October  2018

Updated:   8 October 2018

 

Welcome to the night skies of Spring, featuring Scorpius, Sagittarius, Aquila, Lyra, Cygnus, Mars, Jupiter and Saturn

 

Note:  Some parts of this webpage may be formatted incorrectly by older browsers.

 

The Alluna RC-20 Ritchey Chrétien telescope was installed in March, 2016.

The 20-inch telescope is able to locate and track any sky object (including Earth satellites and the International Space Station) with software called TheSkyX Professional, into which is embedded a unique T-Point model developed for our site with our equipment over the past year.

 

Explanatory Notes:  

 

Times for transient sky phenomena are given using a 24 hour clock, i.e. 20:30 hrs = 8.30 pm. Times are in Australian Eastern Standard Time (AEST), which equals Universal Time (UT) + 10 hours. Daylight saving is not observed in Queensland. Observers in other time zones will need to make their own corrections where appropriate. With conjunctions of the Moon, planets and stars, timings indicate the closest approach. Directions (north or south) are approximate. The Moon’s diameter is given in arcminutes ( ’ ). The Moon is usually about 30’ or half a degree across. The 'limb' of the Moon is its edge as projected against the sky background.

Rise and set times are given for the theoretical horizon, which is a flat horizon all the way round the compass, with no mountains, hills, trees or buildings to obscure the view. Observers will have to make allowance for their own actual horizon. 

Transient phenomena are provided for the current month and the next. Geocentric phenomena are calculated as if the Earth were fixed in space as the ancient Greeks believed. This viewpoint is useful, as otherwise rising and setting times would be meaningless. In the list of geocentric events, the nearer object is given first.

When a planet is referred to as ‘stationary’, it means that its movement across the stellar background appears to have ceased, not that the planet itself has stopped. With inferior planets (those inside the Earth’s orbit, Mercury and Venus), this is caused by the planet heading either directly towards or directly away from the Earth. With superior planets (Mars out to Pluto), this phenomenon is caused by the planet either beginning or ending its retrograde loop due to the Earth’s overtaking it.

Apogee and perigee:   Maximum and minimum distances of the Moon or artificial satellite from the Earth.

Aphelion and perihelion:  Maximum and minimum distances of a planet, asteroid or comet from the Sun.

The zenith is the point in the sky directly overhead from the observer.

The meridian is a semicircle starting from a point on the horizon that is exactly due north from the observer, and arching up into the sky to the zenith and continuing down to a point on the horizon that is exactly due south. On the way down it passes through the South Celestial Pole which is 26.6 degrees above the horizon at Nambour. The elevation of the South Celestial Pole is exactly the same as the observer's latitude, e.g. from Cairns it is 16.9 degrees above the horizon, and from Melbourne it is 37.8 degrees. The Earth's axis points to this point in the sky in the southern hemisphere, and to an equivalent point in the northern hemisphere, near the star Polaris, which from Australia is always below the northern horizon.

All astronomical objects rise until they reach the meridian, then they begin to set. The act of crossing or 'transitting' the meridian is called 'culmination'. Objects closer to the South Celestial Pole than its altitude above the southern horizon do not rise or set, but are always above the horizon, constantly circling once each sidereal day. They are called 'circumpolar'. The brightest circumpolar star from Nambour is Miaplacidus (Beta Carinae, magnitude = 1.67).  

A handspan at arm's length with fingers spread covers an angle of approximately 18 - 20 degrees.

mv = visual magnitude or brightness. Magnitude 1 stars are very bright, magnitude 2 less so, and magnitude 6 stars are so faint that the unaided eye can only just detect them under good, dark conditions. Binoculars will allow us to see down to magnitude 8, and the Observatory telescope can reach visual magnitude 17 or 22 photographically. The world's biggest telescopes have detected stars and galaxies as faint as magnitude 30. The sixteen very brightest stars are assigned magnitudes of 0 or even -1. The brightest star, Sirius, has a magnitude of -1.44. Jupiter can reach -2.4, and Venus can be more than 6 times brighter at magnitude -4.7, bright enough to cast shadows. The Full Moon can reach magnitude -12 and the overhead Sun is magnitude -26.5. Each magnitude step is 2.51 times brighter or fainter than the next one, i.e. a magnitude 3.0 star is 2.51 times brighter than a magnitude 4.0. Magnitude 1.0 stars are exactly 100 times brighter than magnitude 6.0 (5 steps each of 2.51 times, 2.51x2.51x2.51x2.51x2.51 = 2.515 = 100).

 

The Four Minute Rule:   

How long does it take the Earth to complete one rotation? No, it's not 24 hours - that is the time taken for the Sun to cross the meridian on successive days. This 24 hours is a little longer than one complete rotation, as the curve in the Earth's orbit means that it needs to turn a fraction more (~1 degree of angle) in order for the Sun to cross the meridian again. It is called a 'solar day'. The stars, clusters, nebulae and galaxies are so distant that most appear to have fixed positions in the night sky on a human time-scale, and for a star to return to the same point in the sky relative to a fixed observer takes 23 hours 56 minutes 4.0916 seconds. This is the time taken for the Earth to complete exactly one rotation, and is called a 'sidereal day'.

As our clocks and lives are organised to run on solar days of 24 hours, and the stars circulate in 23 hours 56 minutes approximately, there is a four minute difference between the movement of the Sun and the movement of the stars. This causes the following phenomena:

    1.    The Sun slowly moves in the sky relative to the stars by four minutes of time or one degree of angle per day. Over the course of a year it moves ~4 minutes X 365 days = 24 hours, and ~1 degree X 365 = 360 degrees or a complete circle. Together, both these facts mean that after the course of a year the Sun returns to exactly the same position relative to the stars, ready for the whole process to begin again.

    2.    For a given clock time, say 8:00 pm, the stars on consecutive evenings are ~4 minutes or ~1 degree further on than they were the previous night. This means that the stars, as well as their nightly movement caused by the Earth's rotation, also drift further west for a given time as the weeks pass. The stars of autumn, such as Orion are lost below the western horizon by mid-June, and new constellations, such as Sagittarius, have appeared in the east.  The stars change with the seasons, and after a year, they are all back where they started, thanks to the Earth's having completed a revolution of the Sun and returned to its theoretical starting point.

We can therefore say that the star patterns we see in the sky at 11:00 pm tonight will be identical to those we see at 10:32 pm this day next week (4 minutes X 7 = 28 minutes earlier), and will be identical to those of 9:00 pm this date next month or 7:00 pm the month after. All the above also includes the Moon and planets, but their movements are made more complicated, for as well as the Four Minute Drift  with the stars, they also drift at different rates against the starry background, the closest ones drifting the fastest (such as the Moon or Venus), and the most distant ones (such as Saturn or Neptune) moving the slowest.

 

 

 Solar System

 

Sun:   The Sun begins the month in the constellation of Virgo, the Virgin. It leaves Virgo and passes into Libra, the Scales on October 31.   

 

 

Moon Phases:  Lunations (Brown series):  #1184, 1185, 1186 


Last Quarter:          October 02              19:46 hrs          diameter = 32.2' 
New Moon:            
October 09              13:48 hrs          diameter = 32.1'     Lunation #1185 begins
First Quarter:          
October 17              04:02 hrs          diameter = 29.6' 
Full Moon:               
October 25              02:46 hrs          diameter = 31.1'

Last Quarter:          November 01          02:41 hrs          diameter = 32.3'
New Moon:             November 08          02:03 hrs          diameter = 31.2'     Lunation #1186 begins  
First Quarter:          November 16          00:55 hrs          diameter = 29.6'
Full Moon:               November 23          15:40 hrs          diameter = 32.1'
Last Quarter:          November 30         10:20 hrs           diameter = 32.2' 

 
 

 
 

Lunar Orbital Elements:


October 04:            Moon at ascending node at 13:09 hrs, diameter = 32.5'
October 06:            Moon at perigee (366 399 km) at 08:41 hrs, diameter = 32.6'
October 17:            Moon at descending node at 22:06 hrs, diameter = 29.6'
October 18:            Moon at apogee (404 215 km) at 05:21 hrs, diameter = 29.6'
October 31:            Moon at ascending node at 13:46 hrs, diameter = 32.3'

November 01:        Moon at perigee (370 227 km) at 07:17 hrs, diameter = 32.3'
November 14:        Moon at descending node at 00:06 hrs, diameter = 29.6'
November 15:        Moon at apogee (404 345 km) at 01:42 hrs, diameter = 29.6'
November 26:        Moon at perigee (366 607 km) at 22:22 hrs, diameter = 32.6'
November 27:        Moon at ascending node at 15:18 hrs, diameter = 32.6'

Moon at 8 days after New, as on October 18.

