A Case for Ten Planets

Clyde Tombaugh (1906-1997) spent the first fifteen years of his life on a farm near Streator, Illinois, and then his family moved to a farm near Burdett, Kansas (no wonder he got interested in astronomy!), and he went to high school there. Then, on February 18, 1930, Tombaugh, a self-taught amateur astronomer and telescope maker, discovered the ninth planet in our solar system, Pluto. It had been nearly 84 years since the eighth planet, Neptune, had been discovered, in 1846. And it would be another 62 years before another trans-Neptunian object (TNO) would be discovered.

Clyde Tombaugh made his discovery using a 13-inch f/5.3 photographic refractor at the Lowell Observatory in Flagstaff, Arizona.

Clyde Tombaugh was 24 years old when he discovered Pluto. He died in 1997 at the age of 90 (almost 91). I was very fortunate to meet Prof. Tombaugh at a lecture he gave at Iowa State University in 1990. At that lecture, he told a fascinating story about the discovery of Pluto, and I remember well his comment that he felt certain that no “tenth planet” larger than Pluto exists in our solar system, because of the thorough searches he and others had done since his discovery of Pluto. But, those searches were done before the CCD revolution, and just two years later, the first TNO outside the Pluto-Charon system, 15760 Albion (1992 QB1), would be discovered by David Jewitt (1958-) and Jane Luu (1963-), although only 1/9th the size of Pluto.

Pluto is, by far, the smallest of the nine planets. At only 2,377 km across, Pluto is only 2/3 the size of our Moon! Pluto has a large moon called Charon (pronounced SHAR-on) that is 1,212 km across (over half the size of Pluto), discovered in 1978 by James Christy (1938-). Two additional moons were discovered using the Hubble Space Telescope (HST) in 2005: Hydra (50.9 × 36.1 × 30.9 km) and Nix (49.8 × 33.2 × 31.1 km). A fourth moon was discovered using HST in 2011: Kerberos (10 × 9 × 9 km). And a fifth moon, again using HST, in 2012: Styx (16 × 9 × 8 km).

Pluto has been visited by a single spacecraft. New Horizons passed 12,472 km from Pluto and 28,858 km from Charon on July 14, 2015. Then, about 3½ years later, New Horizons passed 3,538 km from 486958 Arrokoth, on January 1, 2019.

Only one other TNO comparable in size to Pluto (or larger) is known to exist. 136199 Eris and its moon Dysnomia were discovered in 2005 by Mike Brown (1965-), Chad Trujillo (1973-), and David Rabinowitz (1960-). It is currently estimated that Eris is 97.9% the size of Pluto. Not surprisingly, in 2006 Pluto was “demoted” by the IAU from planethood to dwarf planet status. (Is not a “dwarf planet” a planet? Confusing…)

My take on this is that Pluto should be considered a planet along with Eris, of course. The definition of “planet” is really rather arbitrary, so given that Pluto was discovered 75 years before Eris, and 62 years before TNO #2, I think we should (in deference to the memory of Mr. Tombaugh, mostly) define a planet as any non-satellite object orbiting the Sun that is around the size of Pluto or larger. So, by my definition, there are currently ten known planets in our solar system. Is that really too many to keep track of?

There is precedent for including history in scientific naming decisions. William Herschel (1738-1822) is thought to have coined the term “planetary nebula” in the 1780s, and though we now know they have nothing to do with planets (unless their morphology is affected by orbiting planets), we still use the term “planetary nebula” to describe them today.

In the table below, you will find the eight “classical” planets, plus the five largest TNOs, all listed in order of descending size. (The largest asteroid, Ceres, is 939 km across, and is thus smaller than the smallest of these TNOs.)

You’ll see that the next largest TNO after Eris is Haumea, and that its diameter is only 67% that of Eris.

I’ve also listed the largest satellite for each of these objects. Venus and Mercury do not have a satellite—at least not at the present time.

It is amazing to note that both Ganymede and Titan are larger than the planet Mercury! And Ganymede, Titan, the Moon, and Triton are all larger than Pluto.

