys. After Cassini’s 1684 Tethys discovery, it would be over 100 years before William Herschel spotted the fifth one, Mimas. Today we know of 274 saturnian moons.


Elisa Neckar is senior production editor of Astronomy magazine, and the editor of the Today in the History of Astronomy feature on Astronomy.com.

The Sky Today on Sunday, October 25: Dione crosses Saturn

Looking for a sky event this week? Check out our full Sky This Week column. 

October 24: Mercury stands still

Saturn’s small moon Dione transits the disk this evening at 8:43 p.m. EDT, best seen from the eastern half of the U.S. However, the transit itself will be difficult to watch visually no matter your location, and will be best captured via high-speed video. Even if you aren’t an advanced photographer, however, you can watch Dione enter and exit the disk, as well as track several of Saturn’s other moons throughout the night. 

Around 9 P.M. EDT (8 P.M. CDT), Saturn is well above the horizon, in the east for Midwestern observers and the southeast for those along the East Coast. It’s the brightest point of light in this part of the sky and should be visible to the naked eye even with the Moon nearby. You’ll need a telescope to spot its rings and moons, however, and the larger the better to help cut through the Moon’s glare. Prior to the transit’s start, 10th-magnitude Dione is approaching the planet’s northeastern limb, with similarly bright Tethys east of the rings and Rhea to their west. Brighter Titan, which shines around magnitude 8.5, is also visible far west of Saturn all evening, about 2’ from the planet’s center. 

As Dione begins its transit, it will likely seem to disappear for visual observers, as its tiny disk will be difficult to pick out against Saturn’s bright cloud tops. Video capture might also nab the moon’s shadow, which will cross the far northern polar region of the planet, appearing around 9:40 P.M. EDT and disappearing roughly half an hour later, before Dione reaches the northwestern limb. The moon does this just before 10:40 P.M. EDT — now, visual observers will see it pop into view just off the limb and begin pulling away from Saturn to the west. 

Sunrise: 7:22 A.M.
Sunset: 6:06 P.M.
Moonrise: 5:33 P.M.
Moonset: 6:46 A.M.
Moon Phase: Full
*Times for sunrise, sunset, moonrise, and moonset are given in local time from 40° N 90° W. The Moon’s illumination is given at 10 P.M. local time from the same location. 


Alison Klesman is senior editor of Astronomy magazine. She holds a Ph.D. in astronomy and has studied a variety of topics, from minor planets to supermassive black holes.

Oct. 24, 1601: The death of Tycho Brahe

In Astronomy’s 2022 list of the 20 greatest astronomers of all time, Associate Editor Michael Bakich ranked Tycho Brahe No. 2, second only to Galileo, noting: “Danish astronomer Tyge (Tycho) Ottesen Brahe was history’s greatest pre-telescopic observer.”

Born Dec. 14, 1546, Tycho was raised by an uncle who funded his education at the University of Leipzig. There, he discovered that most existing publications of stellar and planetary positions were hugely inaccurate, and decided to devote his life to rectifying this problem. Among the career highlights that prompted Bakich to rank him so high: “Although Brahe didn’t have a telescope, he constructed many observing instruments: several quadrants, an armillary sphere, a sextant, and a large globe. Two of his famous observations were of the supernova that appeared in 1572 (now called Tycho’s Nova) and the Great Comet of 1577. When he measured their positions, he saw no parallax, meaning that their distances placed them beyond the Moon.”

Tycho died Oct. 24, 1601, in Prague, leaving his data to his protégé, Johannes Kepler. His careful observations allowed Kepler to determine the laws of planetary motion; these laws, in turn, became the basis for the work of Isaac Newton.


Elisa Neckar is senior production editor of Astronomy magazine, and the editor of the Today in the History of Astronomy feature on Astronomy.com.

The Sky Today on Saturday, October 24: Mercury stands still

Looking for a sky event this week? Check out our full Sky This Week column. 

October 23: Nab Neptune near the Moon

Mercury reaches a stationary point in Libra at 8 A.M. EDT. The tiny planet is only briefly visible after sunset, but if you’ve got a clear horizon, give it a try. Look west roughly 20 to 30 minutes after sunset, and scan for a magnitude 0.5 point of light just above the horizon. Mercury is 2.5° high in the southwest 20 minutes after sunset, and 1° high in the west 10 minutes later. You may want to try sweeping the area slowly with binoculars, but make sure the Sun has set completely below the horizon before pulling out any optical aid. Mercury’s disk stretches 9” across and the planet is 28% lit if you can catch it through a telescope. 

Today’s standstill marks an end to Mercury’s prograde, or eastward, movement. After this, it will begin tracking westward, or retrograde, heading back past Alpha (α) Librae in just a few days and crossing into Virgo in early November, joining Venus. 

Sunrise: 7:21 A.M.
Sunset: 6:07 P.M.
Moonrise: 5:05 P.M.
Moonset: 5:35 A.M.
Moon Phase: Waxing gibbous (98%)
*Times for sunrise, sunset, moonrise, and moonset are given in local time from 40° N 90° W. The Moon’s illumination is given at 10 P.M. local time from the same location. 


Alison Klesman is senior editor of Astronomy magazine. She holds a Ph.D. in astronomy and has studied a variety of topics, from minor planets to supermassive black holes.

Announcing the winners of Astronomy Magazine’s 2026 Astrophotography Contest

Astronomy magazine is proud to announce the winners of its 2026 Astrophotography Contest, presented by Celestron — the magazine’s first photo contest in 13 years.

More than 1,400 entries poured in from photographers around the world, with images ranging from faint nebulae and stunning planetary close-ups to dramatic solar images and beautiful nightscapes. As astroimaging has grown more advanced since our last photo contest, it has also become more accessible, and this year we strove to open the contest to as many imagers as possible. The Smartscopes category let imagers using all-in-one devices compete on a level playing field. Our Newcomer category was open to photographers ages 13 to 17 or anyone with fewer than two years of experience. And in the Processing category, you didn’t need imaging gear at all: every entrant worked from the same free Telescope Live dataset.

The magazine’s editors chose the grand prize winner, eight category winners, and 22 runners-up with a panel of guest judges: Contributing Editors Tony Hallas, Molly Wakeling, and Michael Bakich; planetary imager Damian Peach; and Editor Emeritus Dave Eicher.

See every winner and runner-up in our winners gallery.

