+ All Categories
Home > Documents > 2. The Celestial Sphere Goals :

2. The Celestial Sphere Goals :

Date post: 01-Feb-2016
Category:
Upload: nyoko
View: 45 times
Download: 0 times
Share this document with a friend
Description:
2. The Celestial Sphere Goals : 1. Gain familiarity with the basic co-ordinate systems used in astronomy. 2. Tackle simple problems in practical astronomy involving timekeeping and star positions. 3. Examine the timekeeping systems in current use. Astronomical Co-ordinate Systems: - PowerPoint PPT Presentation
Popular Tags:
50
2. The Celestial Sphere 2. The Celestial Sphere Goals Goals: 1. Gain familiarity with the basic co-ordinate systems used in astronomy. 2. Tackle simple problems in practical astronomy involving timekeeping and star positions. 3. Examine the timekeeping systems in current use.
Transcript
Page 1: 2. The Celestial Sphere Goals :

2. The Celestial Sphere2. The Celestial Sphere

GoalsGoals:

1. Gain familiarity with the basic co-ordinate systems used in astronomy.

2. Tackle simple problems in practical astronomy involving timekeeping and star positions.

3. Examine the timekeeping systems in current use.

Page 2: 2. The Celestial Sphere Goals :

Astronomical Co-ordinate Systems:

All co-ordinate systems constructed on spheres are defined by a fundamental great circle (FGC) and a reference point (RP) on the FGC.

All co-ordinates are angles measured:(i) between great circles perpendicular to the FGC, or(ii) between small circles parallel to the FGC.

The FGC has two poles, and the RP is defined in a variety of ways, which accounts for slight differences from one system to another.

Page 3: 2. The Celestial Sphere Goals :

Terrestrial Co-ordinates.FGC = Earth’s equator: poles the North Pole and South Pole.RP = crossing point of equator by the Greenwich meridian.Co-ordinates:Longitude = angle measured east and west from the Greenwich meridian. Longitude meridians are great circles.Latitude = measured north and south (not plus or minus) from the Equator. Latitude parallels are small circles.Examples: Halifax. 63º 36'.0 W, 44º 36'.0 N Vancouver. 123º 04'.2 W, 49º 09'.0 N

Page 4: 2. The Celestial Sphere Goals :

Horizon System.FGC = horizon, with poles the zenith and nadir.RP = north point.Co-ordinates:azimuth = angle measured through east from 0º to 360. Azimuth circles are great circles.altitude = measured from horizon towards zenith (positive) or nadir (negative) from +90º to –90º. Alternate: zenith distance,z = 90º – altitude.

Page 5: 2. The Celestial Sphere Goals :
Page 6: 2. The Celestial Sphere Goals :

Meridian = NS line running through zenith.Prime vertical = EW line running through zenith.Use. Airport runways are designated by azimuth 10°, i.e. runway 32 aligns along azimuth 320° magnetic. Air mass, for correction of photometry, is calculated from zenith distance z.

Example Question. In what directions does runway 05/23 run?

Solution: Given the name of the runway, 05/23, it must run along azimuth directions 50° (northeast) and 230° (southwest), which are 180° apart.

Page 7: 2. The Celestial Sphere Goals :

Equatorial System.FGC = celestial equator (CE, projection on the sky of Earth’s equator), with poles the north and south celestial poles, NCP and SCP.RP = intersection point of meridian with CE (observer-oriented), or vernal equinox γ (sky-oriented).Co-ordinates:declination = angle measurednorth or south of CE from 0ºto +90 and 90° (δ).hour angle = angle measuredwest of meridian (HA), orright ascension = angle measuredeastward from vernal equinox (RA).

Page 8: 2. The Celestial Sphere Goals :
Page 9: 2. The Celestial Sphere Goals :
Page 10: 2. The Celestial Sphere Goals :

From relations for angles associated with parallel lines, 90° – θ = 90° – , i.e. θ = .

Page 11: 2. The Celestial Sphere Goals :
Page 12: 2. The Celestial Sphere Goals :
Page 13: 2. The Celestial Sphere Goals :
Page 14: 2. The Celestial Sphere Goals :
Page 15: 2. The Celestial Sphere Goals :
Page 16: 2. The Celestial Sphere Goals :

StarTrails1h exposure

Page 17: 2. The Celestial Sphere Goals :
Page 18: 2. The Celestial Sphere Goals :

The orbit of Earth about the Sun and the 23½° obliquity of the ecliptic (its angle relative to the normal to Earth’s orbital plane) give rise to Earth’s seasons.

Page 19: 2. The Celestial Sphere Goals :

Solar insolation as a function of season.

Page 20: 2. The Celestial Sphere Goals :
Page 21: 2. The Celestial Sphere Goals :

A typical sky scene showing seasonal variations in the Sun’s diurnal motion.