Largest Objects in the Solar System

Object Diameter (km) Largest Satellite Diameter (km) Size Ratio
Jupiter 139,822 Ganymede 5,268 3.8%
Saturn 116,464 Titan 5,149 4.4%
Uranus 50,724 Titania 1,577 3.1%
Neptune 49,244 Triton 2,707 5.5%
Earth 12,742 Moon 3,475 27.3%
Venus 12,104 N/A N/A N/A
Mars 6,779 Phobos 23 0.3%
Mercury 4,879 N/A N/A N/A
Pluto 2,377 Charon 1,212 51.0%
Eris 2,326 Dysnomia 700 30.1%
Haumea 1,560 Hiʻiaka 320 20.5%
Makemake 1,430 S/2015 (136472) 175 12.2%
Gonggong 1,230 Xiangliu 200 16.3%

Should any other non-satellite objects with a diameter of at least 2,000 km be discovered in our solar system, I think we should call them planets, too.

Impetus for Iapetus

PIA11690: Global View of Iapetus’ Dichotomy, NASA/JPL/Space Science Institute

What a strange world Iapetus is! The third largest satellite of Saturn—and the outermost of Saturn’s large satellites—is a moon of many mysteries. We’ll take a look at three of them.

Mystery #1: Iapetus appears to be an original satellite of Saturn, and yet unlike the other regular satellites, its orbit is inclined 15.5˚ relative to Saturn’s equator. The reason for this steep inclination is not well understood.

And, oh, the view! Iapetus is the perfect perch to view Saturn’s rings, as it orbits Saturn every 79.3 days in its steeply inclined orbit.

Saturn from Iapetus at the highest point of its inclined orbit

Mystery #2: Iapetus has the largest albedo dichotomy in the solar system. Why? Iapetus is locked in synchronous rotation as it orbits around Saturn, with the leading hemisphere ten times darker than its trailing hemisphere.

Iapetus has an average visual magnitude of 10.2 west of Saturn and 11.9 east of Saturn. Its albedo ranges from 0.5 to 0.05. (Diagram not to scale)
Bright and dark material on Iapetus. The 500-km-wide crater Engelier is at bottom.

It is thought that the natural state of the Iapetian surface is the bright icy part, with the dark material a thin veneer, less than a meter thick.

Mystery #3: Iapetus has a shape consistent with a body spinning every ~16 hours and yet its rotation period is 79.3 days, and it has a prominent ridge that can be followed 3/4 of the way around the equator.

Walnut-shaped Iapetus with its prominent equatorial ridge
Iapetus’ equator-girdling ridge, up to 20 km high, is heavily cratered and therefore ancient

The surface of Iapetus is heavily cratered, indicating it is very old. Could two comparable-sized objects have collided almost head-on billions of years ago to form Iapetus?

Mountainous terrain along Iapetus’ equatorial ridge imaged by the Cassini spacecraft during its closest flyby on September 10, 2007

As beautiful as spacecraft flyby and orbital images are of Iapetus and the many other interesting moons in our solar system, can you imagine what vistas await us once we start exploring their surfaces with rovers? Anticipation of these images and scientific discoveries surely is an impetus to explore the surface of Iapetus (and other moons) sooner rather than later.

Dark and light material on Iapetus was imaged up close by the Cassini spacecraft during its September 10, 2007 flyby.
Sizes of Iapetus, Earth’s moon, and Earth compared


References

Bonnefoy, Léa E., Jean-François Lestrade, Emmanuel Lellouch, Alice Le Gall, Cédric Leyrat, Nicolas Ponthieu, and Bilal Ladjelate. “Probing the subsurface of the two faces of Iapetus.” arXiv preprint arXiv:1911.03394 (2019).

Leleu, Adrien, Martin Jutzi, and Martin Rubin. “The peculiar shapes of Saturn’s small inner moons as evidence of mergers of similar-sized moonlets.” Nature astronomy 2, no. 7 (2018): 555-561.

Rivera-Valentin, Edgard G., Amy C. Barr, EJ Lopez Garcia, Michelle R. Kirchoff, and Paul M. Schenk. “Constraints on planetesimal disk mass from the cratering record and equatorial ridge on Iapetus.” The Astrophysical Journal 792, no. 2 (2014): 127.