The photograph above shows the Moon when approximately eight days after New, just after First Quarter.  A detailed map of the Moon's near side is available here.  A rotatable view of the Moon, with ability to zoom in close to the surface (including the far side), and giving detailed information on each feature, may be downloaded  here.

Click here for a photographic animation showing the lunar phases. It also shows the Moon's wobble or libration, and how its apparent size changes as it moves from perigee to apogee each month. It takes a little while to load, but once running is very cool !  All these downloads are freeware, although the authors do accept donations if the user feels inclined to support their work.

 

 

Lunar Feature for this Month:

 

Each month we describe a lunar crater, cluster of craters, valley, mountain range or other object, chosen at random, but one with interesting attributes. A recent photograph from our Alluna RC20 telescope will illustrate the object. As all large lunar objects are named, the origin of the name will be given if it is important. This month we will look at the area near the Moon's South Pole.


This image of the south polar region of the Moon was taken at 7:10 pm on 30 July 2017.
 

Much of the Moon's near side is occupied by large, flat, dark areas covered with cooled basaltic lava. These areas were once though to be 'seas' (Maria), and the lighter coloured areas 'lands' (Terrae). Galileo's first observations of the Moon in 1609 showed that there were no bodies of water on the Moon, and the seas were in fact lava plains. Strangely, the far side of the Moon has no large maria, but is almost totally covered with large overlapping impact craters. The south polar region of the Moon is unlike the rest of the near side, and is very much like the far side.

There is no mare material visible in the image above - on the contrary, it shows thousands of craters crowded together. Seen from above they are all more or less circular in shape, but due to their position near the South Pole they are greatly foreshortened into ovals, but this is merely due to perspective. The closer they are to the South Pole, the more exaggerated is this effect. Craters along the Moon's edge or 'limb' are seen in profile, as if from a low-flying spacecraft. The South Pole is marked with a coloured dot.

There are two craters that are very close to the Moon's South Pole. The closer one, marked with an 'A ', is called 'Amundsen'. It has a diameter of 109 kilometres. The adjoining one, marked with an ' S', is called 'Scott'. It has a diameter of 111 kilometres. These two craters are not usually visible, as the Moon's monthly wobble or libration takes them out of sight. They are best seen when libration has swung them towards the Earth around First or Last Quarters, as above.

 

Amundsen and Scott

Regarding the Earth, in the first years of the 20th century there was a race by two teams of explorers to be first to reach the South Pole in Antarctica. There was a Norwegian team headed by Roald Amundsen, which relied on horses and dogs to pull their sledges carrying supplies. Trying to beat them to the Pole was a British team headed by Robert Falcon Scott, which used the new motor-driven tractors then becoming available as well as dogs. Amundsen was against using machines untried in polar conditions, saying that, in an emergency, "you can't eat a tractor." All of Scott's motor vehicles failed before they had gone very far, and his men towards the end had to pull the sledges themselves.

History records that Amundsen, secretly starting before Scott, reached the geographic South Pole first with four other team members on 14 December 1911. They left a small black tent and Norwegian flag at the site. Scott and four other men reached the Pole on 17 January 1912, 34 days after Amundsen. They were bitterly disappointed to have been beaten and sadly began the return journey. A relentless blizzard overtook them and they sheltered for days in a tent where they perished from starvation and cold.  Amundsen's team returned safely from their expedition to world-wide acclaim, but their success has always been overshadowed by the deaths of Scott and his men. Today there is a permanent base at the South Pole where scientists live and work in air-conditioned comfort.


The photograph of the Moon's South Polar area covers the area inside the rectangle above.

 

Click  here  for the  Lunar Features of the Month Archive

 




Geocentric Events:




It should be remembered that close approaches of Moon, planets and stars are only perspective effects as seen from the Earth - that is why they are called 'geocentric or Earth-centred phenomena'. The Moon, planets and stars do not really approach and dance around each other as it appears to us from the vantage point of our speeding planet.

 

October 1:            Limb of Moon 37 arcminutes south of the star Zeta Tauri (mv= 2.97) at 18:43 hrs
October 2:            Moon 1.4º south of the star Mu Geminorum (mv= 2.87) at 14:43 hrs
October 6:            Venus at eastern stationary point at 04:50 hrs  (diameter = 49.9")
October 6:            Moon 2.3º north of the star Regulus (Alpha Leonis, mv= 1.36) at 10:16 hrs
October 6:            Mercury 2º north of the star Spica (Alpha Virginis, mv= 0.98) at 16:44 hrs
October 10:          Saturn 1.7º south of the star Mu Sagittarii (mv= 3.84) at 07:22 hrs
October 10:          Moon 5.7º north of Mercury at 18:25 hrs
October 12:          Moon 4.5º north of Jupiter at 07:54 hrs
October 12:          Pluto at eastern quadrature at 13:58 hrs
October 15:          Moon 2.2º north of Saturn at 10:56 hrs
October 16:          Moon occults the star Pi Sagittarii (mv= 2.88) between 12:23 and 12:11 hrs
October 16:          Moon 1.3º north of Pluto at 19:44 hrs
October 16:          Mercury at aphelion at 19:06 hrs  (diameter = 5.1")
October 18:          Moon 2.3º north of Mars at 23:06 hrs
October 18:          Moon occults the star Theta Capricorni (mv= 4.08) between 22:58 and 00:08 hrs
October 19:          Limb of Moon 44 arcminutes north of the star Deneb Algedi (Alpha Capricorni, mv= 2.85) at 16:34 hrs
October 20:          Mercury 2º south of the star Zuben Elgenubi (Alpha Librae, mv= 2.75) at 17:40 hrs
October 21:          Moon 1.9º south of Neptune at 09:32 hrs
October 24:          Uranus at opposition at 10:27 hrs  (diameter = 3.7")
October 25:          Moon 3.7º south of Uranus at 02:23 hrs
October 27::         Venus at inferior conjunction at 00:15 hrs  (diameter = 61.3")
October 27:          Moon 1.9º north of the star Aldebaran (Alpha Tauri, mv= 0.87) at 21:21 hrs
October 28:          Moon occults the star Zeta Tauri (mv= 2.97) between 23:29 and 00:22 hrs
October 29:          Mercury 3.1º south of Jupiter at 21:24 hrs
October 29:          Moon 1.2º south of the star Mu Geminorum (mv= 2.87) at 18:08 hrs
October 30:          Jupiter 43 arcminutes north of the star Kappa Librae (mv= 4.75) at 18:26 hrs

November 6:        Moon 9º north of Venus at 19:41 hrs
November 7:        Mercury at greatest elongation east (23º 09') at 00:56 hrs  (diameter = 6.6")
November 9:        Moon 4.3º north of Jupiter at 04:02 hrs
November 12:      Moon  2.1º north of Saturn at 01:42 hrs
November 12:      Moon has a grazing occultation of the star Pi Sagittarii (mv= 2.88) between 23:44 and 23:52 hrs
November 13:      Moon 1.5º north of Pluto at 03:40 hrs
November 16:      Moon 1.1º north of the star Deneb Algedi (Alpha Capricorni, mv= 2.85) at 02:52 hrs
November 16:      Limb of Moon 35 arcsminutes south of Mars at 13:19 hrs
November 16:      Venus at western stationary point at 20:25 hrs  (diameter = 51.3")
November 17:      Mercury at eastern stationary point at 11:24 hrs  (diameter = 8.4")
November 17:      Moon 2.4º south of Neptune at 17:21 hrs
November 21:      Moon 4.1º south of Uranus at 08:51 hrs
November 24:      Moon 2.1º north of the star Aldebaran (Alpha Tauri, mv= 0.87) at 08:21 hrs
November 25:      Limb of Moon 1 arcminute south of the star Zeta Tauri (mv= 2.97) at 09:35 hrs
November 25:      Neptune at eastern stationary point at 08:38 hrs  (diameter = 2.3")
November 26:      Limb of Moon 7 arcminutes south of the star Mu Geminorum (mv= 2.87) at 02:01 hrs
November 26:      Jupiter in conjunction with the Sun at 16:27 hrs  (diameter = 31.0")
November 27:      Mercury in inferior conjunction at 19:07 hrs  (diameter = 9.9")
November 28:      Mercury 25 arcminutes north of Jupiter at 08:03 hrs

 

 

The Planets for this month:   

 

Mercury:   Mercury passed through superior conjunction on September 21 and has now moved to the western twilight sky. It shines nearly as bright as Sirius, but is only visible when it is at a large angular distance from the glare of the Sun. As Mercury lies well inside the Earth's orbit and close to the Sun, it can never move more than 27.8º from the Sun. In the second week of October, Mercury will be visible close to the western horizon during twilight, and will appear close to Venus on October 16 and close to Jupiter on October 28 and 29. The thin crescent Moon will be between Mercury and Jupiter on November 9. Mercury will be best seen when it is at its maximum angular distance from the Sun in the first three weeks of November.

