RASC Calgary Centre - A Complete Guide to
Right Ascension and Declination

By: Larry McNish
Copyright © 2005- Larry McNish - All rights reserved.

Page last updated November 5, 2018
(Page originally created Dec 17, 2005)

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Finding Things in the Night Sky

Every star, cluster, nebula, galaxy, radio source, and quasar has a position in the night sky. All the Solar System objects - the Sun, the Moon, the other planets, asteroids, and comets have their own motion across the background of stars, so for all these objects their sky position changes hourly or daily but can be mathematically predicted.

All the textbooks, star charts, planispheres and "GOTO" computers refer to sky position coordinates - called Right Ascension and Declination.

But; What are they?, Why are they necessary? and, How can you visualize them on the night sky? This web page is designed to assist the beginning astronomer in understanding these terms, and how to apply them, just as amateur and professional astronomers the world over use them to find everything in the night sky.

Contents
Use these links to go directly to a topic, or you can read all of them by scrolling from top to bottom.
Your Observing Site
Declination
Right Ascension
Sidereal Time
The Ecliptic
Putting it all together
Polar View
Eastern View
Western View
How to use it
Precession




Your Observing Site

1.
A typical observing location - looking South The first step in any observing session is to pick a safe observing site, and for us in the Northern Hemisphere, it usually means one with a relatively clear horizon, especially towards the South.

The diagram at left will be used to show the observer (you) and your telescope at such a site on a clear dark night.

Note that the observer is looking South, with East to your left, West to your right, and North behind you.

Although we know the sky forms a complete dome over the observer, I will only show the "southern" half of the view in these diagrams or else they get too complicated.

There is one more point of interest to the observer - the point directly above you (straight "up") which is called the Zenith. Note that this is not the position of Polaris - the Pole Star. In this diagram (for mid-northern latitudes), Polaris would actually be behind you in the Northern sky, and so it is not visible in this view.

Right side viewA "right side view" of the diagram above, Right side view showing the location of Polarisand where Polaris would be behind you.

2.
The importance of knowing your Lat, Long, Date and Standard Time The next step is to know where you are and the current date and Local Standard Time. These are important because as the Earth rotates on its axis every 24 hours and also as it revolves around the Sun every year, everything "up there" moves.

A good, high-resolution topographical map or a GPS receiver can tell you where you are. Your Longitude West or East of Greenwich, England is measured in degrees from 0° to 180°. (By convention, all locations in the Western Hemisphere are specified as negative numbers so, for instance, Calgary is at (roughly) -114° Longitude.)

An accurate watch, clock or cell phone can tell you the exact time. It is then up to you to know the local regulations concerning Daylight Saving Time in order to come up with the Local Standard Time. For instance in most of North America, during Daylight Saving Time, the Standard time is one hour less than the DST clock time.


Canadian Time Zones
Canadian Time Zones
Click: NRC or Canadian Geographic Magazine for more information on Canadian Time Zones.
World Time Zones

Standard Time Zones of the World
Click: CIA or USNO for more information on World time zones.


3.
Your Meridian and your LMST Directly South of you, curving from the South point on the horizon up to the Zenith, is an imaginary line in the sky known as your Meridian. Everything in the sky left of your Meridian is rising and everything right of your Meridian is setting - just like the Sun does. Everything on your Meridian has therefore reached its highest point in the sky tonight, and is therefore at its best for viewing since it is as far as it can be away from the (murky) horizons. This is why it is important to choose a site with a clear southern horizon in step 1. (When an object reaches this highest point in the sky we say it is at its Upper Culmination (or usually we just say "Culmination". We'll talk about "Lower Culmination" later.)

Also - if you move to a different spot on the Earth, you get a slightly different view of the sky. If you move East you get to look at things that haven't risen yet at this location. If you move West you get to look at things that have already set at this location. If you move South you get to look at things that more northern observers cannot see. So, your Latitude and Longitude on Earth are two very important numbers since they, along with the date and time, determine exactly what portion of the sky you can see.

[Optional reading: Mathematically, your exact longitude along with your Time Zone (both measured from Greenwich) and your exact Local Standard Time can be used to calculate a number known as your LMST - your Local Mean Sidereal Time. If you click on this link you will be taken to a page where this is done. One thing you will see is that since your LMST involves your clock time, it is constantly changing. Another is that your LMST does not depend on your Latitude. Everyone on the same N-S longitude line has the same Meridian and LMST. There will be more on this later.]


Side view of your Meridian Side view of your Meridian animation
Click for animation

Click on the image at left to open a new window with a 231 KB animation of the stars and constellations rising in the East and setting in the West for the night of Jan 1, 2006 as seen from Calgary. (Close the new window when you are finished with it.)