Page 22: 2. The Celestial Sphere Goals :

RA() and δ() during the year are defined by the apparent motion of the Sun in the sky along the ecliptic = Sun’s apparent path, and can be calculated directly or from tables.

Page 23: 2. The Celestial Sphere Goals :
Page 24: 2. The Celestial Sphere Goals :

Solar day (24h) is rotation of Earth relative to Sun, sidereal day (23h 56m) is rotation of Earth relative to stars.

Page 25: 2. The Celestial Sphere Goals :

HA and RA are measured in temporal units and are equivalent to angles. On the celestial equator: 1h = 15°, 1m = 15', and 1s = 15″, with the equalities changing by cos δ with increasing declination.

Because of their link to timekeeping, HA and RA are tied directly to sidereal (star) time and apparent solar time.

Sidereal time (SidT)= HA(γ)Apparent solar time = HA() + 12h

Now, HA(γ) = HA(*) + RA(*) = HA() + RA()

Thus, SidT = HA() + RA() = Apparent solar time 12h + RA()

Page 26: 2. The Celestial Sphere Goals :

By geometry and algebra, Sidereal Time = HA(γ)But HA(γ) = HA(*) + RA(*)

So Sidereal Time = HA(*) + RA(*)

Page 27: 2. The Celestial Sphere Goals :

Useful values:Vernal Equinox, March 20:RA() = 0h, δ() = 0°Summer Solstice, June 21:RA() = 6h, δ() = +23½°Autumnal Equinox, September 23:RA() = 12h, δ() = 0°Winter Solstice, December 22:RA() = 18h, δ() = 23½°

annual insolation

The actual dates of the equinoxes and solstices slowly change with time. They were March 25, June 25, September 25, and December 25 when Julius Caesar modified the original Roman calendar system (Julian Calendar) in 46 BC.

Page 28: 2. The Celestial Sphere Goals :

An example.

1. Towards what directions on the co-ordinate axes must an equatorial telescope be set in order to point it towards Betelgeuse, RA = 5h 56m, δ = +7° 25' at 5h sidereal time?

Page 29: 2. The Celestial Sphere Goals :

Solution: By definition, SidT = HA(γ) = HA(*) + RA(*)

5h = HA(*) + 5h 56m

And so HA(*) = 5h – 5h 56m = –0h 56m

The hour angle setting of the telescope should be set to –0h 56m, i.e. 56m east of the meridian.

And the declination setting of the telescope should be set to +7° 25'.

Page 30: 2. The Celestial Sphere Goals :

Another example.

2. Show that apparent solar time (AST) and sidereal time (SidT) are identical on the date of the autumnal equinox.

Page 31: 2. The Celestial Sphere Goals :

Solution: By definition, SidT = HA(γ) = HA(*) + RA(*)

The Sun is also a star, so SidT = HA() + RA()

But AST = HA() + 12h

And RA() = 12h at the Autumnal Equinox.

So at the Autumnal Equinox,

SidT = HA() + RA() = HA() + 12h = AST

i.e. Sidereal Time and Apparent Solar Time are identical on the date of the Autumnal Equinox.

Page 32: 2. The Celestial Sphere Goals :

3. When is the best time of year to observe the stars of Orion, RA = 5½h?Solution:The optimum time for observing any object is when it lies on the observer’s meridian at local midnight, which corresponds to 0h local apparent solar time (LAST).i.e. LAST = HA() + 12h = 0h (midnight)So HA() = 0h 12h = 24h 12h = 12h

Orion is then on the meridian, so local sidereal time = RA(*) = 5½h = HA() + RA() RA() = 5½hHA() = 5½h12h = 29½h12h = 17½h

The Sun is at RA = 17½h approximately one week prior to the winter solstice, i.e. around Dec. 15.

Page 33: 2. The Celestial Sphere Goals :

Ordering the Planets Outwards

Object Motion relative to the Stars

Stars infiniteSaturn 29.30 yearsJupiter 11.86 yearsMars 1.88 yearsSun 365¼ daysVenus 225 daysMercury 88 daysMoon 27½ days

Page 34: 2. The Celestial Sphere Goals :

Saturn governs the 1st hour of the 1st day, Jupiter the 2nd hour, Mars the 3rd hour, etc., and Mars the 24th hour. The Sun then governs the 1st hour of the 2nd day, the Moon the 1st hour of the 3rd day, Mars the 1st hour of the 4th day, Mercury the 1st hour of the 5th day, Jupiter the 1st hour of the 6th day, and Venus the 1st hour of the 7th day. The days of the week are therefore:

Saturn-daySun-dayMoon-dayMars-dayMercury-dayJupiter-dayVenus-day

Page 35: 2. The Celestial Sphere Goals :

North American time zones

Page 36: 2. The Celestial Sphere Goals :

World time zones ─ note the peculiarities

Page 37: 2. The Celestial Sphere Goals :

Calendars.Apparent solar time is defined by the passage of the Sun across the sky, but civil time is more closely related to the motion of the mean Sun, a fictitious object, across the sky.Mean solar time = HA(mean Sun) + 12h

The mean Sun differs from the true Sun in the following way. The true Sun travels along the ecliptic at a rate that varies according to the distance of Earth from the Sun. The mean Sun travels along the celestial equator at a uniform rate.Additional complications arise from the use of time zones and daylight saving time.