 

Venus:   This, the brightest planet, passed through superior conjunction (on the far side of the Sun) on January 9, thereby moving from the pre-dawn eastern sky to the twilight western sky. This month it is very prominent in the early evenings as a so-called 'evening star'.

Over the past six months, Venus has been approaching Jupiter in the sky as they circle around the Sun in their orbits. On September 29 they were at their closest, a little less than 14º apart. After that date, Venus turned away from Jupiter and their distance apart will increase as Venus prepares to go through inferior conjunction (passing between the Earth and the Sun) later this month.

On October 1, Venus will be 33º or under two handspans east of the Sun, and when twilight fades at 6:30 pm it will be about a handspan above the western horizon. It will appear in a small telescope as a tiny 'crescent Moon' with a magnitude of -4.5 and a phase of 17% (a narrow crescent like the New Moon). It will be near the junction of the constellations Virgo, Libra and Centaurus. The waxing crescent Moon will be between Venus and Jupiter on the evening of October 11. We will lose Venus from our early evening sky in the third week of October as it will be coming too close to the glare of the Sun to observe safely. It will pass through inferior conjunction on October 27. It will reappear in the eastern pre-dawn sky in early November as a 'morning star', where it will remain until August next year.

(The coloured fringes to the first and third images below are due to refractive effects in our own atmosphere, and are not intrinsic to Venus. The planet was closer to the horizon when these images were taken than it was for the second photograph, which was taken when Venus was at its greatest elongation from the Sun).

                     February 2018                        August 2018                          October 2018                      

Click here for a photographic animation showing the Venusian phases. Venus is always far brighter than anything else in the sky except for the Sun and Moon. For most of 2017, Venus appeared as a 'Morning Star' in the pre-dawn sky, where it stayed for about nine months. Venus passed on the far side of the Sun (superior conjunction) on January 9, 2018, and is now in the  evening sky as an 'Evening Star'. It will return to the morning sky to be a 'Morning Star' once again on October 27.

Because Venus is visible as the 'Evening Star' and as the 'Morning Star', astronomers of ancient times believed that it was two different objects. They called it Hesperus when it appeared in the evening sky and Phosphorus when it was seen before dawn. They also realised that these objects moved with respect to the so-called 'fixed stars' and so were not really stars themselves, but planets (from the Greek word for 'wanderers'). When it was finally realised that the two objects were one and the same, the two names were dropped and the Greeks applied a new name Aphrodite (Goddess of Love)  to the planet, to counter Ares (God of War). We use the Roman versions of these names, Venus and Mars, for these two planets.



Venus at 6.55 pm on September 7, 2018. The phase is 36 % and the angular diameter is 32 arcseconds.

 

This is the year of Mars:   The red planet is ideally placed for viewing this month as it is well above the eastern horizon as night falls and is close to the zenith at mid-evening. On October 1 it is well past opposition, now half a magnitude fainter than Jupiter, and with an angular diameter of 16 arcseconds. Mars reaches a point near the zenith at 7:46 pm. It is near the border of Sagittarius and Capricornus. As the month progresses, Mars will travel eastwards against the background stars, moving deeper into Capricornus. It will pass into the next zodiacal constellation, Aquarius, on November 11.

The opposition on July 27 was very close, and Mars appeared bigger than it has for many years. It was particularly favourable for us in the southern hemisphere, as during the month of opposition it was almost directly overhead each midnight from the Sunshine Coast.

The only problem with the current appearance of Mars is that on May 31 last, a huge dust storm developed in its atmosphere. By the end of June the dust storm had completely enveloped the planet, totally obscuring the normally easily visible surface features and rendering the planet relatively featureless. The Mars rover Opportunity switched off its sensors and other facilities, as the storm turned the sky dark on Mars, and the solar panels on Opportunity were not providing enough electrical power to maintain normal operations, putting it into 'sleep' mode. In August the storm began to dissipate, and some surface features became faintly visible, but not clear. The rover Curiosity, being nuclear powered and independent of sunlight, has continued to work, but the dust has meant that its cameras cannot operate properly. We hope that the storm completely clears before we leave Mars too far behind, so that we can observe details on Mars again, and enabling Opportunity to 'wake up' and resume its work.

The next time that Mars will have an opposition in which it reaches a size as favourable as the current one will be in September 2035, when Mars will be in the constellation Aquarius. The next opposition will occur in just over two years time, on October 14, 2020. Mars will become almost as big as this year (22 arcseconds), but being in the constellation Pisces will not be so favourably placed in the sky, having an altitude at culmination of only 58 degrees.

On October 18, the waxing gibbous Moon will be just to the north (left) of Mars in the early evening sky.

On November 11 Mars will cross into Aquarius, on December 21 it will move into Pisces, on February 13 next it will move into Aries, and on March 23 Mars will enter Taurus. By then the speeding Earth will have left it far behind, and its angular diameter will have fallen from the value in mid-October of 14 arcseconds to only 5 arcseconds next March.

In this image, the south polar cap of Mars is easily seen. Above it is a dark triangular area known as Syrtis Major. Dark Sinus Sabaeus runs off to the left, just south of the equator. Between the south polar cap and the equator is a large desert called Hellas. The desert to upper left is known as Aeria, and that to the north-east of Syrtis Major is called Isidis Regio.  Photograph taken in 1971.



Mars photographed from Starfield Observatory, Nambour on June 29 and July 9, 2016, showing two different sides of the planet.  The north polar cap is prominent.

 

Brilliant Mars at left, shining at magnitude 0.9, passes in front of the dark molecular clouds in Sagittarius on October 15, 2014. At the top margin is the white fourth magnitude star 44 Ophiuchi. Its type is A3 IV:m. Below it and to the left is another star, less bright and orange in colour. This is the sixth magnitude star SAO 185374, and its type is K0 III. To the right (north) of this star is a dark molecular cloud named B74. A line of more dark clouds wends its way down through the image to a small, extremely dense cloud, B68, just right of centre at the bottom margin. In the lower right-hand corner is a long dark cloud shaped like a figure 5. This is the Snake Nebula, B72. Above the Snake is a larger cloud, B77. These dark clouds were discovered by Edward Emerson Barnard at Mount Wilson in 1905. He catalogued 370 of them, hence the initial 'B'. The bright centre of our Galaxy is behind these dark clouds, and is hidden from view. If the clouds were not there, the galactic centre would be so bright that it would turn night into day.


Mars near opposition, July 24, 2018


Mars, called the red planet but usually coloured orange, has now taken on a yellowish tint and has brightened by 0.4 magnitude, making it twice as bright as previous predictions for the July 27 opposition. These phenomena have been caused by a great dust storm which has completely encircled the planet, obscuring the surface features so that they are only seen faintly through the thick curtain of dust. Although planetary photographers are mostly disappointed, many observers are interested to see that the yellow colour and increased brightness mean that a weather event on a distant planet can actually be detected with the unaided eye - a very unusual thing in itself.

The three pictures above were taken on the evening of July 24, at 9:05, 9:51 and 11:34 pm. Although the fine details that are usually seen on Mars are hidden by the dust storm, some of the larger features can be discerned, revealing how much Mars rotates in two and a half hours. Mars' sidereal rotation period (the time taken for one complete rotation or 'Martian day') is 24 hours 37 minutes 22 seconds - a little longer than an Earth day. The dust storm began in the Hellas Desert on May 31, and after two months it still enshrouded the planet. In August it began to clear.
 

Central meridian: 295º.
 

 

The two pictures immediately above were taken on the evening of September 7, at 6:25 and 8:06 pm. The dust storm is finally abating, and some of the surface features are becoming visible once again. This pair of images also demonstrates the rotation of Mars in 1 hour 41 minutes (equal to 24.6 degrees of longitude), but this time the view is of the opposite side of the planet to the set of three above. As we are now leaving Mars behind, the images are appreciably smaller (the angular diameter of the red planet has fallen to 20 arcseconds). Well past opposition, Mars on September 7 exhibited a phase effect of 92.65 %.


 
Central meridian: 180º.

 

Jupiter:   On October 1, this gas giant planet is only visible in the sky for a couple of hours after twilight fades, low in the west. It is in the centre of the constellation Libra, the Scales. It spends the month less than half-a-handspan above the star Zuben Elgenubi, which is the brightest star in Libra. As October progresses, Jupiter will be found closer to the sunset point for a given time each night. Brighter Venus will be close by. In the second half of the month we will lose Venus, leaving Jupiter alone. Jupiter will pass on the far side of the Sun (conjunction) on November 26, and will also disappear from out evening sky. In December, both Jupiter and Venus will reappear in the eastern pre-dawn sky. The waxing crescent Moon will be seen just to the north of Jupiter soon after sunset on October 11 and 12.