Iapetus – Wow!

Saturn’s third largest moon, Iapetus (eye-AP-eh-tuss), was discovered at the then-new Paris Observatory in 1671 by Italian-French astronomer (and observatory director) Giovanni Domenico (Jean-Dominique) Cassini (1625-1712).  Upon further observation, Cassini noted that he could only see Iapetus when it was on the west side of Saturn, never the east.  His telescope was not large enough to detect Iapetus on the east side of Saturn because it was much fainter then.  He correctly reasoned that, “it seems, that one part of his surface is not so capable of reflecting to us the light of the Sun which maketh it visible, as the other part is.”  He also must have realized that Iapetus was locked in synchronous rotation—as is our Moon—with the same side facing Saturn all the time, with its rotation period being equal to its orbital period.  Today we know these periods to be 79.3215 days.

The leading hemisphere of Iapetus has a visual albedo of only about 5%, whereas most of the trailing hemisphere is much brighter, having an albedo around 25%.  Thus, when Iapetus is on the west side of Saturn, its apparent visual magnitude is around 10.2, but on the east side of Saturn Iapetus is 1.7 magnitudes fainter at 11.9.  Without a doubt, Iapetus is one of the most outlandish places in the solar system, and the Cassini Saturn orbiter flybys certainly amplified the strangeness.

Cassini made one close targeted flyby of Iapetus on September 10, 2007, passing within 762 miles of the surface.  Here are a few of the best photos of Iapetus from Cassini.

The first high-resolution glimpse of the bright trailing hemisphere of Saturn’s moon Iapetus

This is a raw, or unprocessed, image taken by the Cassini spacecraft during its close flyby of Saturn’s moon Iapetus on Sept. 10, 2007 showing its prominent equatorial ridge—still a mystery

The “Himalayas” of Iapetus

The Transition Zone

Closest View of Iapetus

Dark material splatters the walls and floors of craters in the surreal, frozen wastelands of Iapetus

May 30, 2017 – Cassini bids farewell to Saturn’s yin-and-yang moon, Iapetus

The dark material appears to have been deposited from elsewhere in the Saturnian system, but sublimation of water ice may also play a role.  In any event, the dark material is a relatively thin veneer, significantly less than a meter thick in many places.

The warm day on Iapetus sees a surface temperature of -227° F on the dark terrain and an even colder -256° F on the bright terrain.  Inhospitable, to say the least!

Saturn at Eastern Quadrature

Wednesday evening, September 13, 2017, at 9:59 p.m. CDT, Saturn reaches eastern quadrature as Saturn, Earth, and Sun form a right triangle.  Eastern quadrature is so named as Saturn is 90° east of the Sun.  This is the time when Saturn presents to us its most gibbous phase.  Even so, Saturn will be 99.7% illuminated due to its great distance from us.

A more noticeable effect will be the shadow of Saturn on its rings, a phenomenon best seen at eastern or western quadrature.

Saturn will only be 12° above our horizon in SW Wisconsin at the exact moment of eastern quadrature Wednesday evening.  Earlier that evening, Saturn crosses the celestial meridian at 6:51 p.m.—22 minutes before sunset.  If it weren’t for daylight, that would be the best time to observe Saturn: when it is highest in the sky and we are seeing it through the least amount of atmosphere.  If you have a telescope equipped with a polarizing filter, you can significantly darken the blue sky background around Saturn since the planet will be exactly 90° away from the Sun, where the scattered sunlight is most highly polarized.  Rotate the polarizer until the sky is darkest around Saturn.

Speaking of Saturn, the Cassini mission will come to a bittersweet end on Friday, September 15 around 5:31 a.m. CDT when the storied spacecraft, which has been orbiting Saturn since June 30, 2004, will have plunged deep enough into Saturn’s atmosphere that it is no longer able to point its high gain antenna towards Earth.  Soon after that, Cassini will burn up in Saturn’s massive atmosphere.  We on Earth will not receive Cassini’s last radio transmission until 1h23m later—at around 6:54 a.m. CDT.