4.
Your Celestial Equator So, Why do you need to know your Latitude? The answer is that your Latitude determines how far South you can see. The further South you are, the more of the Southern Sky you can see (and less of the Northern sky).

Now we have to think about the spinning Earth for a minute. The Earth spins on its N-S Axis. Polaris, the Pole star, is the star that happens to be nearest a line extended upwards from the Earth's North Pole. We can't see the South Pole region from North America. The North Pole of the Earth defines a point on the Celestial Sphere (the whole night sky) called the North Celestial Pole.

Another very important reference is the Earth's Equator. If we extend the circle describing Earth's Equator out into the sky (as we did for its axis to find Polaris) it turns out that, if you make it a large enough circle, we can see it from "up here" in the Northern Hemisphere. , and the circular Equator defines a huge circle on the Celestial Sphere called, simply the Celestial Equator. Everything North of the Celestial Equator is called the Northern Sky, and everything South of it is called the Southern Sky - you may have been using these terms without realizing that it is all defined by a circle in the sky above the Equator.

If you were on the Equator, this line would start due East, curve straight up to your Zenith and then curve straight down due West. If you were at the north Pole it would circle around your horizon just as the Equator is a circle around the Earth's axis. If you are in-between then the circle would still start exactly East and end exactly West, but would be "tilted" somewhere between your horizon and your Zenith. In fact, it would be tilted up from your Southern horizon by the amount 90° - your Latitude as shown in the diagram.

The further South you go, the higher in the sky the Celestial Equator" would be. The further North you go, the lower it would be.

Side view of your Celestial Equator
Side view of your Celestial Equator.
Earth's Celestial Equator
Earth's Celestial Equator projected out to the stars
(not to scale).

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Declination

5.
Declination OK - so we used our Longitude to define our Meridian, and our Latitude to determine where the Celestial Equator would be. So, why is this important?

The answer is that the whole coordinate system for everything up there is based on it.

Let's start with Declination.

If you can imagine the Celestial Equator in the sky where it crosses your Meridian, we have a pretty specific spot in the sky. This point is the starting point for Declination which is defined as "how far above or below the celestial equator is an object in the sky".

Starting at 0° and going upwards to +90° is the Northern Sky. Starting at 0° and going downwards to -90° is the Southern Sky.

In the "half-dome" diagram at left you can see that Declination increases upwards. It actually keeps on going over the observer's head and then back "down" towards the Northern horizon until it reaches Polaris! You can also see that from this location we can see a portion of the Southern Sky - not nearly as much as the Northern Sky, but at least some of it.

From here, we can see the entire Northern Sky (over the year) and, we can see down to a Declination of -(90° - your Latitude). For Calgary at 51° North, this means we can see any object with a Declination from +90° to about -39° (depending, again, on the Southern horizon visibility).

Side view of a Declination Arc Side view of a Declination Arc for an observer at 45° Latitude.

6.
Declination Lines Ok - Another thing about Declination:

It's a bit tricky to see, but if we make up a Declination grid, all the lines have the following characteristics:

- they all meet at the N and S Celestial Poles,
- they all cross the Celestial Equator at a right angle (just like N-S lines of Longitude do on Earth)
- Declination is always measured + and - from the Celestial Equator

The Diagram at left shows several lines for measuring Declination - useful for things that are not on the Meridian.

Note that southern objects (for instance at Declination of -20°) "set" before reaching the Western horizon. They also "rise" from a position that is more southerly than the Eastern horizon. Again, a clear southern view is necessary if you want to be able to see these objects.


7.
Lines of constant Declination Ok - a few more things about Declination before we move on:

If we "join" all the same values of Declination in the image above (e.g. all the +10° points etc.) we get "lines of constant Declination" as shown at left.

All these lines are actually parallel to each other and never meet.

This also shows that southern objects (like those at -30°) rise south of East, set south of West, and are visible for a much shorter time than more northerly objects.

[Optional reading: For really accurate measurements of positions, 10° lines or even 1° lines are not enough. Each degree of Declination is divided into 60 minutes of arc (abbreviated min or ' ) and each of those minutes is divided into 60 seconds of arc (abbreviated sec or " ). Therefore a really accurate Declination position might be specified as +30 deg 15 min 41 sec or +30° 15' 41". For even greater accuracy, the seconds value might be shown with a decimal fraction such as +30° 15' 41.03", and if you want to convert the entire thing into decimal degrees the formula is: Declination = degrees + (minutes / 60) + (seconds / 3600) which, for the example of +30° 15' 41.03" results in a value of +30.2613972 degrees.]