       

Jupiter as photographed from Nambour on the evening of April 25, 2017. The images were taken, from left to right, at 9:10, 9:23, 9:49, 10:06 and 10:37 pm. The rapid rotation of this giant planet in a little under 10 hours is clearly seen. In the southern hemisphere, the Great Red Spot (bigger than the Earth) is prominent, sitting within a 'bay' in the South Tropical Belt. South of it is one of the numerous White Spots. All of these are features in the cloud tops of Jupiter's atmosphere.



Jupiter as it appeared at 7:29 pm on July 2, 2017. The Great Red Spot is in a similar position near Jupiter's eastern limb (edge) as in the fifth picture in the series above. It will be seen that in the past two months the position of the Spot has drifted when compared with the festoons in the Equatorial Belt, so must rotate around the planet at a slower rate. In fact, the Belt enclosing the Great Red Spot rotates around the planet in 9 hours 55 minutes, and the Equatorial Belt takes five minutes less. This high rate of rotation has made the planet quite oblate. The prominent 'bay' around the Red Spot in the five earlier images appears to be disappearing, and a darker streak along the northern edge of the South Tropical Belt is moving south. Two new white spots have developed in the South Temperate Belt, west of the Red Spot. The five upper images were taken near opposition, when the Sun was directly behind the Earth and illuminating all of Jupiter's disc evenly. The July 2 image was taken just four days before Eastern Quadrature, when the angle from the Sun to Jupiter and back to the Earth was at its maximum size. This angle means that we see a tiny amount of Jupiter's dark side, the shadow being visible around the limb of the planet on the left-hand side, whereas the right-hand limb is clear and sharp. Three of Jupiter's Galilean satellites are visible, Ganymede to the left and Europa to the right. The satellite Io can be detected in a transit of Jupiter, sitting in front of the North Tropical Belt, just to the left of its centre.  
 

Jupiter at opposition, May 9, 2018

     

Jupiter reached opposition on May 9, 2018 at 10:21 hrs, and the above photographs were taken that evening, some ten to twelve hours later. The first image above was taken at 9:03 pm, when the Great Red Spot was approaching Jupiter's central meridian and the satellite Europa was preparing to transit Jupiter's disc. Europa's transit began at 9:22 pm, one minute after its shadow had touched Jupiter's cloud tops. The second photograph was taken three minutes later at 9:25 pm, with the Great Red Spot very close to Jupiter's central meridian.

The third photograph was taken at 10:20 pm, when Europa was approaching Jupiter's central meridian. Its dark shadow is behind it, slightly below, on the clouds of the North Temperate Belt. The shadow is partially eclipsed by Europa itself. The fourth photograph at 10:34 pm shows Europa and its shadow well past the central meridian. Europa is the smallest of the Galilean satellites, and has a diameter of 3120 kilometres. It is ice-covered, which accounts for its brightness and whitish colour. Jupiter's elevation above the horizon for the four photographs in order was 50º, 55º, 66º and 71º. As the evening progressed, the air temperature dropped a little and the planet gained altitude. The 'seeing' improved slightly, from Antoniadi IV to Antoniadi III. At the time of the photographs, Europa's angular diameter was 1.57 arcseconds. Part of the final photograph is enlarged below.

Jupiter at 11:34 pm on May 18, ten days later. Changes in the rotating cloud patterns are apparent, as some cloud bands rotate faster than others and interact. Compare with the first photograph in the line of four taken on May 9. The Great Red Spot is ploughing a furrow through the clouds of the South Tropical Belt, and is pushing up a turbulent bow wave.
 


Saturn:
   The ringed planet reached opposition on June 27 and is now ideally placed for observing, being almost exactly overhead at 6:20 pm at mid-month. Saturn is presently the brightest object in that part of the sky, brighter than any nearby stars, although outshone by Mars and Jupiter (Mars is about one-and-a-half handspans east, and Jupiter a little over two handspans west). On September 7 Saturn will be close to two of the best nebulae in the sky, the Lagoon Nebula (M8) and the Trifid Nebula (M20). All three will be within a 2.1 degree circle. Saturn will remain in the constellation Sagittarius all year. The waxing crescent Moon will be close to Saturn on October 15.

 

Left: Saturn showing the Rings when edge-on.    Right: Over-exposed Saturn surrounded by its satellites Rhea, Enceladus, Dione, Tethys and Titan - February 23/24, 2009. <




 Saturn with its Rings wide open on July 2, 2017. The shadow of its globe can just be seen on the far side of the Ring system. There are three main concentric rings: Ring A is the outermost, and is separated from the brighter Ring B by a dark gap known as the Cassini Division, which is 4800 kilometres wide, enough to drop Australia through. Ring A also has a gap inside it, but it is much thinner. Called the 'Encke Gap', it is only 325 kilometres wide and can be seen in the image above. The innermost parts of Ring B are not as bright as its outermost parts. Inside Ring B is the faint Ring C, almost invisible but noticeable where it passes in front of the bright planet as a dusky band. Spacecraft visiting Saturn have shown that there are at least four more Rings, too faint and tenuous to be observable from Earth, and some Ringlets. Some of these extend from the inner edge of Ring C to Saturn's cloudtops. The Rings are not solid, but are made up of countless small particles, 99.9% water ice with some rocky material, all orbiting Saturn at different distances and speeds. The bulk of the particles range in size from dust grains to car-sized chunks. At bottom centre, the southern hemisphere of the planet can be seen showing through the gap of the Cassini Division. The ring system extends from 7000 to 80 000 kilometres above Saturn's equator, but its thickness varies from only 10 metres to 1 kilometre. The globe of Saturn has a diameter at its equator of 120 536 kilometres. Being made up of 96% hydrogen and 3% helium, it is a gas giant, although it has a small, rocky core. There are numerous cloud bands visible.

The photograph above was taken when Saturn was close to opposition, with the Earth between Saturn and the Sun. At that time, the shadow of Saturn's globe upon the Ring system was directly behind the planet and hardly visible. The photograph below was taken at 7:14 pm on September 09, 2018, when Saturn was near eastern quadrature. At such a time, the angle from the Sun to Saturn and back to the Earth is near its maximum, making the shadow fall at an angle across the Rings as seen from Earth. It may be seen falling across the far side of the Ring to the left side of the globe.

 

 

Uranus:  This ice giant planet is observable from about 8 pm on this month, as it will reach opposition (rising in the east as the Sun sets in the west) on October 24. Uranus shines at about magnitude 5.8, so a pair of binoculars or a small telescope is required to observe it. It is currently in the south-western corner of the constellation Aries, near the eastern boundary of Pisces. At mid-month it rises at about 6:30 pm. The almost Full Moon will be in the vicinity of Uranus in the early hours of October 24.

 

Neptune:   The icy blue planet reached opposition on September 8, so will be observable this month for most of the night. On October 1 it is about two handspans above the eastern horizon as darkness falls. The waxing gibbous Moon will be in the vicinity of Neptune on October 20 and 21.

Neptune, photographed from Nambour on October 31, 2008


Pluto: 
 The erstwhile ninth and most distant planet reached opposition on July 12 and is well-placed for viewing this month, as it will be about a handspan west of the zenith as darkness falls. Pluto's angular diameter is 0.13 arcseconds, less than one twentieth that of Neptune. Located just east of the 'Teaspoon' which is north-east of the Sagittarius 'Teapot', it is a faint 14.1 magnitude object near the centre of Sagittarius. A telescope with an aperture of 25 cm or more is necessary to observe Pluto. The First Quarter Moon will be in the vicinity of Pluto on the night of October 16.

 

  

The movement of the dwarf planet Pluto in two days, between 13 and 15 September, 2008. Pluto is the one object that has moved.
Width of field:   200 arcseconds

This is a stack of four images, showing the movement of Pluto over the period October 22 to 25, 2014. Pluto's image for each date appears as a star-like point at the upper right corner of the numerals. The four are equidistant points on an almost-straight line. Four eleventh magnitude field stars are identified.  A is GSC 6292:20, mv = 11.6.  B is GSC 6288:1587, mv = 11.9.  C is GSC 6292:171, mv = 11.2.  D is GSC 6292:36, mv = 11.5.  (GSC = Guide Star Catalogue).   The position of Pluto on October 24 (centre of image) was at Right Ascension = 18 hours 48 minutes 13 seconds,  Declination =  -20º 39' 11".  The planet moved 2' 51" with respect to the stellar background during the three days between the first and last images, or 57 arcseconds per day, or 1 arcsecond every 25¼ minutes.