Emily Lakdawalla, who is arguably the best planetary science journalist in the world these days, includes the visual timeline of Cassini’s demise shown below and in her recent blog entry, “What to expect during Cassini’s final hours”.

Also, on Wednesday evening, don’t miss NOVA: Death Dive to Saturn, which will air on Wisconsin Public Television’s flagship channel at 8:00 p.m.

It may be a while before we visit ringed Saturn and its retinue of moons again.  But further exploration of Titan and Enceladus is certain to feature prominently in humankind’s next mission to Saturn.  Hopefully, that will be soon.

Saturn at Opposition: Radiant Rings

If you look at Saturn through a telescope this Thursday morning, you’ll notice something very special about the view.  Saturn’s spectacular ring system—which is presently tilted towards us near its maximum amount—will look unusually bright and white compared with the ball of the planet.  Even though you may have looked at Saturn numerous times before and noticed that the rings are brighter and whiter than the disk of the planet (as well they should be, being composed almost entirely of water ice), you will be wholly unprepared for the view that awaits you this Thursday morning.  The rings will be positively radiant!  Why haven’t you noticed this before?

Saturn, you see, reaches opposition at 5:18 a.m. CDT on Thursday, June 15.  At the moment of opposition in Iowa County, Wisconsin, Saturn will only be 2° above the SW horizon and the Sun just three minutes before sunrise in the NE.  Best to look around 3:03 a.m. at the beginning of astronomical twilight when Saturn will be a respectable 19° above the SSW horizon.

When a superior planet (like Saturn) is at opposition, the Sun, the Earth, and the planet (in that order) form very nearly a straight line.  When we look at Saturn when it is at opposition, we see sunlight reflected off of the icy ring particles pretty much along the path the sunlight took.  Put another way, when light is shining normal (perpendicular) to a reflective surface, more light is reflected back along the normal than is scattered in other directions, so the reflection seems bright.  What’s more, since our line of sight to Saturn’s rings at opposition most closely aligns with the line of incident sunlight, we “see” no shadows from the ring particles, and the rings appear even brighter because of that.  Of course, we can’t see individual ring particles, but when sunlight strikes the rings more from the side, innumerable tiny shadows are cast by ring particles on other ring particles, and the total amount of light reflected back to us is diminished.  This phenomenon is called the opposition effect.

Saturn’s equator and ring plane are tilted 26.7° relative to its orbit around the Sun, so that means we see the rings at different angles throughout Saturn’s 29.5 year orbital period.  For example, the rings were seen edge-on in 1995.  They were tipped 26.7° to the north (meaning we had the best view of the south side of the rings and the southern hemisphere of the planet) in 2003.  The rings were again seen edge-on in 2009, and this year they are tipped 26.7° to the south, meaning we presently have the best view of the north side of the rings and the northern hemisphere of the planet.

Saturn goes through seasons just like the Earth, and the tilt of the rings reflects this.  Just as the northern hemisphere of the Earth is tilted most towards the Sun at summer solstice, Saturn’s northern hemisphere and the north side of its rings are tilted most towards the Sun when Saturn is at its summer solstice.  At the autumnal equinox on Earth, the Earth’s equator lines up with the Sun, and when Saturn is at its autumnal equinox, Saturn’s equator and its rings line up with the Sun.  At winter solstice, the southern hemisphere of the Earth is tilted most towards the Sun.  Likewise, when Saturn is at winter solstice, the south side of Saturn’s rings and its southern hemisphere are tilted most towards the Sun.  At the vernal equinox on Earth, the Earth’s equator once again lines up with the Sun.  And, when Saturn reaches its vernal equinox, Saturn’s equator and its rings once again line up with the Sun.  And so on.  The only difference is our four seasons take a year, but the four seasons on Saturn take nearly 30 years.

The tilt of Saturn’s rings would thus progress peacefully and sinusoidally with two maxima and two minima every 29.5 years—if we were observing from the Sun.  But, of course, we are observing Saturn from spaceship Earth, so the tilt of the rings that we see changes due to our position relative to Saturn in addition to Saturn’s position relative to the Sun.  This causes more rapid—albeit smaller—variations in the observed tilt angle as we orbit much faster around the Sun than Saturn does.  For example, right now we see Saturn’s rings tilted 26.6°.  On July 15, it will be 26.7°.  On August 15, 26.8°.  On September 15, 26.9°.  On October 15, 27.0°.  On November 15, back to 26.9° again.