Side view of a Declination Arc Side view of Declination lines for an observer at 45° Latitude:
- they are all parallel
- the circles get smaller towards the Celestial Poles
- only the Celestial Equator touches the exact E-W horizon

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Right Ascension

8.
Right Ascension If Declination is the "up-down" coordinate, then what is the "left-right" coordinate?

The answer is Right Ascension. If you could take a flat star chart that has grid lines for locating things on it and hold it up to the sky and then bend it so that it fits into the bowl of the Celestial Sphere, the result would be like the diagram at left. The purple lines on the diagram represent left-right divisions, except that they are all curved. You have seen lines like this above where we drew several lines from which we could measure Declination.

Each of these curved lines is like a N-S longitude line on the Earth - they all meet at the poles and they all cross the Equator at a 90° angle. But how to label them? They are not nearly as fixed in the sky as Declination, since the Earth is constantly rotating bringing new grid lines up from the East, and loosing those low in the West. So a fixed degree system based on the Pole and the Equator just won't work. They need to be tied into the fact that Earth rotates every 24 hours and this is an amount of time.

So, that was it - they divided the sky map into 24 bands from left-to-right and labeled them as "hours" meaning that it took approximately 1 hour for each of them to move a distance equal to its width across the sky. The lines defining these bands therefore became the logical choice for a grid system, and it was based on things in the sky - not on the Earth's poles or equator.

So each object was catalogued as being at a certain point in Declination and would appear at a certain "hour angle". In other words, if you stood outside and looked at the sky for several hours you would see the stars seem to move across your Meridian from East to West at that rate.

Note that since everything is rotating constantly, the Right Ascension "value" on both the East and West horizons and your Meridian changes continuously - every minute of the night.It also changes every day of the year as Earth goes around the Sun - but that's the next topic.

So, where to start this numbering system - every point in the sky crosses your Meridian each day, and every spot on Earth has a slightly different exact local time (remember - this was before Standard Time Zones were invented). The choice could not be given to one preferred city on Earth - it had to be based on the stars. The choice was the "Vernal Equinox" - i.e. the point in the sky where the Sun was at the time of the March Equinox. From that specific point on the Celestial Equator, they simply numbered the "hours" 0, 1, 2, 3, and so on up to 22, 23, and 24 was made the same as the 0 line.

The trick was, they numbered them to the East (i.e. to the left) since that is the order in which the lines rise up from the Eastern Horizon - so the numbers get larger to the East (left).

So now we had a grid system we could draw on paper and from the starting points of 0° Declination and 0 hours of Right Ascension we could chart everything in the sky, and use this map anywhere on Earth.

Side view of Right Ascension Lines Side view of of Right Ascension Lines for an observer at 45° Latitude animation
Click for animation

Click on the image at left to open a new window with a 338 KB animation of the stars, constellations, and Right Ascension lines, rising in the East and setting in the West for the night of Jan 1, 2006 as seen from Calgary. (Close the new window when you are finished with it.)
- they are all the same size
- the separation gets less until they all meet at the Celestial Poles
- they cross the Celestial Equator at a right angle
- 0h is found in the constellation Pisces
- they are numbered from 0 to 23
- larger numbers rise up from the East

Due south of you, your Meridian defines your exact local time and since we now map stars by time, this is called your local "star time" or LMST - your Local Mean Sidereal Time. This is just the star's Right Ascension value from the map for that star.

[Optional reading: For really accurate measurements of positions, "hour" lines are not enough. Each of these represented an hour of time, and therefore, for greater accuracy they sub-divided these "hours" into 60 "minutes" and each minute into 60 "seconds" (of time). It is slightly confusing to use the same terms as the subdivisions of degrees, but remember, all these lines curve up to the poles where they meet, so the value is not an angle of separation since the separation keeps getting smaller and smaller on the sky till there is no angular separation at all at the poles, yet the sky still takes 24 hours to rotate, even at the poles.

Therefore a really accurate Right Ascension position might be specified as 3 hours 15 minutes 41 seconds or 3h 15m 41s. For even greater accuracy, the seconds value might be shown with a decimal fraction such as 3h 15m 41.03s, and if you want to convert the entire thing into decimal hours the formula is: RA = hours + (minutes / 60) + (seconds / 3600) which, for the example of 3h 15m 41.03s results in a value of 3.2613972 hours. Right Ascension is never negative or greater than 24 hours.]