Meteor Showers:


Orionids                      October 22                                  Thin waxing crescent Moon, 6% sunlit                                         ZHR = 20
                                    Radiant:   Near the bright star Betelgeuse.  Associated with Comet Halley


Use this 
Fluxtimator  to calculate the number of meteors predicted per hour for any meteor swarm on any date, for any place in the world.


ZHR = zenithal hourly rate (number of meteors expected to be observed at the zenith in one hour). The maximum phase of meteor showers usually occurs between 3 am and sunrise. The reason most meteors are observed in the pre-dawn hours is because at that time we are on the front of the Earth as it rushes through space at 107 000 km per hour (30 km per second). We are meeting the meteors head-on, and the speed at which they enter our atmosphere is the sum of their own speed plus ours. In the evenings, we are on the rear side of the Earth, and many meteors we see at that time are actually having to catch us up. This means that the speed at which they enter our atmosphere is less than in the morning hours, and they burn up less brilliantly.

Although most meteors are found in swarms associated with debris from comets, there are numerous 'loners', meteors travelling on solitary paths through space. When these enter our atmosphere, unannounced and at any time, they are known as 'sporadics'. Oan average clear and dark evening, an observer can expect to see about ten meteors per hour. They burn up to ash in their passage through our atmosphere. The ash slowly settles to the ground as meteoric dust. The Earth gains about 80 tonnes of such dust every day, so a percentage of the soil we walk on is actually interplanetary in origin. If a meteor survives its passage through the air and reaches the ground, it is called a 'meteorite'.  In the past, large meteorites (possibly comet nuclei or small asteroids) collided with the Earth and produced huge craters which still exist today. These craters are called 'astroblemes'. Two famous ones in Australia are Wolfe Creek Crater and Gosse's Bluff. The Moon and Mercury are covered with such astroblemes, and craters are also found on Venus, Mars, planetary satellites, minor planets, asteroids and even comets.




 

Comets:

Green comets in the news

Comet PANSTARRS (C/2017 S3)

A comet that may become visible to the naked eye exploded in brightness, suddenly increasing its luminosity 16-fold on July 1. Whatever happened on Comet PANSTARRS (C/2017 S3) has given it an expanding green atmosphere almost twice the size of the planet Jupiter. Visit the July 4 edition of  Spaceweather   and subsequent news releases for pictures and more information about this comet.

Comet 21P/Giacobini-Zinner

On September 10, another green comet will make its closest approach to Earth in 72 years. This small but active comet is named Comet 21P/Giacobini-Zinner. The 'P' indicates that it is a periodic comet in an elliptical orbit around the Sun, and returning regularly for us to see. After it passes Earth, it will swing around the Sun and head out towards the furthest point in its orbit, just beyond Jupiter. After 36 years it will head back towards the Sun.

This month it will shine at magnitude 7 so it will be easy to see in small telescopes and binoculars, but not with the unaided eye. It will only be observable in the hour or so before dawn begins to light the sky, low to the north-east horizon. On September 10 it will be gliding through the stars of the constellation Auriga about 58 million kilometres from our planet. In the week ahead, it will cross into Gemini and on September 15 it will pass right across the rich star cluster M35, providing a spectacular photo-opportunity for amateur astronomers. Visit the September 9 edition of  Spaceweather  for details and observing tips.


Comet Lulin

This comet, (C/2007 N3), discovered in 2007 at Lulin Observatory by a collaborative team of Taiwanese and Chinese astronomers, is now in the outer Solar System, and has faded below magnitude 15.

Comet Lulin at 11:25 pm on February 28, 2009, in Leo. The brightest star is Nu Leonis, magnitude 5.26.

 

The LINEARrobotic telescope operated by Lincoln Near Earth Asteroid Research is used to photograph the night skies, searching for asteroids which may be on a collision course with Earth. It has also proved very successful in discovering comets, all of which are named ‘Comet LINEAR’ after the centre's initials. This name is followed by further identifying letters and numbers. Generally though, comets are named after their discoverer, or joint discoverers. There are a number of other comet and near-Earth asteroid search programs using robotic telescopes and observatory telescopes, such as:
Catalina Sky Survey, a consortium of three co-operating surveys, one of which is the Australian Siding Springs Survey (below),
Siding Spring Survey, using the 0.5 metre Uppsala Schmidt telescope at Siding Spring Observatory, N.S.W., to search the southern skies,
LONEOS, (Lowell Observatory Near-Earth Object Search), concentrating on finding near-Earth objects which could collide with our planet,
Spacewatch, run by the Lunar and Planetary Laboratory of the University of Arizona,
Ondrejov, run by Ondrejov Observatory of the Academy of Sciences in the Czech Republic, 
Xinglong, run by Beijing Astronomical Observatory 

Nearly all of these programs are based in the northern hemisphere, leaving gaps in the coverage of the southern sky. These gaps are the areas of sky where amateur astronomers look for comets from their backyard observatories.

To find out more about current comets, including finder charts showing exact positions and magnitudes, click here. To see pictures of these comets, click here.

 

The 3.9 metre Anglo-Australian Telescope (AAT) at the Australian Astronomical Observatory near Coonabarabran, NSW.

 

 

 

Deep Space

 

 

Sky Charts and Maps available on-line:


There are some useful representations of the sky available here. The sky charts linked below show the sky as it appears to the unaided eye. Stars rise four minutes earlier each night, so at the end of a week the stars have gained about half an hour. After a month they have gained two hours. In other words, the stars that were positioned in the sky at 8 pm at the beginning of a month will have the same positions at 6 pm by the end of that month. After 12 months the stars have gained 12 x 2 hours = 24 hours = 1 day, so after a year the stars have returned to their original positions for the chosen time. This accounts for the slow changing of the starry sky as the seasons progress.

The following interactive sky charts are courtesy of Sky and Telescope magazine. They can simulate a view of the sky from any location on Earth at any time of day or night between the years 1600 and 2400. You can also print an all-sky map. A Java-enabled web browser is required. You will need to specify the location, date and time before the charts are generated. The accuracy of the charts will depend on your computer’s clock being set to the correct time and date.

To produce a real-time sky chart (i.e. a chart showing the sky at the instant the chart is generated), enter the name of your nearest city and the country. You will also need to enter the approximate latitude and longitude of your observing site. For the Sunshine Coast, these are:

latitude:   26.6o South                      longitude:   153o East

Then enter your time, by scrolling down through the list of cities to "Brisbane: UT + 10 hours". Enter this one if you are located near this city, as Nambour is. The code means that Brisbane is ten hours ahead of Universal Time (UT), which is related to Greenwich Mean Time (GMT), the time observed at longitude 0o, which passes through London, England. Click here to generate these charts.

_____________________________________


Similar real-time charts can also be generated from another source, by following this second link:

Click here for a different real-time sky chart.

The first, circular chart will show the full hemisphere of sky overhead. The zenith is at the centre of the circle, and the cardinal points are shown around the circumference, which marks the horizon. The chart also shows the positions of the Moon and planets at that time. As the chart is rather cluttered, click on a part of it to show that section of the sky in greater detail. Also, click on Update to make the screen concurrent with the ever-moving sky.

The stars and constellations around the horizon to an elevation of about 40o can be examined by clicking on

View horizon at this observing site

The view can be panned around the horizon, 45 degrees at a time. Scrolling down the screen will reveal tables showing setup and customising options, and an Ephemeris showing the positions of the Sun, Moon and planets, and whether they are visible at the time or not. These charts and data are from YourSky, produced by John Walker.

The charts above and the descriptions below assume that the observer has a good observing site with a low, flat horizon that is not too much obscured by buildings or trees. Detection of fainter sky objects is greatly assisted if the observer can avoid bright lights, or, ideally, travel to a dark sky site. On the Sunshine Coast, one merely has to travel a few kilometres west of the coastal strip to enjoy magnificent sky views. On the Blackall Range, simply avoid streetlights. Allow your eyes about 15 minutes to become dark-adapted, a little longer if you have been watching television. Small binoculars can provide some amazing views, and with a small telescope, the sky’s the limit.

In August, the Eta Carinae Nebula is best viewed in the early evening, to the south-west of the Southern Cross.

 

 

 

The Stars and Constellations for this month:

 

These descriptions of the night sky are for 9 pm on October 1 and 7 pm on October 31. Broadly speaking, the following description starts low in the north-west and follows the horizon to the right, heading round to the east, then south, then west, then overhead and back to the north-west.


Setting towards the north-west is the constellation of Cygnus, the Swan. Cygnus is also known as the Northern Cross, but to us in the southern hemisphere it appears this month lying on its right-hand side. The star at the bottom of the Cross, or on its upper left as we see it tonight, is a beautiful double star or binary, called Albireo.

