<<

The The Celestial Sphere

We will learn:

● Great Circles; ● Coordinate Systems; ● and , etc; ● [Seasons and Sun Motions]; ● The Celestial Sphere “We will be able to calculate when a given star will appear in my sky.” The Celestial Sphere

Woodcut image displayed in Flammarion's `L'Atmosphere: Meteorologie Populaire (Paris, 1888)' The Celestial Sphere: Great Circle

A great circle on a sphere is any circle that shares the same center point as the sphere itself. Any two points on the surface of a sphere, if not exactly opposite one another, define a unique great circle going through them. A line drawn along a great circle is actually the shortest distance between the two points (see next slides). A small circle is any circle drawn on the sphere that does not share the same center as the sphere. The Celestial Sphere: Great Circle

• A great circle divides the surface of a Pole of Great Circle sphere in two equal parts.

• A great circle is the largest circle that fits on the sphere.

• If you keep going straight across a sphere then you go along a great circle.

• A great circle has the same center C as the sphere that it lies on. Primary Great Circle Great Circle • The shortest route between two points, measured across the sphere, is part of a great circle. The Celestial Sphere: Great Circle

How many great circles do you need to define your coordinate? Pole of Great Circle

Every great circle has two poles. A single great circle doesn’t define a coordinate system uniquely (cf: rotation).  We need a secondary great circle to define a coordinate system. Primary Great The secondary great circle is a Circle Great Circle great circle that goes through the poles of a primary great circle The Celestial Sphere: Great Circle The diagram in the left tries to Why is the shortest path? show the two locations as small blue spheres, the red lines being their position vectors from the centre of the sphere. (Their center lines of latitudes and are represented by white circles).

From this you can see that the shortest distance between the two points is given by the length of an arc of a circle concentric with the sphere and with the same radius as the sphere. The Celestial Sphere: Great Circle

Great Circle: the shortest path

Loxodrome: maintains the constant compass direction, cuts all meridians at the same angle The Celestial Sphere: Coordinate Systems

Coordinate Principal great ``Prime "  Coordinates system circle Secondary great circle

horizon or observer's altitude, northsouth meridian observer's horizon

Equatorial Projection of Head of Aries  vernal (α), or Celestial 's equator (δ),

plane of Earth's head of Aries  vernal Ecliptic (λ), ecliptic revolution equinox Ecliptic latitude (β)

plane of the Galactic longitude (l ), Galactic Galactic center Galactic latitude (b ) The Celestial Sphere: Coordinate Systems

Transformation between the Spherical Coordinate Systems with Eulerian matrix operators.

• α : rotation about z axis • β : rotation about y axis • γ : rotation about x axis

There are known numerical transformations between different coordinate systems (which is beyond the scope of this class.) The Celestial Sphere: Coordinate Systems Horizon Nadir: opposite zenith North point: on the horizon : a great circle that contains the zenith and is perpendicular to the horizon  there could be many vertical circles on your horizon Meridian: a vertical circle that contains the zenith, nadir, the north celestial pole, and the due north and south points on the horizon. Your meridian, which is a secondary great circle, also divides your sky in half. There is only one meridian on your horizon. The Celestial Sphere: Coordinate Systems

Altitude: how far above the horizon to look for an object, from zero degrees at the horizon to 90 degrees at the zenith  Elevation

Azimuth: the direction towards the horizon one must face to look up from the horizon to the object. In this system we start from 0 degrees for the north meridian, then 90 degrees for due east, etc.  Direction The Celestial Sphere: North and South Poles

The is an extension of the Earth’s equator to the surface of the celestial sphere

The north/south celestial pole is an extension of the Earth’s north/south pole. The Celestial Sphere: Earth’s Latitude & Longitude Two perpendicular great circles: the equator & Greenwich longitude circle

(NRAO is located at Charlottesville.)

What are the longitude and latitude of Toronto? The Celestial Sphere: Horizon, Meridian, & Celestial equator

A horizon (plane) is a plane tangent to the Earth’s surface at the observer’s feet. The Celestial Sphere: Horizon, Meridian, & Celestial equator

The North Celestial Pole (near Polaris) is at altitude of your location’s latitute. The Equatorial Coordinate: (R.A. & decl.) RA: extension of the latitude to the celestial sphere DEC: extension of the longitude to the celestial sphere (vernal equinox) RA & DEC: fixed on the celestial sphere; (Alt., Az.) varies (Latitude, Longitude) vs. (R.A., decl.)

(Latitude, Longitude) (R.A., decl.)

 Earth equator for LAT;  Celestial equator for decl.;  A vertical circle to the  A vertical circle to the equator containing a equator containing a reference location for LON; reference location for decl.;  The reference location is  The reference location is Greenwich observatory, a vernal equinox, a fixed fixed location on earth. location on the celestial sphere. The Equatorial Coordinate: (R.A. & decl.) (R.A., decl.) and Vernal Equinox are where the Sun meets the celestial equator (Vernal equinox for spring; Autumn equinox for autumn)

Motion of the Sun through the year on Vernal Equinox: the ecliptic plane. ascending node of the ecliptic on the equator (R.A., decl.) and Vernal Equinox

What are R.A. and decl. of the Sun at vernal equinox, summer solstice, fall equinox, and winter solstice? How high (in elevation) can you see a star?

SALT: the highest elevation at X (when star X is on meridian) which a star can appear in the northern hemisphere.