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Sidereal Time

9.
The Diagram below (not to scale) attempts to show one day in Earth's orbit around the Sun.
The upper portion of the diagram shows that one day is approximately 1° along Earth's Orbital path.
The lower portion attempts to show the Earth's 24 hour rotation during that day - viewed from somewhere above the North Pole.

Earth's Orbit and Rotation relative to the distant stars.

Things to notice in the diagram above.
  • If the orbit was a perfect circle of 360° (instead of a slight ellipse), then 1 day (in a 365¼ day year) is 360° / 365.25 Days = 0.986° or slightly less than 1° per day - a very small angle (shown in the upper part of the diagram).
  • At the bottom of the Diagram we see a magnified portion, with the Earth on "Day 1" and the Sun directly above the purple dot at local Noon.
  • 24 hours later on "Day 2" we see the Sun directly above the purple dot at local Noon again.
  • But on "Day 2" we have been carried along in our orbit that 1° so the Earth had to rotate a little more than 360° to again point directly at the Sun.
  • On Day 3 it happens again - The Earth has to rotate a bit more than 360° per day to keep the Noon Sun in the right place in the daytime sky.
So, the Earth rotates more than 360° per day. However, we define our 24 hour "day" relative to the Sun, not relative to the Earth's actual rotation. If we didn't do this, then "Noon" would occur a little later each day until "Noon" was happening at night!

Now look at the white dot and the purple line from that spot on Earth to a distant Star. Each "day" we go a little past the point where we once had a view of that star on our Meridian. Or, conversely, each night our Meridian points to a different star.

In fact, if we time the Earth's rotation using our 24 hour "Sun" clock, we would see a star reappear on our Meridian 23 hours and 56 minutes later. This 4 minutes per day difference totals about 1461 minutes per year or slightly more than a full day. So, relative to the stars the Earth makes an additional rotation over the year. It is this slight additional rotation per day that causes the summer constellations to set is the West as the Winter constellations rise in the East - in other words it gives us a chance to see the whole sky, at night, over the course of a year.

We call the 23hr 56min period a Sidereal "Day" - the time it takes for the Earth to rotate relative to a star.

This has the effect of sliding our star chart to the right by 4 minutes of Right Ascension per day, in addition to the complete rotation of 24 hours of Right Ascension it makes. These two factors combine so the Right Ascension of everything up there changes not only every hour, but every day they slide a little further to the West.

Finally - putting all this Right Ascension stuff together:

If you want to see an object that is catalogued as "Right Ascension xx hours" then it will be on your local Meridian when your LMST is "xx hours". You can either go out on a night before then, and wait a few hours for it to be there, or wait for the appropriate day and go view it on the Meridian right away.

Since there are 24 hours of Right Ascension and 12 (roughly equal) months in the year, the time a constellation is on or near the Meridian changes about 2 hours each month (or roughly 1 hour every 2 weeks) as the Earth progresses in its orbit around the Sun.


[Optional reading 1:]
  • The radius of the Earth's orbit is 149,597,871 Km (92,955,807.46 Mi)
  • The Circumference of Earth's orbit (the path) is therefore 2 π R or approximately 940,000,000 Km (580,000,000 Mi) around
  • In one day the Earth travels only 1/365¼ of the way around its orbit or approximately 2,600,000 Km (1,600,000 Mi)
  • Since the Earth is 12,756 Km (7,926.21 Mi) in diameter, the Earth moves approximately 202 times its own size in one day!
  • So, the lower part of the diagram showing the Earth from day to day is definitely not to scale!
[Optional Reading 2:]
  • Due to the fact that the Earth's orbit is a slight ellipse, the Sidereal day is actually defined as an average over the year - called the Mean Sidereal Day which is 86,164.0909 seconds, or 23 hrs 56 min 4.0909 seconds.
  • The "year" is not exactly 365¼ days (sometimes called the Julian Year).
  • Even with our calendar rules for leap years and century leap years, it is not 365.2425 days (the average Gregorian Year)
  • With respect to the distant stars, the "year" is 365.2421896698 days or about 99.999915 % of the average Gregorian year.
  • Comparison with complicated equations involving the timings of the Vernal Equinox reveals that the Gregorian calendar accumulates an error of one day in about 2500 years. Although various adjustments to the leap-year system have been proposed, none has been instituted. In other words, our calendar should work for the next 2500 years.


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The Ecliptic

If the Earth orbited the Sun standing "straight up and down", then the Equator (both Earth's and the Celestial Equator) would be parallel to the Earth's orbital plane. The Sun would never deviate from the Celestial Equator, and all the other planets in their orbits would be found close to the Celestial Equator as well. Of course this would also mean we wouldn't have seasons since the Sun would rise at the same point due East, follow the Celestial Equator path, and set at the same point due West every day of the year.