Whereas most binaries are a pair of similar stars, there are many in which the two stars are very different, such as brilliant Sirius the Dog Star with its tiny white dwarf companion known as 'The Pup'. Albireo's two components have a marked colour contrast, the brighter star being a golden yellow, and the fainter companion being a vivid electric blue. It is a wonderful object to view with a small telescope.

At the top of the Northern Cross is the brightest star in the constellation. It appears close to the north-north-western horizon tonight. This star is the first magnitude star Deneb, or Alpha Cygni. Deneb is a white giant star, and is the nineteenth brightest in the sky. Its name is Arabic for 'tail'. It will be due north at about 7.00 pm at mid-month.

High in the sky and approaching culmination is the Great Square of Pegasus. It will be standing directly above the northern horizon at 9.30 pm at mid-month. It is very large, each side being around 15 degrees long. It is about as large as a fist held at arm's length, and is a similar distance above the horizon. The Great Square is remarkable for having few naked-eye stars within it.

The names of the four stars marking the corners of the Square (starting at the top-left one and moving in a clockwise direction around the Square) are Markab, Algenib, Alpheratz and Scheat. Although these four stars are known as the Great Square of Pegasus, only three are actually in the constellation of Pegasus, the Winged Horse. In point of fact, Alpheratz is the brightest star of the constellation Andromeda, the Chained Maiden.

Andromeda trails down from Alpheratz below the north-eastern horizon. To its right is the zodiacal constellation of Aries, now risen in the north-east. The brightest star in Aries is a second magnitude orange star called Hamal. Above it is the white star Sheratan, slightly fainter. Just below the horizon is Taurus, soon to rise.

In the east, a mv 2.2 star is about halfway up the sky. This is Beta Ceti, the brightest ordinary star in the constellation Cetus, the Whale. Its common name is Diphda, and it has a yellowish-orange colour. By rights, the star Menkar being also known as Alpha Ceti should be brighter, but Menkar is actually more than half a magnitude fainter than Diphda. Menkar may be seen rising above the east-north-eastern horizon.

Cetus is a large constellation, running around the eastern horizon tonight, and to the unaided eye it appears unremarkable. But it does contain a most interesting star, which even ancient peoples noticed. The astronomer Hevelius named it Mira, the Wonderful (see below). Between Cetus and Pegasus is the zodiacal constellation of Pisces, the Fishes. Pisces is found just above Aries, and contains a faint ring of stars, known as the 'Circlet'. The planet Uranus is about 24 degrees to the east of the Circlet this month, between the stars Alrescha and Algenib.

Above Diphda is Fomalhaut, a bright, white first magnitude star in the faint constellation Piscis Austrinus, the Southern Fish. Above Fomalhaut and to the right is a large, flattened triangle of stars, Grus, the Crane. Fomalhaut and Grus are both almost directly overhead at this time.

Very high in the south-east is Achernar, which is the ninth brightest star. It is the main star in the constellation Eridanus the River, which winds its way from Achernar towards the eastern horizon below Cetus. It then continues below the horizon all the way to Orion, which this month will not rise above the eastern horizon until a little after 10.00 pm.

Achernar's visual magnitude ( mv ) is  0.45, and it is a hot blue-white star of B3 spectral type. The width of the field is 24 arcminutes and the faintest stars are mv 15.

 

Between Achernar and the south-eastern horizon can be seen the brilliant supergiant Canopus rising in the south-east. Canopus is the second-brightest star in the night sky, being outshone only by Sirius, which is smaller but much closer.

To the left of Achernar, the faint constellation of Phoenix may be seen. Its brightest star is Ankaa, a mv 2.39 star which is halfway between Diphda and Achernar, but slightly above.

A little to the east of due south, the Large Magellanic Cloud (LMC) is gaining altitude. The Small Magellanic Cloud (SMC) is about a handspan above it, and to the right of Achernar. Both of these Clouds appear as faint smudges of light, but in reality they are dwarf galaxies containing millions of stars.

From our latitude both Magellanic Clouds are circumpolar. This means that they are closer to the South Celestial Pole than that Pole's altitude above the horizon, so they never dip below the horizon. They never rise nor set, but are always in our sky. Of course, they are not visible in daylight, but they are there, all the same.

The Southern Cross is almost out of sight below the southern horizon, and Alpha and Beta Centauri are setting nearby. Near the west-south-western horizon, we see the bright S-shaped constellation of Scorpius, the Scorpion, with the red-supergiant star Antares marking the Scorpion's heart. The planet Saturn is in the adjoining constellation of Sagittarius, the Archer, which is about 45º above the south-western horizon, just above Scorpius. The star clouds in the centre of our Milky Way galaxy lie behind the stars of Sagittarius. Saturn will spend all of October slowly moving eastward through Sagittarius.

Antares, a red supergiant star

The star which we call Antares is a binary system. It is dominated by the great red supergiant Antares A which, if it swapped places with our Sun, would enclose all the planets out to Jupiter inside itself. Antares A is accompanied by the much smaller Antares B at a distance of between 224 and 529 AU - the estimates vary. (One AU or Astronomical Unit is the distance of the Earth from the Sun, or about 150 million kilometres or 8.3 light minutes.)  Antares B is a bluish-white companion, which, although it is dwarfed by its huge primary, is actually a main sequence star of type B2.5V, itself substantially larger and hotter than our Sun. Antares B is difficult to observe as it is less than three arcseconds from Antares A and is swamped in the glare of its brilliant neighbour. It can be seen in the picture above, at position angle 277 degrees (almost due west or to the left) of Antares A. Seeing at the time was about IV on the Antoniadi Scale, or in other words below fair. Image acquired at Starfield Observatory in Nambour on July 1, 2017.

The Trifid Nebula, M20, in Sagittarius, is composed of a reflection nebula (blue), an emission nebula (pink), and dark lanes of dust.

The centre of our galaxy is teeming with stars, and would be bright enough to turn night into day, were it not for intervening dust and molecular clouds. This dark cloud was discovered by Edward Emerson Barnard in 1905 and is known as B72, 'The Snake'. A satellite passed through the field of view at right.

 

East of Sagittarius and a little to the west of the zenith is Capricornus, the Sea-Goat. This month it is dominated by the bright, orange planet Mars. Between Capricornus and Pisces is a rather faint constellation, Aquarius, the Water Bearer. Aquarius is almost directly overhead at this time, and this year contains the faint planet Neptune, which lies about half a handspan south of the asterism known as the 'Water Jar'. Mars will cross into Aquarius on November 11.

The constellations Sagittarius (top) and Scorpius (bottom), with the elegant curve of Corona Australis to the left of Sagittarius. They are high in the west at 8.00 pm this month.

 

High in the north-west, between Capricornus and Albireo, is the constellation of Aquila, the Eagle. The centre of this constellation is marked by a short line of three stars, of which the centre star is the brightest. These stars, from left to right, are Tarazed, Altair and Alshain, and they indicate the Eagle's body. A handspan east of the bright, first magnitude Altair is a faint but easily recognised diamond-shaped group of stars, Delphinus the Dolphin.

Vega is the brightest star at centre left, with the stars of Lyra to its right. Deneb is the brightest star near the bottom edge. Cygnus, or the 'Northern Cross', stretches up vertically from Deneb to Albireo, above centre. We see the Northern Cross upside-down. The three bright stars of Aquila form a line at upper right, with Altair, the brightest, being the middle one. The small diamond-shaped constellation of Delphinus, the Dolphin, is above centre-right.

 

The zodiacal constellations visible tonight, starting from the west-south-western horizon and heading north-east, are Scorpius, Sagittarius, Capricornus, Aquarius, Pisces and Aries.

More photographs of the amazing sights visible in our sky this month are found in our Picture Gallery.

If you would like to become familiar with the constellations, we suggest that you access one of the world's best collections of constellation pictures by clicking here. To see some of the best astrophotographs taken with the giant Anglo-Australian telescope, click here.


 

Mira, the Wonderful


The amazing thing about the star Mira or Omicron Ceti is that it varies dramatically in brightness, rising to magnitude 2 (brighter than any other star in Cetus), and then dropping to magnitude 10 (requiring a telescope to detect it), over a period of 332 days.

This drop of eight magnitudes means that its brightness diminishes over a period of five and a half months to one six-hundredth of what it had been, and then over the next five and a half months it regains its original brightness.

The seventeenth century Polish astronomer Johannes Hevelius named it Mira, meaning 'The Wonderful' or 'The Miraculous One'.

We now know that many stars vary in brightness, even our Sun doing so to a small degree, with a period of 11 years. One type of star varies, not because it is actually becoming less bright in itself, but because another, fainter star moves around it in an orbit roughly in line with the Earth, and obscures it on each pass. This type of star is called an eclipsing variable and they are very common.