Grand Prize: “The Dementors of Cepheus,” by Julien De Winter, Landon Boehm, and Brian Diaz

A pair of shadowy, wraithlike figures weave their way through a grand tapestry of stellar life and death in our grand-prize-winning image. The imagers refer to them as the “Dementors of Cepheus” — a reference to the wardens of the prison Azkaban in the Harry Potter series. Here, they guard not convicts, but a corpse: The filaments of gas in the center of the frame are the remnants of a supernova, cataloged as SNR G110.3+11.3, that blew apart a massive star.

Judges called this image “sensational” and “impressive.” Astronomy Contributing Editor Molly Wakeling praised its composition and also its sense of depth — one of the things she looks for in a good astrophotograph. “If you can get that 3D feel to it, that’s when you know you’ve made it.”

The team wins a Celestron RASA 8 astrograph.

Photo data: November 2025–January 2026 · Starfront Observatories, Rockwood, Texas · 7-inch Takahashi Epsilon-180ED astrograph at f/2.8 · ZWO ASI6200MC Pro and ASI6200MM Pro cameras · 29.6 hours of total exposure (broadband 19¾ hours, Hα 9.8 hours with Antlia 3nm filter) · Credit: Julien De Winter; Landon Boehm; Brian Diaz

Category winners

  • Deep Sky — Broadband: Prasaad Milner, the Blue Horsehead Nebula and Rho Ophiuchi cloud complex
  • Deep Sky — Narrowband: Emmanuel Joly, the Sharpless 2-115 complex in Cygnus
  • Solar System Objects: Simon Labergère, Saturn with Titan and Tethys
  • Solar Imaging: Mehmet Ergün, the active Sun in hydrogen-alpha
  • Nightscapes: Tom Rae, the Milky Way over Aoraki/Mount Cook National Park, New Zealand
  • Smartscopes: Nathanael Martin, the Angel Nebula (NGC 2170)
  • Processing: Marius Dinga, RCW 38
  • Newcomer: Andy Garrett, the Rosette Nebula

The December 2026 issue of Astronomy has full captions for each winning image, along with profiles of the photographers. Subscribe so you don’t miss it.

Congratulations to all our winners, and thank you to everyone who submitted an image to the contest.


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2026 Full Moon calendar: When to see the Full Moon and phases

The phenomenon of a Full Moon arises when our planet, Earth, is precisely sandwiched between the Sun and the Moon. This alignment ensures the entire side of the Moon that faces us gleams under sunlight. Thanks to the Moon’s orbit around Earth, the angle of sunlight hitting the lunar surface and being reflected back to our planet changes. That creates different lunar phases.

The next Full Moon will be the October Hunter’s Moon, which occurs at 12:12 a.m. EDT on Monday, Oct. 26, 2026.

We’ll update this article multiple times each week with the latest moonrise, moonset, Full Moon schedule, and some of what you can see in the sky each week.

Here’s the complete list of Full Moons this year and their traditional names.

2026 Full Moon schedule and names of each

(All times Eastern; * denotes a Super Moon.)

  • Saturday, Jan. 3 — 5:03 a.m. — Wolf Moon*
  • Sunday, Feb. 1 — 5:09 p.m. — Snow Moon
  • Tuesday, March 3 — 6:38 a.m. — Worm Moon | Total lunar eclipse
  • Wednesday, April 1 — 10:12 p.m. — Pink Moon
  • Friday, May 1 — 1:23 p.m. — Flower Moon
  • Sunday, May 31 — 4:45 a.m. — Blue Moon
  • Monday, June 29 — 7:57 p.m. — Strawberry Moon
  • Wednesday, July 29 — 10:36 a.m. — Buck Moon
  • Friday, Aug. 28 — 12:19 a.m. — Sturgeon Moon | Partial lunar eclipse
  • Saturday, Sept. 26 — 12:49 p.m. — Corn Moon | Harvest Moon
  • Monday, Oct. 26 — 12:12 a.m. — Hunter’s Moon
  • Tuesday, Nov. 24— 9:54 a.m. — Beaver Moon*
  • Wednesday , Dec. 23 — 8:28 p.m. — Cold Moon*

The phases of the Moon in October 2026

The images below show the day-by-day phases of the Moon in October. The Full Moon this month will be on Monday, Oct. 26, 2026.

The moonrise and moonset schedule this week

The times below for sunrise, sunset, moonrise, and moonset are given in local time from 40° N 90° W. The Moon’s illumination is given at 10 P.M. local time from the same location. All other times are Eastern unless otherwise specified. For more details on upcoming sky events, check out our full Sky This Week column.

Friday, October 23
The nearly Full Moon passes 5° north of Neptune at 11 P.M. EDT, creating a celestial triangle with the ice giant and nearby gas giant Saturn. Our satellite and Neptune share the constellation Pisces, while Saturn floats in northwestern Cetus. 

By early evening, the trio stands above the southeastern horizon, and by local midnight they are high in the south. Neptune is 4° south of (below) the Moon, while Saturn is 8° to our satellite’s southeast (left). Only the latter planet is visible to the naked eye, as Neptune requires binoculars or a telescope to view.

Sunrise: 7:19 A.M.
Sunset: 6:09 P.M.
Moonrise: 4:41 P.M.
Moonset: 4:26 A.M.
Moon Phase: Waxing gibbous (95%)

Saturday, October 24
The Moon passes 7° north of Saturn at 2 P.M. EDT. You can catch them rising together in the east after dark, with Saturn just to the Moon’s lower left as they gain altitude with every passing hour. Despite the waxing Moon’s brightness, you should still be able to easily spot the ringed planet with the naked eye. 

Sunrise: 7:21 A.M.
Sunset: 6:07 P.M.
Moonrise: 5:05 P.M.
Moonset: 5:35 A.M.
Moon Phase: Waxing gibbous (98%)

Sunday, October 25

Sunrise: 7:22 A.M.
Sunset: 6:06 P.M.
Moonrise: 5:33 P.M.
Moonset: 6:46 A.M.
Moon Phase: Full

Monday, October 26
October’s Full Moon occurs at 12:12 A.M. EDT, shining brightly in both the morning and evening sky. The October Full Moon is also called the Hunter’s Moon, which follows the Full Harvest Moon we saw in September.

Observing the Full Moon can actually be a bit challenging. At Full phase, the Sun appears directly overhead from the nearside and it is lunar “noon,” which means shadows are at their shortest and the landscape does not appear as three-dimensional as we peer up at it. However, that doesn’t mean there’s no observing to be had! 