The best time, then, to see Saturn’s rings at their most radiant is when Saturn is at opposition and when Saturn’s rings are near maximum tilt. Here on Spaceship Earth, that will next occur on Thursday, June 15, 2017.  Fortunately, Saturn’s phase angle will be just 0.1° during all of Wednesday night and Thursday morning.  Saturn rises at 8:27 p.m. Wednesday evening, June 14, and reaches 10° above the SE horizon at 9:40 p.m.  Enjoy!

Evening Planets

The most convenient time for most of us to observe the planets is in the early evening.  With that in mind, I’ve prepared an ephemeris of favorable evening times to view each of the eight major planets of the solar system over the next ten years.  Some interesting patterns emerge, which I will comment on.

With the exception of Mercury, what follows is a range of dates when each planet is at least 10° above the horizon at the end of evening twilight at latitude 43° N.  Mercury, however, is never even above the horizon at the end of evening twilight.

Mercury’s Maximum
Altitude at 43° N
Solar Depression
Angle
End of
Twilight
13°
Civil
12°
Nautical
below horizon
18°
Astronomical

Here is a list of dates when Mercury is highest above the western horizon at the end of evening civil twilight.

Mercury

Dates – Highest Above
Evening Horizon
Altitude
Constellation
July 18, 2017
Leo
November 28, 2017
Sgr
March 15, 2018
12°
Psc
July 2, 2018
Cnc
November 10, 2018
Oph
February 27, 2019
11°
Psc
June 16, 2019
10°
Gem
October 20, 2019
Lib
February 11, 2020
11°
Aqr
May 30, 2020
12°
Gem
September 25, 2020
Vir
January 25, 2021
10°
Cap
May 14, 2021
13°
Tau
September 2, 2021
Vir
January 9, 2022
Cap
April 28, 2022
13°
Tau
August 14, 2022
Leo
December 24, 2022
Sgr
April 11, 2023
13°
Ari
July 28, 2023
Leo
December 8, 2023
Sgr
March 24, 2024
12°
Psc
July 11, 2024
Cnc
November 20, 2024
Oph
March 8, 2025
12°
Psc
June 25, 2025
Cnc
November 1, 2025
Sco
February 20, 2026
11°
Psc
June 9, 2026
11°
Gem
October 10, 2026
Lib
February 4, 2027
11°
Aqr
May 24, 2027
13°
Tau
September 15, 2027
Vir

Mercury, the innermost planet, whips around the Sun every 88 days (116 days relative to the Earth—its synodic period).  It never strays more than 28° from the Sun.

As you can see in the graph below, Mercury is presently highest above our evening twilight horizon when it reaches greatest eastern elongation in April, and lowest in October.

Similarly, greatest eastern elongations that occur in the constellations Taurus and Aries present Mercury highest above our evening twilight horizon, and Libra, the lowest.

Now, let us turn to Venus.  Unlike Mercury, Venus usually spends a considerable number of days well above the horizon near greatest elongation.  This occurs because Venus orbits further from the Sun—reaching a maximum angular separation of 47°— and because its orbital period is only 140.6 days shorter than the Earth’s: the Earth “keeps up” with Venus reasonably well as the two planets orbit the Sun (the synodic period of Venus is 583.9 days), so it is a long time between successive elongations.  In the next ten years, we will see Venus high above the evening horizon during only three intervals, though for a generous three or four months each time.

Venus

Dates – At Least 10° Above the Horizon
at the End of Evening Twilight
Constellation
January 2, 2020 – May 7, 2020
Cap – Tau
February 26, 2023 – June 3, 2023
Cet – Cnc
November 30, 2024 – March 2, 2025
Sgr – Psc

Now, we turn to the superior planets: Mars, Jupiter, Saturn, Uranus, and Neptune.  These planets are visible in our evening sky during and after opposition.