North South How high (in elevation) can you see a star?

SALT: the highest elevation at X (when star X is on meridian) which a star can appear in the northern hemisphere.

North South Star X is SALT above the southern horizon.

SALT = DEC + (90o – LAT) = (DEC – LAT) + 90˚

Objects with DEC = LAT have altitudes of 90o crossing the zenith. SALT determines how high in the sky an object can be. The maximum DEC the Moon can achieve is +28.5o. What’s the maximum altitude we can ever see the Moon at Toronto ? The Celestial Sphere at the Poles The Celestial Sphere at the Equator The Celestial Sphere: Locus of the constant declination

Locus of the “constant decl.” gives a path of a star (from rise to set) which is “parallel to the equator.”

Star on the Celestial Equator: from the due east to the due west. The Celestial Sphere at the Latitude LAT

At the northern hemisphere

Star at less than LAT from the NCP: “Never sets.” Star at less than LAT from the SCP: “Never rises.” The Celestial Sphere at the Latitude LAT

Observer’s horizon

(At the northern hemisphere) The Celestial Sphere at the Latitude LAT

● Objects on the Celestial Equator: Due East  Dew West 12 above horizon

● Objects of the North Circumpolar Region: North of the Due East/West more than 12 hours above horizon

● Objects of the South ● North Circumpolar Region: Circumpolar Region: (90o – LAT) < DEC < 90o South of the Due ● South Circumpolar Region: East/West less than 12 – 90o < DEC < – (90o – LAT) hours above horizon The Celestial Sphere: , Transit and Local Sidereal Time When an object crosses my meridian, it transits. Hour Angle (HA) is the amount of time (= angle) before or after transit. It increases between –12h and +12h (= 0h – 24h). HA is object specific. Examples: A star with HA = +2h crossed the meridian two hours ago. A star with HA = 1h will be on the meridian in one hour. The Celestial Sphere: Hour Angle, Transit and Local Sidereal Time Local Sidereal time (LST) is the RA of an object on the meridian (= transit object). (So it changes.)  LST is the HA of the vernal equinox.

LST = 0 if the vernal equinox is in transit. (Note that RA is measured from vernal equinox.)

Local Sidereal Time = Hour Angle + Right Ascension The Celestial Sphere: Hour Angle, Transit and Local Sidereal Time

If the LST = 20h, an object of RA = 20h is in transit. At this time, the HA of an object of RA = 5h is 15h. The object transited 15 hours ago.

If the LST = 2h, the HA of an object of RA = 5h is −3h. So this object will transit in 3 hours. The vs. Sidereal Time

Earth has both rotation and revolution. Sidereal Time Toward distant stars Sidereal time is the hour angle of the vernal equinox, the ascending node of the ecliptic on the celestial equator. The daily motion of this point provides a measure of the rotation of the Earth with respect to the stars, rather than the Sun.

Earth has both rotation and revolution, so the solar day is really “longer” than the true rotation period of the Earth Time based on the Earth’s rotation with respect to the stars (= sidereal time) is a better measurement. Sidereal Time

One solar day is approximately 4 minute longer than one sidereal day. Why?

Earth moves around the Sun in 365.25 days In one day, the Earth rotates 360/365.25days ≈ 0.986/day. Longitude, Universal Time, Greenwich Time

● Longitude = (Greenwich Mean Time – Local Mean Time)  15 ● Universal Time (UT) = Greenwich Mean Time (GMT) ● Sidereal Time = Hour Angle of the Vernal Equinox. (Here the Vernal Equinox is used as a reference point of the stars. The daily motion of this gives a measure of the Earth rotation with respect to the stars.) ● Local Sidereal Time (LST) = Greenwich Sidereal Time (GST) + Longitude Offset. (LST is RA of an transit object for a given time: LST = RA + HA of an object. GST is available in Astronomical Almanac.) Exercises

At midnight on 1998 Feb. 4, LST at St.Andrews (longitude 2°48‘ W ) was 8h45m. What was the local HA of Betelgeuse (R.A. = 5h55m) at midnight? HA = LST – RA  2h50m. At what time was Betelgeuse on the meridian at St.Andrews? Betelgeuse would be on the meridian 2h50m before midnight at 21h10m. At what time was Betelgeuse on the meridian at Greenwich? St.Andrews is 2°48' west of Greenwich, so it is 0h11m behind Greenwich (divide by 15). So Betelgeuse was on the Greenwich meridian 11 minutes before it reached that of St.Andrews’ (i.e. at 20h59m). Local Sidereal Time Calculation (using Almanac)

1. Convert (local standard) time to UT. 2. Convert the solar interval since 0h UT to a sidereal interval. 3. Calculate the GST at the time of interest. 4. Correct for the observer’s longitude and calculate LST. Local Sidereal Time Calculation (using Almanac)

1. Convert (local standard) time to UT. 2. Convert the solar interval since 0h UT to a sidereal interval. 3. Calculate the GST at the time of interest. 4. Correct for the observer’s longitude and calculate LST. The Ecliptic Motion and the location of the Sun The Ecliptic Motion and the location of the Sun

What are R.A. and decl. of the Sun at vernal equinox, summer solstice, fall equinox, and winter solstice?

Based on the information, can you estimate roughly where the Sun is today? What are the R.A. and decl. of the Sun today?

From this, can you estimate the rough coordinates of stars that you can see tonight?