First, though, if you plan to use a telescope, consider a Moon filter to cut down on the glare. If you don’t have one, you can observe while wearing sunglasses to get the same effect — just make sure not to slip them over your eyes until you’re about to step up to the eyepiece. Using higher magnifications will also reduce the amount of bright light streaming into your eye, as greater magnification reveals less of the lunar surface in a single field of view. 

Although many features are not at their best during a Full Moon, the rays of ejecta left behind as impactors slammed into the surface to create craters can be viewed during a Full Moon. In particular, the large crater Tycho in the lunar south has a huge, well-defined system of rays you can explore, some of which stretch hundreds of miles from the crater itself. Other craters that have stunning rays you can seek out during Full Moon include Copernicus, Proclus, Aristarchus, Stevinus, and Byrgius.

Sunrise: 7:23 A.M.
Sunset: 6:05 P.M.
Moonrise: 6:06 P.M.
Moonset: 8:02 A.M.
Moon Phase: Waning gibbous (99%)

Tuesday, October 27

Sunrise: 7:24 A.M.
Sunset: 6:04 P.M.
Moonrise: 6:47 P.M.
Moonset: 9:20 A.M.
Moon Phase: Waning gibbous (95%)

Wednesday, October 28
The Moon passes 5° north of Uranus at 6 A.M. EDT this morning. You’ll find our satellite hanging above the Pleiades (M45) in Taurus, roughly 45° high in the west around 6 A.M. local daylight time. Together with Uranus, the Moon and Pleiades form a triangle in the sky that slowly sets as twilight approaches. 

The Moon reaches perigee, the closest point to Earth in its orbit, later today at 2:06 P.M. EDT. At that time, our satellite will stand 226,433 miles (364,409 kilometers) away.

Sunrise: 7:25 A.M.
Sunset: 6:02 P.M.
Moonrise: 7:39 P.M.
Moonset: 10:36 A.M.
Moon Phase: Waning gibbous (88%)

Thursday, October 29

Sunrise: 7:26 A.M.
Sunset: 6:01 P.M.
Moonrise: 8:41 P.M.
Moonset: 11:47 A.M.
Moon Phase: Waning gibbous (80%)

Friday, October 30

Sunrise: 7:27 A.M.
Sunset: 6:00 P.M.
Moonrise: 9:53 P.M.
Moonset: 12:45 P.M.
Moon Phase: Waning gibbous (69%)

The phases of the Moon

The phases of the Moon are: New Moon, waxing crescent, First Quarter, waxing gibbous, Full Moon, waning gibbous, Last Quarter, and waning crescent. A cycle starting from one Full Moon to its next counterpart, termed the synodic month or lunar month, lasts about 29.5 days.

Though a Full Moon only occurs during the exact moment when Earth, Moon, and Sun form a perfect alignment, to our eyes, the Moon seems Full for around three days.

RELATED: 20 things to see on the Moon

Different names for different types of Full Moon

There are a wide variety of specialized names used to identify distinct types or timings of Full Moons. These names primarily trace back to a blend of cultural, agricultural, and natural observations about the Moon, aimed at allowing humans to not only predict seasonal changes, but also track the passage of time. 

For instance, almost every month’s Full Moon boasts a name sourced from Native American, Colonial American, or other North American traditions, with their titles mirroring seasonal shifts and nature’s events.

Wolf Moon (January): Inspired by the cries of hungry wolves.

Snow Moon (February): A nod to the month’s often heavy snowfall.

Worm Moon (March): Named after the earthworms that signal thawing grounds.

Pink Moon (April): In honor of the blossoming pink wildflowers.

Flower Moon (May): Celebrating the bloom of flowers.

Strawberry Moon (June): Marks the prime strawberry harvest season.

Buck Moon (July): Recognizing the new antlers on bucks.

Sturgeon Moon (August): Named after the abundant sturgeon fish.

Corn Moon (September): Signifying the corn harvesting period.

Hunter’s Moon (October): Commemorating the hunting season preceding winter.

Beaver Moon (November): Reflects the time when beavers are busy building their winter dams.

Cold Moon (December): Evocative of winter’s chill.

In addition, there are a few additional names for Full Moons that commonly make their way into public conversations and news.

Super Moon: This term is reserved for a Full Moon that aligns with the lunar perigee, which is the Moon’s nearest point to Earth in its orbit. This proximity renders the Full Moon unusually large and luminous. For a Full Moon to earn the Super Moon tag, it should be within approximately 90 percent of its closest distance to Earth.

Blue Moon: A Blue Moon is the second Full Moon in a month that experiences two Full Moons. This phenomenon graces our skies roughly every 2.7 years. Though the term suggests a color, Blue Moons aren’t truly blue. Very occasionally, atmospheric conditions such as recent volcanic eruptions might lend the Moon a slightly blueish tint, but this hue isn’t tied to the term.

Black Moon: A Black Moon is a recent, unofficial term that can describe one of two situations. Either the third of four New Moons in a single astronomical season or the second of two New Moons in a month is a Black Moon. As its name suggests, the Black Moon is completely dark, as it is a New Moon that occurs when the Moon is between the Sun and Earth. The New Moon cannot be observed except during a total solar eclipse.

Harvest Moon: Occurring closest to the autumnal equinox, typically in September, the Harvest Moon is often renowned for a distinct orange tint it might display. This Full Moon rises close to sunset and sets near sunrise, providing extended hours of bright moonlight. Historically, this was invaluable to farmers gathering their produce.

Common questions about Full Moons

What is the difference between a Full Moon and a New Moon? A Full Moon is witnessed when Earth is between the Sun and the Moon, making the entire Moon’s face visible. Conversely, during a New Moon, the Moon lies between Earth and the Sun, shrouding its Earth-facing side in darkness.

How does the Full Moon influence tides? The Moon’s gravitational tug causes Earth’s waters to bulge, birthing tides. During both Full and New Moons, the Sun, Earth, and Moon are in alignment, generating “spring tides.” These tides can swing exceptionally high or low due to the combined gravitational influences of the Sun and Moon.