Page 38: 2. The Celestial Sphere Goals :

The analemma represents the equation of time = Apparent Solar Time – Mean Solar Time.

Page 40: 2. The Celestial Sphere Goals :

Length (days)Julian Gregorian

Month Calendar CalendarJanuary 31 31February 29 28March 31 31April 30 30May 31 31June 30 30Quintilus (July) 31 31Sextilus (August) 30 31September 31 30October 30 31November 31 30December 30 31

Page 41: 2. The Celestial Sphere Goals :

Important Calendar Dates

Calendar Event Julian Modern

Vernal Equinox March 25 March 20Summer Solstice June 25 June 21Autumnal Equinox Sept. 25 Sept. 23

Winter Solstice Dec. 25 Dec. 22

Page 42: 2. The Celestial Sphere Goals :
Page 43: 2. The Celestial Sphere Goals :

The year length varies according to the calendar system, which has changed from lunar calendars, through luni-solar calendars, to solar calendars, such as the Julian Calendar, Gregorian Calendar, and current modified Gregorian Calendar.

Variable star studies normally cite observations according to the Julian Date, JD, measured as the number of sequential days from noon, UT, on January 1, 4713 BC (named by Joseph Scaliger after his father Julius Scaliger), or, better yet, HJD = Heliocentric Julian Date (corrected to the barycentre of the solar system). Another term, modified Julian Date, MJD = JD 2400000.5, is occasionally used.

Page 44: 2. The Celestial Sphere Goals :

Ecliptic System.FGC = ecliptic, with poles the north and south ecliptic poles, NEP and SEP.RP = vernal equinox γ.Co-ordinates:celestial (or ecliptic) longitude, λ = angle measured eastward from γ from 0º to 360.celestial (or ecliptic)latitude, β = angle measured from ecliptic.The system is useful for studies of solar system objects.

Page 45: 2. The Celestial Sphere Goals :

Galactic System.FGC = Galactic equator (GE), defined by the Milky Way, with poles the north and south Galactic poles, NGP and SGP.RP = direction to the Galactic centre (GC), defined by Sgr A*.Co-ordinates:Galactic longitude, l = angle measured Eastward from GC from 0º to 360.Galactic latitude, b = angle measured north orsouth of GE from 0º to +90 and 90°.

Page 46: 2. The Celestial Sphere Goals :

Precession of the Equinoxes.Earth’s axis of rotation precesses relative to the perpendicular to its orbit because of gravitational influences by the Sun and Moon, but not in the fashion implied by the Wikipedia figure below. The sense of precession is actually opposite the sense of Earth’s rotation. Theperiod is ~25,725 years.

A top’sprecession.

Page 47: 2. The Celestial Sphere Goals :
Page 48: 2. The Celestial Sphere Goals :

Precession andthe location of the NCP. Note that the NCP was near the bright star Thuban near2700 BC, when the pyramids were built, andwas once nearVega, a name that means “fallen.”

Page 49: 2. The Celestial Sphere Goals :

Astronomical TerminologyZenith. The point in the sky directly overhead.Nadir. The point directly beneath one’s feet.Azimuth. A measurement of angle increasing from north

through east.Altitude (astronomical). A measurement of angular

distance from the true horizon upwards.Ecliptic. The great circle in the sky along which the Sun

appears to move because of Earth’s orbit about it.Right Ascension. A celestial co-ordinate like longitude on

Earth, increasing eastwards.Declination. A celestial co-ordinate like latitude on

Earth, measured from the celestial equator.Celestial Equator. The projection on the celestial sphere

of Earth’s equator.Celestial Sphere. The imaginary sphere centred on the

observer upon which the stars appear to be projected.

Page 50: 2. The Celestial Sphere Goals :

Astronomical Terminology (continued)Diurnal. = daily (once a day).Insolation. The amount of sunlight falling on Earth’s

surface.Constellation. A group of conspicuous stars designated

by ancient star gazers.Zodiacal Constellation. A constellation lying in the band

of sky around the ecliptic, where the Moon and planets are always found.

Solstice. Time of greatest or smallest declination for the Sun.

Equinox. Time when the Sun crosses the celestial equator. (Vernal = spring)

Stellar Aberration. The apparent displacement in a star’s location in the sky of at most 20½ seconds of arc resulting from Earth’s orbital motion about the Sun at a speed of 30 km/s.


Recommended