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Astronomy Principles and Practice Fourth Edition.pdf

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90 The celestial sphere: timekeeping systems<br />

Figure 9.2. The relation between local sidereal time <strong>and</strong> Greenwich sidereal time.<br />

Then the Greenwich hour angle of X is GPX which is the longitude λW of the observer.<br />

The Greenwich hour angle of the vernal equinox is GP which is equal to the hour angle<br />

XP plus the longitude λW of the observer.<br />

Or<br />

GHA = HA + λW.<br />

But the hour angle of is the LST, therefore we may write<br />

GAST = LST + λW.<br />

If were any celestial object ⋆, we would have<br />

GHA⋆ = HA⋆ + λW.<br />

It is easily seen that if the longitude of the local observer had been east we would have written<br />

GHA⋆ = HA⋆ − λE.<br />

If we agree that a western longitude is positive <strong>and</strong> eastern is negative, we may combine these<br />

relations to give<br />

GHA⋆ = HA⋆ + λ (9.2)<br />

a very important expression often remembered by the mnemonic:<br />

Longitude east, Greenwich least,<br />

Longitude west, Greenwich ‘best’.<br />

The sidereal day at a given place begins when the vernal equinox transits across the observer’s<br />

meridian <strong>and</strong> ends 24 sidereal hours later when is once more on the meridian. Thus, one sidereal<br />

day is the time taken for one rotation of the Earth about its axis with respect to the stellar background.<br />

The sidereal clock in an observatory should, therefore, read 0 h when is on the meridian. We have<br />

the following table:<br />

1 sidereal day = 24 sidereal hours<br />

1 sidereal hour = 60 sidereal minutes<br />

1 sidereal minute = 60 sidereal seconds.

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