Here are the dates for all the lunar phases in 2026:

New First Quarter Full Last Quarter
Jan. 3 Jan. 10
Jan. 18 Jan. 25 Feb. 1 Feb. 9
Feb. 17 Feb. 24 March 3 March 11
March 18 March 25 April 1 April 10
April 17 April 23 May 1 May 9
May 16 May 23 May 31 June 8
June 14 June 21 June 29 July 7
July 14 July 21 July 29 Aug. 5
Aug. 12 Aug. 19 Aug. 28 Sept. 4
Sept. 10 Sept. 18 Sept. 26 Oct. 3
Oct. 10 Oct. 18 Oct. 26 Nov. 1
Nov. 9 Nov. 17 Nov. 24 Dec. 1
Dec. 8 Dec. 17 Dec. 23 Dec. 30

Oct. 23, 1893: Birth of Ernest Opik

Born Oct. 23, 1893, in Estonia, Ernest Opik was based at the Astronomical Observatory in Tartu from 1921-1944. It was there in the 1920s that he began to research meteors and comets, their frequencies, and their speeds. In 1932, he proposed a reservoir of long-period comets that formed a large cloud, orbiting the Sun at the farthest reaches of the solar system. Opik’s theory was based on the fact that comets rapidly burn out once they swing into the inner solar system; therefore, he concluded, there must be a source out there somewhere to continue providing all the new comets we observe. In the 1950s, Jan Oort used cometary orbits to provide the mathematical evidence for this fresh-comet reserve. Although still a theoretical structure, this bubble or shell around our solar system is widely accepted as the explanation for long-period comets and is today known as the Oort Cloud – or, sometimes, as the Opik-Oort Cloud.


Elisa Neckar is senior production editor of Astronomy magazine, and the editor of the Today in the History of Astronomy feature on Astronomy.com.

The Sky Today on Friday, October 23: Nab Neptune near the Moon

Looking for a sky event this week? Check out our full Sky This Week column. 

October 22: Iapetus at superior conjunction

The nearly Full Moon passes 5° north of Neptune at 11 P.M. EDT, creating a celestial triangle with the ice giant and nearby gas giant Saturn. Our satellite and Neptune share the constellation Pisces, while Saturn floats in northwestern Cetus. 

By early evening, the trio stands above the southeastern horizon, and by local midnight they are high in the south. Neptune is 4° south of (below) the Moon, while Saturn is 8° to our satellite’s southeast (left). Only the latter planet is visible to the naked eye, as Neptune requires binoculars or a telescope to view. With the bright Moon nearby, the latter is your best bet, as it offers higher magnification. Through a scope, Neptune will look like a “flat,” bluish-gray star, with a tiny disk extending 2” in diameter. 

Saturn is much more impressive, with its disk 19” across and its rings some 44” from end to end. Its brightest moon, Titan, is just to the planet’s northeast, while around midnight CDT fainter Rhea and Tethys are east of the ringed world and Dione stands to its west. Iapetus, around 11th magnitude, remains relatively nearby, now about 2’ southeast of the planet. It’s still a great opportunity to catch so many of Saturn’s moons huddled close together.

Sunrise: 7:19 A.M.
Sunset: 6:09 P.M.
Moonrise: 4:41 P.M.
Moonset: 4:26 A.M.
Moon Phase: Waxing gibbous (95%)
*Times for sunrise, sunset, moonrise, and moonset are given in local time from 40° N 90° W. The Moon’s illumination is given at 10 P.M. local time from the same location. 


Alison Klesman is senior editor of Astronomy magazine. She holds a Ph.D. in astronomy and has studied a variety of topics, from minor planets to supermassive black holes.

The Sky This Week from October 23 to 30: Gaze at the Full Hunter’s Moon 

Friday, October 23
The Moon passes 5° north of Neptune at 11 P.M. EDT; you can catch the pair in the south around that time, along with Saturn in the southwest, just to the Moon’s lower left. Saturn is visible to the naked eye, but Neptune is not. The distant ice giant will require binoculars or a telescope to spot and may still be a challenge, hanging below the bright Moon in Pisces. 

Above the Moon, look for the four bright stars that form the Great Square of Pegasus: Algenib, Alpheratz, Scheat, and Markab. Alpheratz, at the upper left-hand (northeastern) corner of the Square, is not technically within the bounds of Pegasus, and is officially cataloged as Alpha (α) Andromedae, in the constellation Andromeda. However, it is also cataloged as Delta (δ) Pegasi, as it once belonged to the Winged Horse’s domain. 

Venus reaches inferior conjunction with the Sun at midnight EDT.

Sunrise: 7:19 A.M.
Sunset: 6:09 P.M.
Moonrise: 4:41 P.M.
Moonset: 4:26 A.M.
Moon Phase: Waxing gibbous (95%)
*Times for sunrise, sunset, moonrise, and moonset are given in local time from 40° N 90° W. The Moon’s illumination is given at 10 P.M. local time from the same location.

Saturday, October 24
Mercury reaches a stationary point in Libra at 8 A.M. EDT. The tiny planet is only briefly visible after sunset, but if you’ve got a clear horizon, give it a try. Look west roughly 20 to 30 minutes after sunset, and scan for a magnitude 0.5 point of light just above the horizon. Mercury is 2.5° high in the southwest 20 minutes after sunset, and 1° high in the west 10 minutes later. You may want to try sweeping the area slowly with binoculars, but make sure the Sun has set completely below the horizon before pulling out any optical aid. Mercury’s disk stretches 9” across and the planet is 28% lit if you can catch it through a telescope. 

Today’s standstill marks an end to Mercury’s prograde, or eastward, movement. After this, it will begin tracking westward, or retrograde, heading back past Alpha (α) Librae in just a few days and crossing into Virgo in early November, joining Venus. 

The Moon passes 7° north of Saturn at 2 P.M. EDT. You can catch them rising together in the east after dark, with Saturn just to the Moon’s lower left as they gain altitude with every passing hour. Despite the waxing Moon’s brightness, you should still be able to easily spot the ringed planet with the naked eye. 

Sunrise: 7:21 A.M.
Sunset: 6:07 P.M.
Moonrise: 5:05 P.M.
Moonset: 5:35 A.M.
Moon Phase: Waxing gibbous (98%)

Sunday, October 25
Saturn’s small moon Dione transits the disk this evening at 8:43 p.m. EDT, best seen from the eastern half of the U.S. However, the transit itself will be difficult to watch visually no matter your location, and will be best captured via high-speed video. Even if you aren’t an advanced photographer, however, you can watch Dione enter and exit the disk, as well as track several of Saturn’s other moons throughout the night. 