But this is not the case. Planet Earth's North-South axis is tilted 23.4393° with respect to the plane of the Earth's orbit (called the Ecliptic Plane, so we are rotating at an angle with respect to the way we go around the Sun. Click the image below to open a new window with a 184 KB animation of the way the Earth rotates. (Close the new window when you are finished with it.)

animation


This tilt causes the changing seasons, because it sometimes tips the Northern Hemisphere towards the Sun (in the Summertime) and on the opposite side of our orbit, tips the Northern Hemisphere away from the Sun (in the Wintertime) - see the diagram below.

From the Earth, this is seen as the Sun getting higher in the sky during the Summer, finally reaching its highest point at what we call the "Summer Solstice" around June 21, and lower in the sky during the Winter, finally reaching its lowest point at what we call the "Winter Solstice" around December 21.

This apparent path of the Sun's motion on the celestial sphere as seen from Earth is called the Ecliptic. It results from us looking from the Earth to the Sun i.e. along a line joining the Sun to the Earth's orbit - not the Earth's Equator. The path of the Sun over a year is therefore another great circle in the sky, but it is tilted from the Celestial Equator the same amount as Earth's axis tilt: 23.4393°.

When the Earth's tilt causes the Northern Hemisphere to be tipped towards the Sun, the Sun's path (the Ecliptic) and the Sun can be found high is the daytime sky. When the Earth's tilt causes the Northern Hemisphere to be tipped away from the Sun, the Sun and the Sun's path (the Ecliptic) can be found low is the daytime sky.

Earth's Orbital Motion

As can be seen in the diagram above, the situation is reversed on the night side of the Earth. When the Sun's path is highest in the daytime sky (in Summer) the Ecliptic is lowest in the nighttime sky. And vice-versa - when the Sun's path is lowest in the daytime sky (in Winter) the Ecliptic is highest in the nighttime sky. This makes it easier to see the other planets and asteroids in the Wintertime since the Ecliptic plane (also the plane of the Solar system) reaches its highest point away from the (murky) horizon and all the planets (except Pluto) are never found far from this line.

These two great circles in the sky - the Celestial Equator and the Ecliptic - are tilted, but cross each other at two points (kind of like they were hinged there). These two points are called the "March Equinox" around March 21, and the "September Equinox" around September 21.

10.
The Ecliptic


When is the Ecliptic highest or lowest in the sky?

The Celestial Equator always appears at the same position in your sky. However, since the Ecliptic is "tilted" with respect to that line, it seems to pivot about its centre as the Earth rotates and also as the Earth revolves around the Sun. Since the Earth rotates once a day, the Ecliptic seems to go through this pivoting cycle each day. Therefore, there is a time each day when the Ecliptic is at its highest, lowest, and intermediate points. Since the Ecliptic passes through the constellations of the Zodiac, those constellations appear at different heights along with the Ecliptic. Since the planets orbit close to the Ecliptic they also appear at different heights along with the Ecliptic.

Where the Ecliptic arcs through the sky depends on:
  • your exact longitude
  • your time Zone
  • the time-of-day
  • the day of the year
  • whether you observe Daylight Saving Time (and when it starts and ends)
  • where we are in the 4 year leap-year cycle
The tables below show several orientations of the Ecliptic against the Calgary sky, and the approximate dates in 2006 when you would be able to experience that orientation.

The Ecliptic at its highest position.
The Ecliptic at its highest position occurs each day at different times, e.g.:
00h MST ~ Dec 31
 
06h MST ~ Sep 30
06h MDT ~ Oct 16
12h MST ~ July 1
12h MDT ~ July 16
18h MST ~ Mar 31
18h MDT ~ Apr 16
When highest, it is easiest to see the Zodiac constellations and outer planets at night, and, the angle with the Eastern and Western horizons is greatest, making it the best time to see objects just after sunset or just before sunrise (e.g. Mercury).


The Ecliptic and the Celestial Equator.
The Ecliptic rises across the Celestial Equator due south twice each day at different times, e.g.:
00h MST ~ Mar 30
00h MDT ~ Apr 16
06h MST ~ Dec 30
 
12h MST ~ Sep 30
12h MDT ~ Oct 15
18h MST ~ June 30
18h MDT ~ July 16
The Sun's path defines the Ecliptic, and the Sun's Declination is only zero at the March and September equinoxes when the Ecliptic crosses the Celestial Equator.


