Julian Date: 2458994.16
2019-2020: CLIV
THE DAILY ASTRONOMER
Tuesday, May 26, 2020
Remote Planetarium 41: Stellar Motions
Stars move.
However, when admiring the stars on any clear night, one perceives them as stagnant. Well, honestly, if one watches the stars at the same time of year once every decade, they still seem boringly inert. Look at the constellation Orion. Were one to venture outside in early February to find the great hunter, one would find him high in the south around 8:00 p.m. For an entire human lifetime Orion would be thus situated; due south around 8:00 p.m. in early February. The Orion of one's youth is identical to the Orion's of one's old age. Moreover, the Orion of your great great grandfather's youth seems the same as that of your great great grandchild's last days. From these observations one can well understand the ancient belief that the stars were immutable, immortal and immobile. Astronomers have only recently - by astronomical time frames- discovered that they are nothing of the sort. They move through the galaxy at speeds exceeding a hundred miles per second. They're also constantly changing and, like everything else in the cosmos, their time within it is finite. (Topics for another day.)
Our focus today is stellar motions. We will divide these motions into two categories: proper and improper. Proper motions are intrinsic motions, whereas improper motions are merely those that we perceive. We also refer to proper motion as "space motion." We identify three main types of improper motion, diurnal, annual and precessional.
- IMPROPER MOTIONS: diurnal (daily), annual and precessional
- PROPER MOTION: space motion
DIURNAL MOTION
The simple westward motion of stars caused by Earth's rotation. Our planet rotates once every 24 hours or every 1440 minutes. Since one rotation covers 360 degrees, a star will shift by one degree every four minutes or about fifteen degrees per hour.
The image above shows a time lapse photograph of the night sky. We can see direct evidence of Earth's rotational motion. Each star follows a circular pathway, the size of which depends on its angular distance from the celestial pole.
If Earth could somehow occupy the location in its orbit (impossible), the stellar motions would be merely diurnal. We would see the same stars at the same time of night each night. However, not only is Earth rotating, it is also revolving around the Sun. As a consequence, stars also exhibit
ANNUAL MOTION
During each rotation, Earth moves approximately one degree ahead in its orbit. As a consequence of this shifting, stars will rise four minutes earlier each day, unless, of course, they're circumpolar. We can use this four minute daily shift to help us follow stars throughout the year. Namely, we can employ the "Two Hour Rule." At the article's beginning we mentioned Orion being due south at 8 p.m. in early February. Let's be a bit more specific. Orion will be due south at 8 p.m. on February 2nd. Each February 2nd for the rest of our lives we can expect to see Orion the Hunter due south at 8 p.m. Now, when will Orion be due south on March 2nd? Well, we know that stars rise four minutes earlier each day. So, in one week, a star's rise time will decrease by 28 minutes or nearly half an hour. In two weeks, the rise time is reduced by one hour. We can then see that a star will rise two hours earlier each month.
If Orion is due south at 8 p.m. on February 2nd, it will be due south at 6 p.m. on March 2nd, 4 p.m. on April 2nd, noon time on May 2nd, and so forth. However, Orion will be due south at 10:00 p.m. on January 2nd, midnight on December 2nd and 2:00 a.m. on November 2nd. One can also determine the time that Orion reaches the due south position (called upper culmination) at any other time. For instance, on February 9th, Orion will be due south at 7:30 p.m. on February 16th, 7:00 p.m.
One may use this rule to track any star or constellation through the year. Just remember, however, that the amount of time a star spends above the horizon depends on its declination, or angular distance north or south of the celestial equator. The higher north the star, the greater its amount of time above the horizon.
PRECESSION:
Have you ever seen a top spin? If you have, you might have noticed that the axis "precesses." As the top rotates on its axis, the axis describes a wide circle so that it is constantly pointing in different directions. Our planet's axis also undergoes precessional shifting due primarily to the gravitational pulls of the Sun and moon.
One of Earth's precessional cycles lasts about 26,000 years. During this time period, the north celestial pole (NCP) will be aligned toward a variety of different stars. Currently, the NCP is oriented toward Polaris, hence the name "North Star." Precessional wobbling will continue to move the NCP toward Polaris until it reaches its minimum angular separation distance of 27' in the year 2102. The graphic below shows the NCP's path over the next 26,000 year period.
Around the year 4000, Errai, a star in Cepheus will become the new "north star." In about 13,000 years, the bright star Vega will have that distinction. Although, as we can see from the graphic, Vega will not be nearly as close to the NCP as Polaris is now.
Not only will the precessional cycle alter the NCP's position, it will also affect the zodiac. Recall that the zodiac refers to the thirteen constellations through which the Sun appears to travel each year. While these constellations will always remain part of the zodiac -until proper stellar motions disfigure the constellations beyond all recognition- their positions relative to the seasonal points will vary over time. The actual shift equals one degree every 73 years. Presently, the Sun appears to occupy the constellation Pisces on the vernal equinox, the first day of spring. The Sun's vernal equinox point had been in the constellation Aries the Ram. In 68 BCE, this point shifted from the Aries into the Pisces region. For this reason, the vernal equinox is also called "The First Point of Aries." The Vernal Equinox point will move into Aquarius in AD 2597!