Around 9 P.M. EDT (8 P.M. CDT), Saturn is well above the horizon, in the east for Midwestern observers and the southeast for those along the East Coast. It’s the brightest point of light in this part of the sky and should be visible to the naked eye even with the Moon nearby. You’ll need a telescope to spot its rings and moons, however, and the larger the better to help cut through the Moon’s glare. Prior to the transit’s start, 10th-magnitude Dione is approaching the planet’s northeastern limb, with similarly bright Tethys east of the rings and Rhea to their west. Brighter Titan, which shines around magnitude 8.5, is also visible far west of Saturn all evening, about 2’ from the planet’s center. 

As Dione begins its transit, it will likely seem to disappear for visual observers, as its tiny disk will be difficult to pick out against Saturn’s bright cloud tops. Video capture might also nab the moon’s shadow, which will cross the far northern polar region of the planet, appearing around 9:40 P.M. EDT and disappearing roughly half an hour later, before Dione reaches the northwestern limb. The moon does this just before 10:40 P.M. EDT — now, visual observers will see it pop into view just off the limb and begin pulling away from Saturn to the west. 

Sunrise: 7:22 A.M.
Sunset: 6:06 P.M.
Moonrise: 5:33 P.M.
Moonset: 6:46 A.M.
Moon Phase: Full

Monday, October 26
October’s Full Moon occurs at 12:12 A.M. EDT, shining brightly in both the morning and evening sky. The October Full Moon is also called the Hunter’s Moon, which follows the Full Harvest Moon we saw in September.

Observing the Full Moon can actually be a bit challenging. At Full phase, the Sun appears directly overhead from the nearside and it is lunar “noon,” which means shadows are at their shortest and the landscape does not appear as three-dimensional as we peer up at it. However, that doesn’t mean there’s no observing to be had! 

First, though, if you plan to use a telescope, consider a Moon filter to cut down on the glare. If you don’t have one, you can observe while wearing sunglasses to get the same effect — just make sure not to slip them over your eyes until you’re about to step up to the eyepiece. Using higher magnifications will also reduce the amount of bright light streaming into your eye, as greater magnification reveals less of the lunar surface in a single field of view. 

Although many features are not at their best during a Full Moon, the rays of ejecta left behind as impactors slammed into the surface to create craters can be viewed during a Full Moon. In particular, the large crater Tycho in the lunar south has a huge, well-defined system of rays you can explore, some of which stretch hundreds of miles from the crater itself. Other craters that have stunning rays you can seek out during Full Moon include Copernicus, Proclus, Aristarchus, Stevinus, and Byrgius.

Sunrise: 7:23 A.M.
Sunset: 6:05 P.M.
Moonrise: 6:06 P.M.
Moonset: 8:02 A.M.
Moon Phase: Waning gibbous (99%)

Tuesday, October 27
The Moon’s bright light washes out dimmer targets, but not all deep-sky objects are out of reach. Late this evening, the constellation Camelopardalis sits in the north, to the right (east) of the Little Dipper and sandwiched between Cassiopeia and Ursa Major. 

In Camelopardalis’ southwestern region is a 6th-magnitude open cluster called NGC 1502. Stretching about 8’ across, this compact group of young stars lies about 9° south of magnitude 4.6 Gamma (γ) Camelopardalis and is visible in binoculars or any telescope. But it’s only the beginning: NGC 1502 lies at one end of a line of stars known as Kemble’s Cascade. This asterism resembles a waterfall with NGC 1502 serving as the spray of water coming from the pool at its base. From NGC 1502, look for a snaking line of nearly two dozen stars roughly 2.5° long, shining between about 7th and 10th magnitude and stretching up toward the northwest. You’ll want binoculars or a finder scope to take them all in at once, or you can slide slowly along the line within the smaller field of view of your telescope. 

The asterism is named for Father Lucian Kemble, who described the pattern in a letter to astronomy popularizer Walter Scott Houston. 

Sunrise: 7:24 A.M.
Sunset: 6:04 P.M.
Moonrise: 6:47 P.M.
Moonset: 9:20 A.M.
Moon Phase: Waning gibbous (95%)

Wednesday, October 28
The Moon passes 5° north of Uranus at 6 A.M. EDT this morning. You’ll find our satellite hanging above the Pleiades (M45) in Taurus, roughly 45° high in the west around 6 A.M. local daylight time. Together with Uranus, the Moon and Pleiades form a triangle in the sky that slowly sets as twilight approaches. 

If you want to view Uranus, you’ll need some optical aid — technically its magnitude of 5.6 puts it within naked-eye range, but the bright Moon nearby will wash it out. You can find the ice giant 5° to the lower left of the Moon as they sink, or about halfway along a line drawn from the Pleiades toward the upper left and ending at the bright star Aldebaran. 

Magnitude 0.9 Aldebaran (Alpha [α] Tauri) is typically envisioned as the eye of Taurus the Bull. The red giant is the 14th brightest star in the sky, shining with a luminosity more than 400 times that of the Sun from a distance of roughly 67 light-years. Despite its brightness, its surface temperature is quite cool, which results in the reddish color. Compare its orangey-red hue to that of Mars in the east. 

The Moon reaches perigee, the closest point to Earth in its orbit, later today at 2:06 P.M. EDT. At that time, our satellite will stand 226,433 miles (364,409 kilometers) away.

Sunrise: 7:25 A.M.
Sunset: 6:02 P.M.
Moonrise: 7:39 P.M.
Moonset: 10:36 A.M.
Moon Phase: Waning gibbous (88%)

Thursday, October 29
The W-shaped constellation Cassiopeia is prominent in the northern sky after sunset as it wheels around the North Celestial Pole, which marked by the North Star, Polaris. Around 8 P.M. local daylight time — after dark but before moonrise — you’ll find the Queen to the right of Polaris when facing north, positioned such that her stars now look like the numeral 3.

In the northern region of Cassiopeia, located to the lower left of the this pattern, is a loose open cluster cataloged as Collinder 463. The Collinder catalog, created in 1931 by Per Collinder, contains nearly 500 open clusters of young stars. Entry No. 463, our target, shines around 6th magnitude and sits roughly 8.2° north of 3rd-magnitude Epsilon (ε) Cassiopeiae, along a line drawn between this star and Polaris. Spanning roughly 73’, it’s easy to observe in binoculars or a small scope. At low magnification, such as through binoculars or a finder scope, many observers think its gaggle of stars form a rough crescent-shaped smudge of light on the sky. What shape do you see? 