The Ecliptic at its lowest position.
The Ecliptic at its lowest position occurs each day at different times, e.g.:
00h MST ~ July 1
00h MDT ~ July 16
06h MST ~ Apr 1
06h MDT ~ Apr 16
12h MST ~ Dec 30
 
18h MST ~ Sep 30
18h MDT ~ Oct 15
When lowest, it is hardest to see the Zodiac constellations and outer planets at night, and, the angle with the Eastern and Western horizons is shallowest, making it the worst time to see objects just after sunset or just before sunrise (e.g. Mercury).



The Ecliptic and the Celestial Equator.
The Ecliptic "sets" across the Celestial Equator due south twice each day at different times, e.g.:
00h MST ~ Sep 30
00h MDT ~ Oct 15
06h MST ~ July 1
06h MDT ~ July 15
12h MST ~ Mar 31
12h MDT ~ Apr 16
18h MST ~ Dec 30
 
The Sun's path defines the Ecliptic, and the Sun's Declination is only zero at the March and September equinoxes when the Ecliptic crosses the Celestial Equator.


animation
Click for animation

Click on the image at left to open a new window with a 219 KB animation of the Ecliptic position among the constellations over the course of a year (at Midnight Standard Time on the 1st and 15th of each month) as seen from Calgary. (Close the new window when you are finished with it.)


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Putting It All Together


animation
>Click for animation

Click on the image at left to open a new window with a 338 KB animation of the stars, constellations, Right Ascension, Declination and the Ecliptic, rising in the East and setting in the West for the night of Jan 1, 2006 as seen from Calgary. (Close the new window when you are finished with it.)

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Polar View

OK - we've covered Declination and Right Ascension looking South, but what about looking North?

First, you have to turn around to look north, so now East is on your right and West is on your left. This means objects rise from your right side and set on your left side (if they "set" at all).

Some high-Declination constellations are "circumpolar" meaning they circle the pole star and never "set" so they are visible every night of the year. Other (lower) constellations are visible only for a range of months, depending on your latitude and its average Declination. In addition, these constellations rise and set daily like the Sun and the planets do, so, the time of night that you are out stargazing also matters.

Click on this link to open another page from this RASC site which contains information on observing the constellations, or, consult a planisphere, one of the many PC or Mac based planetarium software packages, or one of the many other internet sites to see what constellations are visible on any given night.

animation
>Click for animation

Click on the image at left to open a new window with a 405 KB animation of the stars, constellations, Right Ascension, and Declination, rotating around the North Celestial Pole for the night of Jan 1, 2006 as seen from Calgary. (Close the new window when you are finished with it.)

Earlier I said I'd talk about "Lower Culmination" later - and now's the time.

Early in this article we noted that an object reaches "Culmination" or "Upper Culmination" when it rises up to its highest point in your sky and crosses your Meridian. But if you look at the animation above, you can see that many circumpolar objects near the North Celestial Pole cross your Meridian twice each day - once when "circling" from East to West, and again 12 hours later as it passes under Polaris circling back from West to East. So we had to clarify the definition of "Culmination" depending on where you are looking. When far-northern objects cross your Meridian "below" Polaris we call it the object's "Lower Culmination".

In either direction, "Upper Culmination" is the time at which the object is highest in your sky and at its best for viewing or photographing.

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Eastern View

OK, we've covered looking South, and looking North. But what about looking East?

animation
>Click for animation

Click on the image at left to open a new window with a 303 KB animation of the Eastern view for the night of Jan 1, 2006 as seen from Calgary. (Close the new window when you are finished with it.)

Notice that the Celestial Equator looks like a straight line rising diagonally up and right from the East point on the horizon. Objects to the left of it (those with positive Declinations) appear to diverge and curve up and to the left of the Celestial Equator, heading towards their path over Polaris. Objects to the right of it (those with negative Declinations) appear to diverge and curve below and to the right of the Celestial Equator, arcing across the sky to the south.

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Western View

OK, now we've covered looking South, North and East. But what about looking West?

animation
>Click for animation

Click on the image at left to open a new window with a 327 KB animation of the Western view for the night of Jan 1, 2006 as seen from Calgary. (Close the new window when you are finished with it.)

Now the Celestial Equator looks like a straight line dropping diagonally down and right towards the West point on the horizon. Objects above it (those with positive Declinations) appear to start converging with it curving down and to the right of the Celestial Equator, after their path over Polaris. Objects below it (those with negative Declinations) set earlier than the Celestial Equator, arcing across the sky to the south west.

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How to use it

1. The type of telescope mounting you have determines what you have to do in order to "track" an object as it rotates across the sky.
2. The type of mount also determines how you re-point the scope to various objects.

