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Astronomy Principles and Practice Fourth Edition.pdf

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Effect of precession on a star’s equatorial coordinates 143<br />

Figure 11.8. Measurement of the position of .<br />

Figure 11.9. The celestial sphere illustrating the precessional movement of the celestial equator.<br />

11.9 Effect of precession on a star’s equatorial coordinates<br />

Let us consider now the sort of changes made in the star’s coordinates by precession, taking the<br />

precessional period to be 26 000 years. In figure 11.9, the north pole K of the ecliptic is set at the<br />

top of the diagram, with the ecliptic as shown. This is often a convenient orientation for a diagram in<br />

problems on precession where the north celestial pole <strong>and</strong> the celestial equator shift.<br />

Let P 1 , P 2 , P 3 , be the positions of the north celestial pole now (2000 AD say), one-quarter <strong>and</strong><br />

one-half of the precessional period later. The corresponding positions of are 1 , 2 , 3 . The<br />

various celestial equators are also inserted.<br />

Consider a star whose present right ascension <strong>and</strong> declination are 0 h <strong>and</strong> 0 ◦ respectively. The star<br />

is, therefore, at 1 on the celestial sphere.<br />

By 8500 AD, the First Point of Aries <strong>and</strong> the north celestial pole have moved to positions 2 <strong>and</strong><br />

P 2 because of precession, <strong>and</strong> the meridian from the north celestial pole of that date through the star<br />

will cut the equator of that date at A. The star’s equatorial coordinates are then RA = 6 h ,Dec= ε ◦ N,<br />

since 2 A is of length 90 ◦ . That this is so is seen from the fact that 2 is the pole of the great circle<br />

KP 2 1 .

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