Sunrise: 7:26 A.M.
Sunset: 6:01 P.M.
Moonrise: 8:41 P.M.
Moonset: 11:47 A.M.
Moon Phase: Waning gibbous (80%)

Friday, October 30
Magnitude 0.8 Mars, currently tracking eastward through the sky, now stands at the border of Cancer and Leo. It is still within the bounds of the Crab this morning, roughly 60° high in the southeast and just over 6° to the upper right of brighter Jupiter in Leo, about 90 minutes before sunrise. 

To Jupiter’s east (lower left) is magnitude 1.4 Regulus, the brightest star in the Lion, which also serves as the great cat’s heart. Together with Jupiter and Mars, the three form a line slashing upward in the predawn sky.

Far to the planetary pair’s upper right is Procyon, the bright nose of Canis Minor, the Little Dog. And to that star’s far lower right is even brighter Sirius, the nose of Canis Major, the Big Dog — the brightest star in the sky. However, Jupiter (at magnitude –2.0) currently outshines Sirius’ magnitude –1.4 glow.

Mars will continue to move east, joining Jupiter in Leo by tomorrow morning.

Sunrise: 7:27 A.M.
Sunset: 6:00 P.M.
Moonrise: 9:53 P.M.
Moonset: 12:45 P.M.
Moon Phase: Waning gibbous (69%)


Alison Klesman is senior editor of Astronomy magazine. She holds a Ph.D. in astronomy and has studied a variety of topics, from minor planets to supermassive black holes.

Mars’ moon Phobos is destined to become a ring

Phobos, it seems, is not long for this universe — at least on the large cosmic timescale. 

Astronomers have long known that Phobos, the larger and nearer of the two martian moons, is slowly spiraling inward to eventual destruction. The end result won’t be pretty: Phobos will slip closer and closer toward Mars, then strike a gravitational line where the planet’s tidal forces will be strong enough to rip it apart. The rubble pile-like moon will break into smaller boulders, rocks, and dust, and will spread out in orbit around Mars. 

Mars will join the gas giants in having a spectacular feature: a ring system. 

It could be 25 million years from now. It could be up to 75 million years. Recent discoveries about the little moon’s composition and density, however, make it far more likely that its death dive will happen sooner. The pieces that don’t form a ring will fall to the surface, smashing with enough force to pockmark Mars with new craters.

“A lot of planetary science focuses on what happened in the past and what’s happening now,” says planetary scientist Benjamin A. Black. “It’s not often that we look at the future, at what will happen.” Black, a City University of New York professor, and graduate student Tushar Mittal from the University of California, Berkeley, have carried out a detailed examination of the eventual fate of Phobos. 

Related: Japan launches sample return mission to Phobos

It appears the process of coming apart at the seams has already begun. Images of Phobos taken by the Viking orbiters and other spacecraft show a network of grooves in the tiny moon’s surface. At first they appeared to radiate from near Stickney Crater, and geologists assumed that the grooves were cracks caused by the ancient impact. Some certainly are just that, but not all. In 2015, Terry Hurford of NASA’s Goddard Space Flight Center and his colleagues reported a new analysis of the grooves. Most of them actually radiate from the side of Phobos that constantly faces Mars; tidal forces caused by Mars’ gravitational pull are deforming Phobos. Hurford believes the grooves are stretch marks, a visible sign of the inexorable grip of tidal forces on the moon.

The future martian ring will not be the only one in the solar system, of course. Nor will it be the only ring whose existence depends on a moon. There are rings across the giant planets: the four dusty rings of Jupiter; Uranus’ 13 dark, thin rings; and Neptune’s five faint rings and four enigmatic ring arcs are — like the future ring around Mars — all intimately linked to moons and moonlets. And of course, the most familiar ringed planet is Saturn, whose icy surrounding matter can be seen even through a small telescope.

Saturn’s magnificent rings

Galileo Galilei saw what turned out to be Saturn’s spectacular ring system in 1610. (He said the features looked like ears or handles.) But it wasn’t until 1655 that Christiaan Huygens identified them as an entire system of icy rings. In 1856, famed physicist James Clerk Maxwell showed that the rings must be composed of a huge number of tiny particles (he called them “brick-bats”), each independently orbiting Saturn. 

Since then, debate has raged over the origin, age, and composition of Saturn’s rings. Are they leftovers from the formation of Saturn, or the remains of a shattered moon? As old as Saturn itself, or a relatively new addition? And why so much ice? Planetary scientist Robin M. Canup of the Southwest Research Institute in Boulder, Colorado, recently published a proposal that answers these questions. Canup suggests that Saturn’s rings are the very ancient remains of a Titan-sized moon. 

“Saturn originally had multiple massive moons like Jupiter,” says Canup. These moons were large enough for their interiors to differentiate into layers of ices and a rocky core — less like a large comet and more like the four larger moons of Jupiter. When the large moons spiraled inward as Saturn finished its accretion, Canup says, the outer icy layers of at least one were stripped away. The core plunged into Saturn, and the icy remains eventually formed the planet’s main rings. This, she says, explains why the particles making up the rings are 99.9 percent pure water ice. It also explains the striking difference between Jupiter’s and Saturn’s rings and satellites. 

“The existence of Saturn’s much more massive ring system is linked to Saturn having lost its large primordial inner moons,” Canup explains. “Jupiter retained its large inner moons, [while] its dusty ring system is vastly less massive than the ring system at Saturn.”

Related: How long will Saturn’s rings last before they disappear?


Rings of the giant planets

Jupiter’s four faint and dusty rings probably formed by a different mechanism than Saturn’s — and more recently — but its moons still play a vital role. Amalthea and Thebe are the likely sources of the material in Jupiter’s outer two “gossamer” rings. Thebe orbits within the outer gossamer ring, while Amalthea lies near the outer edge of the inner gossamer ring. Metis and Adrastea, two other small moons, orbit near the outer edge of Jupiter’s main ring, and are the sources of the dust grains making up the main and innermost halo rings. 

Some forces work against the rings, keeping them relatively thin. Electromagnetic forces, a phenomenon called plasma drag, and even pressure from sunlight (called the Poynting-Robertson effect) continually remove the micron-sized particles from the rings. But particles sputtered off the moons by meteoroid impacts create dust and continually replenish the rings. 