1. Following Objects across the Sky


An Equatorial Mount (or "German Equatorial Mount") is set up so that the entire mechanism (including the telescope and counterweights) rotate around the Celestial Pole just as the sky does. The mount only has to move the telescope in Right Ascension as time goes by to "track" objects rising in the East and setting in the west. This means only one motor is required (the RA motor), although a Declination motor is often supplied as well just to make pointing the telescope to new objects easier. If you point the telescope to another object (different RA and Declination) the process continues again.

In order to ensure the rotation axis of the mount is precisely aligned with the rotation axis of the Earth, a small "polar-alignment telescope" is often built right in to the axis of rotation and the telescope setup process involves carefully adjusting the tripod's "North leg" and the mounting so that it accurately points to the Celestial Pole (near Polaris). If the mount does not have a separate polar-alignment scope, then the main telescope or its "finder scope" must be used to accurately align the axis of rotation to the Celestial Pole.

This type of mount is ideal for long-duration astrophotography, although the weight and setup time are larger than other types of mounts.

Depending on the design of the mount some "equatorials" have difficulty following an object as it crosses your Meridian and the entire telescope must be "flipped over" to avoid the telescope tube, motor or some other component hitting the mounting or the tripod. See the bottom diagrams on the left. Click the following links to open a new page with a photo of an equatorial scope set up for Observing East of the Meridian, or Observing West of the Meridian.
An (optional) Equatorial Wedge for a fork-mounted telescope performs the same function as an Equatorial Mount - keeping the axis of rotation in line with the Earth's axis. Only the RA motor is required to follow an object, even if the fork mount comes with both. In fact, if you work with a fork-mounted telescope you must either "tell" the tracking system whether you have installed a wedge or not, or turn off the Declination motor while using it. If you don't do this and it starts operating as if there was "no wedge" then it will drive both motors when only one is required and you will not be able to follow objects in the sky.

This design does not allow for a separate "polar telescope" so the main telescope or its "finder scope" must be used to accurately align the axis of rotation to the Celestial Pole.

This type of configuration is also very good for long-duration astrophotography provided the polar alignment is done carefully.
A computerized Fork Mount telescope (with either one or two fork arms) without an Equatorial Wedge has to continually adjust for the changing position of the object of interest by automatically moving the telescope East-to-West as well as South-to-North or North-to-South to follow objects that are either rising in the east or setting in the west. It must therefore have two accurate motor drives and a computer control system to run both motors.

Polar alignment is not necessary (or possible) so another alignment procedure must be used to ensure the pointing accuracy of the two motors is set properly.

This configuration is good for short-duration astrophotography. It cannot be used for long-duration astrophotography because the camera (or CCD detector) is always parallel to the horizon, not rotating with the curved line the objects follow. This causes any long duration image to suffer from "field rotation". However, there are some software packages that can account for this, rotating a set of short duration images appropriately to remove the unwanted effects.
If you have a Dobsonian telescope, or a simple Tripod Mount for a refractor or reflector, (commonly referred to as Alt-Azimuth mounts) then you will have to manually keep the telescope on the object of interest. This involves manually moving the telescope "up-and-west" as the object rises, and "down-and-west" as the object sets. This type of mounting is not recommended for astrophotography because it is very difficult to continuously aim the telescope precisely. However, it is the least expensive mounting and is still very good for visual observing and making drawings or sketches of celestial objects.


2. Re-pointing to different objects

  • The view through a telescope is often inverted - sometimes just Left-Right, but also may be North-South as well. Telescopes without flat mirrors in the path of the optics (refractors, and Schmidt Cassegrains when used "straight through") invert both horizontally and vertically. Newtonians, Dobsonians and other configurations with one flat mirror in the optical path use the mirror to "correct" one direction but not two. A special prism corector may be used with telescopes to correct for both directions making them useful for terrestrial observations as well.
  • The reason we don't make all telescopes with upright and correct views (like binoculars) is that there is no "up" or "down" in outer space, and for every surface (mirror) or glass (lens, prism) the light goes through it looses a bit of intensity and may be distorted a tiny bit. To achieve the clearest views of the sky, telescopes try to use as few optical elements as possible. Besides, if we take pictures trough a telescope, it is an easy thing to flip them horizontally or vertically as we process the images before printing.
  • However, these "reversed" views can make it hard to find objects by looking through the eyepiece and moving the telescope. You will find that movement in one direction cause the image to shift in another direction.
  • Finding one object (r.g. a dim galaxy) by starting at another (e.g. a bright star)
  • point at star "A" of known Right Ascension (Ra) and Declination (Decl)
  • for object "B" - calculate the difference in Right Ascension and Declination from the first object
  • if DeclB is higher (more positive) than DeclA, move the scope "upwards" in Declination the required number of degrees
  • if DeclB is lower than DeclA, point the scope "downwards" in Declination the required number of degrees
  • if RaB is larger than RaA, point the scope "eastwards" in Right Ascension the required number of degrees
  • if RaB is lower than RaA, point the scope "westwards" in Right Ascension the required number of degrees

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Precession

Now that you think you have Right Ascension and Declination pretty well figured out, it's time to learn that it's even more complicated than the long description above.