The star Mira though, varies its light output because of processes in its interior. It is what is known as a pulsating variable. Stars of the Mira type are giant pulsating red stars that vary between 2.5 and 11 magnitudes in brightness. They have long, regular periods of pulsation which lie in the range from 80 to 1000 days.

Last year, Mira reached a maximum brightness of magnitude 3.4 on December 29, 2017 and has now dropped well below naked-eye visibility (magnitude 6) again. It reached its minimum brightness of magnitude 9.3 on August 18. This month Mira will begin to brighten again, and the next maximum will occur on November 26 next.

    

Mira near minimum, 26 September 2008                Mira near maximum, 22 December 2008

 

Astronomers using a NASA space telescope, the Galaxy Evolution Explorer, have spotted an amazingly long comet-like tail behind Mira as the star streaks through space.

Galaxy Evolution Explorer - "GALEX" for short - scanned the well-known star during its ongoing survey of the entire sky in ultraviolet light. Astronomers then noticed what looked like a comet with a gargantuan tail. In fact, material blowing off Mira is forming a wake 13 light-years long, or about 20,000 times the average distance of Pluto from the sun. Nothing like this has ever been seen before around a star.   More, including pictures

 

 

Double and multiple stars


Estimate
s vary that between 15% and 50% of stars are single bodies like our Sun, although the latest view is that less than 25% of stars are solitary. At least 30% of stars and possibly as much as 60% of stars are in double systems, where the two stars are gravitationally linked and orbit their mutual centre of gravity. Such double stars are called binaries. The remaining 20%+ of stars are in multiple systems of three stars or more. Binaries and multiple stars are formed when a condensing Bok globule or protostar splits into two or more parts.

Binary stars may have similar components (Alpha Centauri A and B are both stars like our Sun), or they may be completely dissimilar, as with Albireo (Beta Cygni, where a bright golden giant star is paired with a smaller bluish main sequence star).

     

The binary stars Rigil Kent (Alpha Centauri) at left, and Beta Cygni (Albireo), at right.

     

The binary star Rigel (Beta Orionis, left) is a large white supergiant which is 500 times brighter than its small companion, Rigel B, Yet Rigel B is itself composed or a very close pair of Sun-type stars that orbit each other in less than 10 days. In the centre of the Great Nebula in Orion (M42) is a multiple star known as the Trapezium (right). This star system has four bright white stars, two of which are binary stars with fainter red companions, giving a total of six. The hazy background is caused by the cloud of fluorescing hydrogen comprising the nebula.

Acrux, the brightest star in the Southern Cross, is also known as Alpha Crucis.  It is a close binary, circled by a third dwarf companion.

 

Alpha Centauri (also known as Rigil Kentaurus, Rigil Kent or Toliman) is a binary easily seen with a small telescope. The components are both solar-type main sequence stars, one of type G and the other, slightly cooler and fainter, of type K. Through a telescope this star system looks like a pair of distant but bright car headlights. Alpha Centauri A and B take 80 years to complete an orbit, but a tiny third component, the 11th magnitude red dwarf Proxima Centauri, takes about 1 million years to orbit the other two. It is about one tenth of a light year from the bright pair and a little closer to us, hence its name. This makes it our nearest interstellar neighbour, with a distance of 4.3 light years. Red dwarfs are by far the most common type of star, but, being so small and faint, none is visible to the unaided eye. Because they use up so little of their energy, they are also the longest-lived of stars. The bigger a star is, the shorter its life.

Close-up of the star field around Proxima Centauri

 

Knowing the orbital period of the two brightest stars A and B, we can apply Kepler’s Third Law to find the distance they are apart. This tells us that Alpha Centauri A and B are about 2700 million kilometres apart or about 2.5 light hours. This makes them a little less than the distance apart of the Sun and Uranus (the orbital period of Uranus is 84 years, that of Alpha Centauri A and B is 80 years.)

Albireo (Beta Cygni) is sometimes described poetically as a large topaz with a small blue sapphire. It is one of the sky’s most beautiful objects. The stars are of classes G and B, making a wonderful colour contrast. It lies at a distance of 410 light years, 95 times further away  than Alpha Centauri.

Binary stars may be widely spaced, as the two examples just mentioned, or so close that a telescope is struggling to separate them (Acrux, Antares, Sirius). Even closer double stars cannot be split by the telescope, but the spectroscope can disclose their true nature by revealing clues in the absorption lines in their spectra. These examples are called spectroscopic binaries. In a binary system, closer stars will have shorter periods for the stars to complete an orbit. Eta Cassiopeiae takes 480 years for the stars to circle each other. The binary with the shortest period is AM Canum Venaticorum, which takes only 17½ minutes.

Sometimes one star in a binary system will pass in front of the other one, partially blocking off its light. The total light output of the pair will be seen to vary, as regular as clockwork. These are called eclipsing binaries, and are a type of variable star, although the stars themselves usually do not vary.

 

 

The Milky Way


A glowing band of light crossing the sky is especially noticeable during the winter months, and to a lesser extent in the spring, when it appears more to the west. This glow is the light of millions of faint stars combined with that coming from glowing gas clouds called nebulae. It is concentrated along the plane of our galaxy, and this month it is seen crossing the western half of the sky, starting from the south-south-west and passing through Crux to Norma, Ara, Scorpius, Sagittarius, Scutum and Aquila to Cygnus in the north-north-west.

The plane of our galaxy from Scutum (at left) through Sagittarius and Scorpius (centre) to Centaurus and Crux (right). The Eta Carinae nebula is at the right margin, below centre. The Coalsack is clearly visible, and the dark dust lanes can be seen. Taken with an ultra-wide-angle lens.

 

It is rewarding to scan along this band with a pair of binoculars, looking for star clusters and emission nebulae. Dust lanes along the plane of the Milky Way appear to split it in two in some parts of the sky. One of these lanes can be easily seen, starting near Alpha Centauri and heading towards Antares.

The centre of our galaxy. The constellations partly visible here are Sagittarius (left), Ophiuchus (above centre) and Scorpius (at right). The planet Jupiter is the bright object below centre left. This is a normal unaided-eye view.

 

 

The Season of the Scorpion


The spectacular constellation of Scorpius is about a handspan above the western horizon at about 8.00 pm in mid-October. Three bright stars in a gentle curve mark his head, and another three mark his body. Of this second group of three, the centre one is a bright, red supergiant, Antares. It marks the red heart of the scorpion. This star is so large that, if it swapped places with our Sun, it would engulf the Earth and extend to the orbit of Mars. It is 604 light years away and shines at magnitude 1.06. Antares, an M type star, has a faint companion which can be seen in a good amateur telescope.

The rest of the stars run around the scorpion's tail, ending with two blue-white B type stars, Shaula (the brighter of the two) and Lesath, at the tip of the scorpion's sting. These two stars are at the eastern end of the constellation, and are near the top of the picture below. West of Lesath in the body of the scorpion is an optical double star, which can be seen as two with the unaided eye.

Scorpius, with its head at lower right, and the tail (with sting) at upper left.

 

Probably the two constellations most easily recognisable (apart from Crux, the Southern Cross) are Orion the Hunter and Scorpius the Scorpion. Both are large constellations containing numerous bright stars, and are very obvious 'pictures in the sky'. Both also contain a very bright red supergiant star, Betelgeuse in Orion and Antares in Scorpius. 

A very distant star that is easily seen with the unaided eye is Zeta Scorpii, in the tail of the Scorpion. Actually, there are two stars there, Zeta 1 and Zeta 2. Zeta 2 is an orange K-type giant star which is only 150 light years away. Zeta 1, though, is a blue-white B1 hypergiant, and at a distance of 2600 light years is over 17 times further away than Zeta 2. The light from Zeta 1 left it around 600 BC, when the Greek philosophers Socrates and Plato were alive. It can be found by following the line of the tail of Scorpius, and is the fourth star from Antares, heading south. It lies at the point where the tail takes a sharp turn east.

Zeta 1 Scorpii is the upper star in the bright group of three at centre right. Zeta 2 is below it.

The Lagoon Nebula, M8, in Sagittarius, adjacent to Scorpius

The eastern half of the Lagoon Nebula, M8, showing dark Bok globules where protostars are forming

The centre of the Lagoon Nebula

 

 

Why are some constellations bright, while others are faint ?