The 13 known rings of Uranus are unlike those of Jupiter or Saturn. All but the innermost and two outermost of the rings are quite narrow, ranging from just 0.6 to 59.6 miles (1 to 96 kilometers) wide. Their particles are larger than those in Jupiter’s rings, but there’s little dust. Instead, they’re largely made up of ice with organic chemicals mixed in to give the dark appearances, unique among the outer solar system rings.

But there are similarities: Like Jupiter’s and Saturn’s rings, Uranus’ rings are intimately associated with moons and moonlets. Primordial moons the size of Puck, 100 miles (162km) in diameter, or larger would have had a good chance of surviving for several billion years. But not all would escape a devastating fate. Computer simulations show that the 11 inner moons of Uranus are likely the remains of original larger moons broken up by cometary impacts. What’s more, the current rate of meteoroid impacts among moons and other icy bodies at Uranus’ distance is enough to create all the observed rings and dust bands circling that planet. 

Because the rings appear to be young, probably not more than 600 million years old, the material in the rings must be continually renewed. Particles blasted off the tiny moons and still-unseen moonlets by collisions and meteoroid strikes continually add material to the rings, while the dust continues to dissipate. 

Neptune’s five rings and various dust bands are probably even younger than those of Uranus, and the same processes are likely responsible for them and the moons that orbit in or near them. Naiad and Thalassa orbit in the gap between the innermost Galle and Le Verrier rings, and Despina orbits just inside the Le Verrier ring. Galatea lies slightly inside the outermost Adams ring. These tiny moons are likely rubble-pile objects, agglomerations of fragments from earlier neptunian moons, weakly held together by gravity. The ring particles are material continually blasted off the moons by meteoroid impacts. Unlike the uranian rings, the rings of Neptune are quite dusty, thanks to the destruction of a satellite; at least 20 percent of the material is the size of smoke particles, and in some of the rings, that rises to 70 percent.

The Adams ring also has five distinct clumps or arcs of dust spanning about 40° in longitude. How they can exist for any length of time is a mystery, as these tenuous rings should have faded away. One explanation, by planetary ring expert Carolyn Porco, leader of the Cassini orbiter’s imaging team, is that a resonance effect caused by Galatea’s eccentric orbit may act to keep the particles in the arcs from spreading out and dissipating.


Creating a martian ring

Phobos isn’t nearly the size of a planet, but many of the same mechanisms will drive its destruction. Its companion moon Deimos is about 7.8 miles (12.6 kilometers) in diameter and orbits Mars at an average distance of 14,580 miles (23,460km), far enough away to avoid Phobos’ fate. Phobos is 13.8 miles (22.2km) in diameter. It circles the planet at an average distance of 5,827 miles (9,377km). With an orbital period of just 7 hours, 39.2 minutes, Phobos is one of only 18 of the 181 known moons in the solar system whose orbital period is less than its planet’s rotation period.

That’s one of a few reasons why Phobos is doomed. “There are four factors in action,” explains Mittal. “The tidal force of Mars; the centrifugal forces on Phobos, which is rotating; the gravity of Phobos; and the strength of Phobos. There’s a balance among these. Tidal and rotational stresses act to pull Phobos apart; self-gravity and [tensile] strength act to hold Phobos together.”

Just as our own Moon’s gravity raises tides in both Earth’s oceans and landmasses, Phobos creates a tiny tidal bulge in Mars. The bulge moves as the moon circles Mars, just as the Moon-caused tidal bulge moves around Earth. Because Phobos has an orbital period faster than the martian day, the tidal bulge lags behind Phobos and acts to gradually slow it in its orbit, sending Phobos slowly spiraling in toward the martian surface. The rate is about 0.79 inch (2 centimeters) per year. It’s not much, but there is nothing to stop it.

“As Phobos gets closer to Mars,” says Mittal, “the tidal stresses increase.” The moon’s self-gravity and tensile strength oppose the tidal forces, but eventually Phobos will drop to a distance — called the Roche limit — where the martian gravity will win the tug-of-war. Several studies confirm that Phobos’ inward spiral will lead to its destruction in 25 million to 75 million years.

Phobos could stave off obliteration if it were a dense body, more able to resist the pull of gravity past the Roche limit. Unfortunately, data from the European Space Agency’s Mars Express orbiter show that the moon has a density of just 1.9 grams per cubic centimeter. By comparison, our Moon has a density of 3.3g per cubic centimeter. Even tiny Themisto, Jupiter’s smallest regular moon at just 4.9 miles (8km) in diameter, has an estimated density of about 2.6g per cubic centimeter. Mars Express also revealed that Phobos is porous, likely containing large voids, so it is probably a rubble pile, like many of Uranus’ and Neptune’s tiny moons.

In addition, Phobos’ makeup is similar to carbonaceous chondrite meteorites like the ones that fell on Canada’s Tagish Lake in 2000. These primitive meteorites are made of a bevy of loose, easily broken materials, including magnetite, olivine crystals, phyllosilicates, and complex organic molecules such as amino acids, and are about 10 percent water, formed in oxygen-rich regions of the early solar system. Phobos is not only a rubble pile with a weak gravitational field, but the rubble itself is somewhat frangible.

Then there’s Stickney Crater, the giant impact basin on Phobos. Sometime in its past, Phobos was hit by an object that left a crater 5.6 miles (9km) wide — nearly half the moon’s diameter. The impact surely fractured much of Phobos’ interior, leaving it even weaker. From there, billions of years of meteoroid impacts have churned the surface of Phobos into a layer of fine dust about a hundred meters deep. Given the extremely weak surface gravity (escape velocity for Phobos is a mere 4.56 feet per second), the rock making up the rubble pile just barely stays put.

Black and Mittal used a numerical geotechnical model designed for large underground construction projects to estimate what they call the moon’s “rock mass strength.” The results place the finale for Phobos between 20 million and 40 million years from now, and give more details on its violent end.

As Phobos reaches its Roche limit, about 3,400 miles (5,470km) from the martian surface, tidal forces will start pulling Phobos apart. Just as Saturn’s tidal forces may have peeled away the icy mantle of a Titan-sized moon billions of years ago, the hundred meters or so of regolith will be stripped off Phobos. It will happen quickly: In as little as a week, the dust will spread into a ring circling Mars, the moon no more.