Every Right Ascension and Declination coordinate moves over a long period of time, due to the fact that the Earth's North-South rotation axis "wobbles" like the slow rotational tilting of a spinning top. This is known as Precession and affects the direction in the sky to which the North Pole points, and where the Celestial Equator is found. Since the entire Right Ascension and Declination coordinate system was based on those two values, this is a pretty important effect. (Although it is often called the "Precession of the Equinoxes" you should realize that it would affect not just the positions of the September and March Equinoxes, but everything based on Right Ascension and Declination.)

Precession is caused by the gravitational attraction of the Sun (and the Moon) tugging on the Earth's equatorial bulge - trying to "level" it from its 23.4393° tilt, but never winning. Due to the laws of motion (and something called "angular momentum") the axis keeps its tilt, but the tugging force causes the axis to wobble around in a circle rather than "straightening" up.

The Greek astronomer Hipparchus of Rhodes (190-120 B.C.) discovered that, due to the "wobble" of the Earth's axis as it spins like a top, the North-South axis line (the North Celestial Pole) pivots around a point in space known as the North Ecliptic Pole which is "straight up" from the Ecliptic - the plane of the Earth's orbit around the Sun.

One revolution around this point takes a period of approximately 25,770 years (Beatty et al. 1990) commonly quoted as the "26,000 year precession of the equinoxes". The moving N. Celestial Pole also determines which star is nearest the northern axis line of the Earth on the Celestial Sphere and which one is therefore the "North Star".

Thuban (in southern Draco) was the "pole star" around 3000 BC. The next naked-eye star that served as the Earth's pole star was Kochab in the bowl of the Little Dipper from about 1900 BC to 1100 BC. Due to precession, the current holder of the title "pole star" is Polaris which, at present, is slightly under 1° away from the pole of rotation. Polaris is due to become an even more accurate pole star in the near future - the distance between Polaris and the pole will reach a minimum of just under 1/2° in the year 2100. After that, Alderamin in Cepheus will be the Pole Star around 7500 AD, Deneb in Cygnus will be the Pole Star around 10,000 AD and Vega will become the North Star in about AD 14,000 (see the first diagram below).

Due to this "wobble" all the coordinates of the "fixed stars" slowly change. (Over thousands of years, the relative positions of all the stars also change due to their own motion through the galaxy, but this is not part of Precession.)

Since the constellations "contain" the stars within their borders, the constellation borders must also change with Precession.

Finally, since we base the positions of all moving Solar System objects on our coordinates - these must also take precession into account when they are calculated.

Thankfully, this is a fairly small angle change each year, but it builds up over time so that every 50 years we need to re-publish all the Right Ascension and Declination coordinates. This is called the epoch (i.e. date) of the coordinate list. You will find many old textbooks using epoch 1950 and all newer texts using epoch 2000. By the time your grandchildren get interested in Astronomy, they will probably be deciding whether to use epoch 2000 or 2050.

Oh, and one last thing. Since Precession affects the direction of the tilt of Earth's axis, it will eventually reverse the angle so that when we reach the point in our orbit where we used to have Winter (Earth's axis pointing the Northern Hemisphere away from the Sun) we will then have Summer (Earth's axis pointing the Northern Hemisphere towards the Sun). So, if you can wait about 12,000 years, all those beautiful Winter constellations (like Orion) will finally be visible on hot summer nights (see the second diagram below).

The Precession of the N. Celestial Pole describes
a huge counter-clockwise circle in the northern sky as seen
from the Earth. The angular diameter of this circle is twice
the tilt of Earth's axis - approximately 47° across.

Precession of the N. Celestial Pole

The Earth's Orbital Motion and Precession

Earth's Orbital Motion and Precession

More on Precession:

http://www.jgiesen.de/astro/precession/index.html
http://en.wikipedia.org/wiki/Precession
http://www.seds.org/~spider/spider/ScholarX/coord_ch.html


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