The Milky Way is a barred spiral galaxy some 100000 – 120000 light-years in diameter which contains 100 – 400 billion stars. It may contain at least as many planets as well. Our galaxy is shaped like a flattened disc with a central bulge. The Solar System is located within the disc, about 27000 light-years from the Galactic Centre, on the inner edge of one of the spiral-shaped concentrations of gas and dust called the Orion Arm. When we look along the plane of the galaxy, either in towards the centre or out towards the edge, we are looking along the disc through the teeming hordes of stars, clusters, dust clouds and nebulae. In the sky, the galactic plane gives the appearance which we call the Milky Way, a brighter band of light crossing the sky. This part of the sky is very interesting to observe with binoculars or telescope. The brightest and most spectacular constellations, such as Crux, Canis Major, Orion and Scorpius are located close to the Milky Way.

If we look at ninety degrees to the plane, either straight up and out of the galaxy or straight down, we are looking through comparatively few stars and gas clouds and so can see out into deep space. These are the directions of the north and south galactic poles, and because we have a clear view in these directions to distant galaxies, these parts of the sky are called the intergalactic windows. The northern window is between the constellations Virgo and Coma Berenices, roughly between the stars Denebola and Arcturus. It is out of sight this month.

The southern window is in the constellation Sculptor, not far from the star Fomalhaut. This window is in the south-east in the early evening, but later in the night it will rise high enough for distant galaxies to be observed. Some of the fainter and apparently insignificant constellations are found around these windows, and their lack of bright stars, clusters and gas clouds presents us with the opportunity to look across the millions of light years of space to thousands of distant galaxies.

 

 

Finding the South Celestial Pole 


The South Celestial Pole is that point in the southern sky around which the stars rotate in a clockwise direction. The Earth's axis is aimed exactly at this point. For an equatorially-mounted telescope, the polar axis of the mounting also needs to be aligned exactly to this point in the sky for accurate tracking to take place.

To find this point, first locate the Southern Cross. Project a line from the top of the Cross down through its base and continue straight on towards the south for another four Cross lengths. This will locate the approximate spot. There is no bright star to mark the Pole, whereas in the northern hemisphere they have Polaris (the Pole Star) to mark fairly closely the North Celestial Pole.

Another way to locate the South Celestial Pole is to draw an imaginary straight line joining Beta Centauri in the south-west to Achernar in the south-east. Both stars will be at about the same elevation above the horizon at 7.00 pm at the beginning of October. Find the midpoint of this line to locate the pole.

Interesting photographs of this area can be taken by using a camera on time exposure. Set the camera on a tripod pointing due south, and open the shutter for thirty minutes or more. The stars will move during the exposure, being recorded on the film as short arcs of a circle. The arcs will be different colours, like the stars are. All the arcs will have a common centre of curvature, which is the south celestial pole.

A wide-angle view of trails around the South Celestial Pole, with Scorpius and Sagittarius at left, Crux and Centaurus at top, and Carina and False Cross at right

Star trails between the South Celestial Pole and the southern horizon. All stars that do not pass below the horizon are circumpolar.

 

 

Star Clusters


The two clusters in Taurus, the Pleiades and the Hyades, are known as Open Clusters or Galactic Clusters. The name 'open cluster' refers to the fact that the stars in the cluster are grouped together, but not as tightly as in globular clusters (see below). The stars appear to be loosely arranged, and this is partly due to the fact that the cluster is relatively close to us, i.e. within our galaxy, hence the alternate name, 'galactic cluster'. These clusters are generally formed from the condensation of gas in a nebula into stars, and some are relatively young.

The photograph below shows a typical open cluster, M7*. It lies in the constellation Scorpius, just below the scorpion's sting, in the direction of our galaxy's centre. The cluster itself is the group of white stars in the centre of the field. Its distance is about 380 parsecs or 1240 light years. M7 is visible tonight.

Galactic Cluster M7 in Scorpius

 

Outside the plane of our galaxy, there is a halo of Globular Clusters. These are very old, dense clusters, containing perhaps several hundred thousand stars. These stars are closer to each other than is usual, and because of its great distance from us, a globular cluster gives the impression of a solid mass of faint stars. Many other galaxies also have a halo of globular clusters circling around them.

The largest and brightest globular cluster in the sky is NGC 5139** , also known as Omega Centauri. It has a slightly oval shape. It is an outstanding winter object, but is difficult to observe in October. Shining at fourth magnitude, it is faintly visible to the unaided eye, but is easily seen with binoculars, like a light in a fog. A telescope of 20 cm aperture or better will reveal its true nature, with millions of faint stars giving the impression of diamond dust on a black satin background. It lies at a distance of 5 kiloparsecs, or 16 300 light years.

The globular cluster Omega Centauri

The central core of Omega Centauri


There is another remarkable globular, second only to Omega Centauri. Close to the SMC (see below), binoculars can detect a fuzzy star. A telescope will reveal this faint glow as a magnificent globular cluster, lying at a distance of 5.8 kiloparsecs. Its light has taken almost 19 000 years to reach us. This is NGC 104, commonly known as 47 Tucanae. Some regard this cluster as being more spectacular than Omega Centauri, as it is more compact, and the faint stars twinkling in its core are very beautiful. This month, 47 Tucanae will be observable all night.

The globular cluster 47 Tucanae.


Observers aiming their telescopes towards the SMC generally also look at the nearby 47 Tucanae, but there is another globular cluster nearby which is also worth a visit. This is NGC 362, which is less than half as bright as the other globular, but this is because it is more than twice as far away. Its distance is 12.6 kiloparsecs or 41 000 light years, so it is about one-fifth of the way from our galaxy to the SMC. Both NGC 104 and NGC 362 are always above the horizon for all parts of Australia south of the Tropic of Capricorn


The globular cluster NGC 6752 in the constellation Pavo.

 

*     M42:   This number means that the Great Nebula in Orion is No. 42 in a list of 103 astronomical objects compiled and published in 1784 by Charles Messier. Charles was interested in the discovery of new comets, and his aim was to provide a list for observers of fuzzy nebulae and clusters which could easily be reported as comets by mistake. Messier's search for comets is now just a footnote to history, but his list of 103 objects is well known to all astronomers today, and has even been extended to 110 objects.

**    NGC 5139:   This number means that Omega Centauri is No. 5139 in the New General Catalogue of Non-stellar Astronomical Objects. This catalogue was first published in 1888 by J. L. E. Dreyer under the auspices of the Royal Astronomical Society, as his New General Catalogue of Nebulae and Clusters of Stars. It contained only objects that could be seen through a telescope. Soon after it appeared, the new technique of astrophotography became available, revealing thousands more faint objects in space, and also dark, obscuring nebulae and dust clouds. This meant that the NGC had to be supplemented with the addition of two Index Catalogues (IC). Many non-stellar objects in the sky have therefore NGC numbers or IC numbers. For example, the famous Horsehead Nebula in Orion is catalogued as IC 434. The NGC was revised in 1973, and lists 7840 objects. 

The recent explosion of discovery in astronomy has meant that more and more catalogues are being produced, but they tend to specialise in particular types of objects, rather than being all-encompassing, as the NGC / IC try to be. Some examples are the Planetary Nebulae Catalogue (PK) which lists 1455 nebulae, the Washington Catalogue of Double Stars (WDS) which lists 12 000 binaries, the General Catalogue of Variable Stars (GCVS) which lists 28 000 variables, and the Principal Galaxy Catalogue (PGC) which lists 73 000 galaxies. The largest modern catalogue is the Hubble Guide Star Catalogue (GSC) which was assembled to support the Hubble Space Telescope's need for guide stars when photographing sky objects. The GSC contains nearly 19 million stars brighter than magnitude 15.

 

 

Two close galaxies


Low in the south-south-east, two faint smudges of light may be seen. These are the two Clouds of Magellan, known to astronomers as the LMC (Large Magellanic Cloud) and the SMC (Small Magellanic Cloud). The LMC is directly below the SMC, and is noticeably larger. They lie at distances of 190 000 light years for the LMC, and 200 000 light years for the SMC. They are about 60 000 light years apart. These dwarf galaxies circle our own much larger galaxy, the Milky Way, and are linked to it by the Magellanic Stream. The LMC is slightly closer, but this does not account for its larger appearance. It really is larger than the SMC, and has developed as an under-sized barred spiral galaxy.

The Large Magellanic Cloud - the bright knot of gas to left of centre is the famous Tarantula Nebula.

 

Astronomers have recently reported the largest star yet found, claimed to have 300 times the mass of the Sun, located in a cluster of stars embedded in the Tarantula Nebula (above). Such a huge star would be close to the Eddington Limit, and would have a short lifespan measured in only a couple of million years.

 

These two Clouds are the closest galaxies to our own, but lie too far south to be seen by the large telescopes in Hawaii, California and Arizona. They are 15 times closer than the famous Andromeda and Triangulum galaxies, and so can be observed in much clearer detail. Our great observatories in Australia, both radio and optical, have for many years been engaged in important research involving these, our nearest inter-galactic neighbours.

 

 

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