Another example: the summer solstice point was in Gemini the Twins until 1989, when it then shifted into the Taurus the Bull region. Throughout the 26,000 precessional cycle, the four seasonal points will eventually occupy every point of the zodiac.
The diurnal, annual and precessional stellar motions are all a consequence of Earth's motion. Finally, we will look at proper motions and the space motions of the stars.
PROPER MOTION
Stars move through space in three dimensions; four, if you count time because you believe in the hyperspatial space-time continuum. Consequently, we can divide stellar motions into two components: radial velocity and transverse velocity.
Radial velocity refers to motion either toward or away from an observer. Think of being a batter in a baseball game. When the pitcher throws the ball, it exhibits a high negative radial velocity as it is approaching you. If you hit the ball, its radial velocity will be highly positive. The transverse or tangential velocity will be very low because the ball won't be moving much to either the left or the right when it is approaching you and when you hit it away. Now, further suppose that while you're at the plate, a runner is on first base. When you hit the ball, the man on first will be running toward second. The runner will exhibit a high transverse velocity because he will be moving toward your left. However, the runner's radial velocity will be low because he'll be moving away from you at a very small angle.
The actual space motion can be calculated by combining the radial and transverse velocity components. The proper motion is largely a result of the transverse velocity.
The Sun is moving through the galaxy at a speed of 200 kilometers per hour through the galaxy. Although the stars within our region of the galaxy are moving at comparable speeds, their directions differ so that some stars are approaching us, others are receding and others are traveling along paths nearly parallel with the Sun's trajectory. Moreover, the transverse velocities of the closest stars are greater than those of the more distant stars. For this reason, the 19th century astronomers chose to measure the parallax of the stars with the highest proper motions as those were correctly judged to have been the nearest ones. Astronomers measure proper motions in terms of right ascension and declination. Right ascension measures a celestial object's apparent distance from the vernal equinox while declination measures the object's distance north or south of the celestial equator.
The stars comprising the constellations will eventually disperse as a consequence of this proper motion However, these motions are on the order of milli arc-seconds per year even for the fastest moving stars such as Barnard's Star or Groombridge 1830. Constellation disintegration requires tens to hundreds of thousands of years. The image below shows how the Big Dipper (an asterism within Ursa Major) appeared 100,000 years ago, how it looks today and how it will appear in 100,000 years from now. The five central stars comprising this asterism are actually part of the Ursa Major Moving Cluster and are thus moving together through space. The two stars at either end are not physically associated with them and so will be moving away from them thousands of years in the future.
The upshot of this entire lesson is that nothing remains still. Earth rotates, revolves and precesses. The Sun and the billions of other stars within the galaxy move quickly through the galaxy. Even though we might see Orion due south in early February each year of our lives, the hunter's position relative to the seasons will change and eventually his component stars will tear him apart: far, far in the future.
Tomorrow, an investigation into stellar properties.
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A QUESTION ABOUT PARSECS:
Subscriber JV asked the following question regarding information contained within "The Closest Stars" class. (RP 39)
"Why do astronomers use the dimension parsec if they have the seemingly perfectly good light year? And why 3.26 light years per parsec? Seems an odd number."
Excellent question! I apologize for not having included this information in the class, itself. The term "parsec" is a contraction of the term "parallax second." In this regard, we are referring to the geometric measurement of arc-second. A quick review:
A circle consists of 360 degrees. One can divide that degree into 60 arc minutes. One can divide that arc minute into 60 arc-seconds. The same divisions apply to angular measurements within the sky, as well. The Sun and moon each subtend about half a degree or approximately thirty arc-minutes.(This value is not constant as the separation distances between the Sun and Earth and Earth and the moon are constantly changing.*)
An arc-second, however, is quite small. If someone 4 kilometers away from you holds up a dime, it will subtend an angle of one arc-second in your line of sight. Imagine you had a disc equal in diameter to one astronomical unit, about 93,000,000 miles. That disc would subtend an arc-second at a distance of 3.26 light years, what we call a parsec.
By designating the "parsec" we can simplify the mathematics of the stellar distance calculation. The SD distance above equals the distance separating the Sun from the star. We know the tangent of the angle equals ES (the Earth Sun distance) divided by the distance SD. We can rearrange this relation so that SD equals the Earth-Sun (ES) distance divided by the tangent of the angle. Fortunately, the tangent of very small angles approximately equals the values of those angles. This all reduces to:
DISTANCE = 1/p" where p" is the parallax angle in arc-seconds. The distance in this relation is expressed in parsecs.
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*The Sun's minimum angular diameter is 31.6' and its maximum is 32.7'. The moon's minimum angular diameter is 29.4' and its maximum is 33.5.'
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