Depending on how much material is stripped off Phobos, the ring could initially have a mass density similar to that of today’s rings of Saturn. The martian ring will be very dark, unlike Saturn’s bright icy rings, more like the dusty rings of Jupiter that are darker, thinner, and more diffuse. It will practically hug Mars, closer in relative terms to the planet than the other planetary rings in the solar system. And the ring, say Black and Mittal, will not last long; they estimate its lifetime at between 1 million and 100 million years.

Eventually, the rocky rubble left behind will meet a quicker but equally dramatic end. It will plummet down along slanting paths to impact the surface of Mars and leave a string of elongated craters along the planet’s equator.

Other once and future rings

Is it possible that Mars possessed a ring system in its distant past? “We’re not certain,” says Black, “but it would be worth investigating whether past inwardly migrating moons may have existed. Some fraction of moons might be expected to have an orbital configuration similar to that of Phobos and Mars.”

Some planetary scientists think Mars once did have more than two moons. Researchers have identified 258 elliptical craters on Mars formed by objects hitting the surface at grazing angles. At least some of them could well have been made by oblique impacts of ancient martian moons. If so, others may have broken up before hitting the atmosphere, leaving short-lived rings of rocks and dust around Mars.

There’s no evidence that Mercury or Venus ever possessed ring systems. Earth did, though, for an extremely brief period during the formation of the Moon 4.5 billion years ago when our planet was struck by a Mars-sized body dubbed Theia. Much of Theia merged with Earth, but the “Big Splash” would have blown the remaining material into space. Computer simulations indicate about 20 percent of Theia’s mass would have gone into orbit around Earth as a ring. About 10 percent of the ring’s material then quickly coalesced into the Moon, with the rest eventually falling back to Earth. The ring would not have lasted long, perhaps as little as a month but probably no more than 100 years.

Curiously, our Moon also could end as it began, according to astronomer Lee Anne Willson, university professor emerita at Iowa State University. As part of her research on the fate of Earth as the Sun expands into a red giant, she found that the Moon stood a chance of becoming a ring around Earth.

The Moon is receding from Earth at a rate of about 1.6 inches (4cm) per year. Left unchecked, the Moon will eventually migrate out to a distance where it will take 47 days to orbit Earth. By then, Earth’s rotation also will have slowed to 47 days. The two will then keep the same face to each other, as Pluto and its moon Charon do today.

Before this happens, though, some 5 billion years from now, the Sun will enter its red giant phase. It will start expanding in size, and swallow up Mercury and Venus. As the Earth-Moon system orbits through the Sun’s expanded outer atmosphere, drag forces will cause the Moon’s orbit to begin decaying. The Sun probably will continue to expand, and destroy both Earth and the Moon. On the other hand, if the Sun should blow off about 20 percent of its mass first, the Moon will continue to spiral down to its Roche limit. Tidal forces will tear it apart, just as they will destroy Phobos. 

And then, 9 billion years after the Moon’s birth from a ring of molten impact ejecta, and nearly 5 billion years after the birth and death of the ring around Mars, Earth will once again have a ring.

This story was originally published online August 29, 2019.


Joel Davis is a freelance science writer whose articles have also appeared in Analog, Final Frontier, New Scientist, and Science Digest. His books include Flyby: The Interplanetary Odyssey of Voyager 2 and Journey to the Center of Our Galaxy.

Oct. 22, 2137 B.C.E.: An eclipse darkens skies over ancient China

The earliest solar eclipse for which we have a record appears in the ancient Chinese text Shujing, traditionally said to have been compiled by the philosopher Confucius, which reads: “On the first day of the last month of autumn, the Sun and Moon did not meet harmoniously in Fang.” What an understated way to describe an eclipse!

Pinning the exact date of this event is somewhat problematic; originally, scholars stated it occurred either in 2136 or 2128 B.C.E. The mention of “Fang,” though, ultimately holds the key: This term refers to a section of the sky mainly in Scorpius. Furthermore, we know the eclipse happened during the reign of Zhong Kang, an emperor of the Xia Dynasty. Based on these details, the only eclipse that could have been seen from the capital city was on Oct. 22, 2137 B.C.E.

There’s also a long-standing tale — which may be true but very probably isn’t — about this eclipse and two royal astrologers, He and Ho. In at least one version, they were drunk prior to the event and didn’t warn the emperor that the eclipse was coming. Whether or not they even knew it was coming is debatable. Long story short, they reportedly were killed for their mistake.


Michael E. Bakich is a contributing editor for Astronomy magazine. With degrees in astronomy and planetarium education, he has led many eclipse tours, published several books on observing, and logged thousands of hours at the eyepiece.

The Sky Today on Thursday, October 22: Iapetus at superior conjunction

Looking for a sky event this week? Check out our full Sky This Week column. 

October 21: Catch early-morning Orionids

Saturn’s strange, two-faced moon Iapetus orbits on a wide path that it takes nearly 80 days to complete. During that time, it slowly rotates in synchrony with its orbit, brightening and fading by up to two magnitudes, depending on which hemisphere is facing Earth. 

Tonight, Iapetus is just past superior conjunction, sitting south of Saturn and glowing at 11th magnitude. It is visible with a telescope. Saturn is already well-positioned soon after darkness falls, reaching a height of roughly 30° above the eastern horizon by 8 P.M. local daylight time. Through a telescope, you’ll easily view its lovely rings, showing off their southern side. Bright Titan, its largest moon, is just 1.6’ east of the planet, shining at mid-8th magnitude. Tethys, Rhea, and Dione shine around 10th magnitude and are closer to the ringed world. Around 8 P.M. CDT, Dione is east of Saturn and Tethys and Rhea are west of the planet. 

Iapetus lies 1.7’ south-southeast of Saturn, fainter than the other four moons. Because its orbit takes it so far from the planet and because it is faint, Iapetus is easiest to find at superior and inferior conjunction, so tonight is a great time to track it down. 

Sunrise: 7:18 A.M.
Sunset: 6:10 P.M.
Moonrise: 4:18 P.M.
Moonset: 3:20 A.M.
Moon Phase: Waxing gibbous (89%)
*Times for sunrise, sunset, moonrise, and moonset are given in local time from 40° N 90° W. The Moon’s illumination is given at 10 P.M. local time from the same location. 


Alison Klesman is senior editor of Astronomy magazine. She holds a Ph.D. in astronomy and has studied a variety of topics, from minor planets to supermassive black holes.