Mars has the longest synodic period of all the major planets—780 days—so it takes an unusually long period of time for the orbital positions of Mars and the Earth to change relative to one another.  Approximately every two years we get the opportunity to see Mars at least 10° above the horizon at the end of evening twilight.  The number of evenings Mars is visible varies quite a lot (due to its significant orbital eccentricity): 293 evenings during the 2018 perihelic opposition of Mars, down to 145 evenings during the aphelic opposition of Mars in 2027.  In any event, Mars spends a considerable amount of time during these intervals very far away from Earth and therefore disappointingly small in our telescopes.  The best time to observe Mars is during the early weeks of the intervals listed below when Mars is at or near opposition.

Mars

Dates – At Least 10° Above the Horizon
at the End of Evening Twilight
Constellation
July 21, 2018 – May 10, 2019
Cap – Tau
October 5, 2020 – May 27, 2021
Psc – Gem
November 28, 2022 – June 11, 2023
Tau – Cnc
January 7, 2025 – June 22, 2025
Cnc – Leo
February 12, 2027 – July 7, 2027
Leo – Vir

Jupiter orbits the Sun every 11.9 years, so it is easy to see why it is in a different constellation along the zodiac each year.

Jupiter

Dates – At Least 10° Above the Horizon
at the End of Evening Twilight
Constellation
March 30, 2017 – July 24, 2017
Vir
April 29, 2018 – August 29, 2018
Lib
May 28, 2019 – October 19, 2019
Oph
June 26, 2020 – December 10, 2020
Sgr
July 30, 2021 – January 22, 2022
Aqr
September 10, 2022 – March 1, 2023
Psc
October 21, 2023 – April 5, 2024
Ari
November 28, 2024 – May 5, 2025
Tau
January 1, 2026 – May 28, 2026
Gem
February 2, 2027 – June 16, 2027
Leo

The orbital periods of Saturn, Uranus, and Neptune are 29.5, 84.0, and 164.8 years, respectively, so we can see why they take a successively longer amount of time to traverse their circle of constellations.  You’ll also notice that the interval of visibility shifts later each year, but the shift is less with increasing orbital distance.  The synodic periods of Saturn, Uranus, and Neptune are 378.1, 369.7, and 367.5 days, respectively.

Saturn

Dates – At Least 10° Above the Horizon
at the End of Evening Twilight
Constellation
May 31, 2017 – October 25, 2017 Oph
June 10, 2018 – November 11, 2018 Sgr
June 20, 2019 – November 28, 2019 Sgr
June 30, 2020 – December 12, 2020 Cap – Sgr
July 12, 2021 – December 27, 2021 Cap
July 24, 2022 – January 9, 2023 Cap
August 7, 2023 – January 23, 2024 Aqr
August 21, 2024 – February 4, 2025 Aqr
September 5, 2025 – February 17, 2026 Psc
September 20, 2026 – March 2, 2027 Cet – Psc

Uranus

Dates – At Least 10° Above the Horizon
at the End of Evening Twilight
Constellation
October 2, 2017 – March 16, 2018
Psc
October 7, 2018 – March 20, 2019
Ari
October 12, 2019 – March 23, 2020
Ari
October 15, 2020 – March 27, 2021
Ari
October 20, 2021 – March 31, 2022
Ari
October 25, 2022 – April 4, 2023
Ari
October 30, 2023 – April 7, 2024
Ari
November 3, 2024 – April 12, 2025
Tau
November 8, 2025 – April 16, 2026
Tau
November 13, 2026 – April 20, 2027
Tau

Neptune

Dates – At Least 10° Above the Horizon
at the End of Evening Twilight
Constellation
August 13, 2017 – January 30, 2018
Aqr
August 16, 2018 – February 2, 2019
Aqr
August 19, 2019 – February 4, 2020
Aqr
August 21, 2020 – February 6, 2021
Aqr
August 24, 2021 – February 8, 2022
Aqr
August 27, 2022 – February 11, 2023
Aqr
August 30, 2023 – February 13, 2024
Psc
September 1, 2024 – February 15, 2025
Psc
September 4, 2025 – February 17, 2026
Psc
September 7, 2026 – February 17, 2027
Psc