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Astronomy Principles and Practice Fourth Edition.pdf

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Chapter 9<br />

The celestial sphere: timekeeping systems<br />

9.1 Introduction<br />

Primitive people based their sense of the passage of time on the growth of hunger or thirst <strong>and</strong> on<br />

impersonal phenomena such as the changing altitude of the Sun during a day, the successive phases<br />

of the Moon <strong>and</strong> the changing seasons. By about 2000 BC civilizations kept records <strong>and</strong> systematized<br />

the impersonal phenomena into the day, the month <strong>and</strong> the year. We have seen that emphasis was<br />

given to the year as a unit of time by their observation that the Sun made one revolution of the stellar<br />

background in that period of time.<br />

Since everyday life is geared to daylight, the Sun became the body to which the system of<br />

timekeeping used by day was bound. The apparent solar day was then the time between successive<br />

passages of the Sun over the observer’s meridian or the time during which the Sun’s hour angle<br />

increased by 24 h (360 ◦ ). In a practical way the Sun was noted to be on the meridian when the shadow<br />

cast by a vertical pillar was shortest.<br />

However, the apparent diurnal rotation of the heavens provided another system of timekeeping<br />

called sidereal time, based on the rotation of the Earth on its axis. The interval between two successive<br />

passages of a star across the observer’s meridian was then called a sidereal day. Early on in the history<br />

of astronomy it was realized that the difference between the two systems of timekeeping—solar <strong>and</strong><br />

stellar—was caused by the orbital motion of the Sun relative to Earth. Thus, in figure 9.1, if two<br />

successive passages of the star over the observer’s meridian define a sidereal day (the star being taken<br />

to be at an infinite distance effectively from the Earth), the Earth will have rotated the observer O<br />

through 360 ◦ from O 1 to O 2 . In order that one apparent solar day will have elapsed, however, the<br />

Earth will have to rotate until the observer is at O 3 when the Sun will again be on the meridian. Since<br />

the Earth’s radius vector SE sweeps out about 1 ◦ per day <strong>and</strong> the Earth rotates at an angular velocity<br />

of about 1 ◦ per 4 minutes, the sidereal day is consequently about 4 minutes shorter than the average<br />

solar day.<br />

We will now consider these systems in greater detail.<br />

9.2 Sidereal time<br />

We have seen that the First Point of Aries (Vernal Equinox ) is the reference point chosen on the<br />

rotating celestial sphere to define the sidereal day. The time between successive passages of the vernal<br />

equinox across the observer’s meridian is one sidereal day. So the hour angle of the vernal equinox<br />

increases from 0 h to 24 h <strong>and</strong> the local sidereal time (LST) is defined as the hour angle of the vernal<br />

equinox (HA). The LST, as its name implies, depends upon the observer’s longitude on the Earth’s<br />

surface.<br />

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