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Astronomy Principles and Practice Fourth Edition.pdf

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148 The reduction of positional observations: II<br />

1. A star in the ecliptic has celestial longitude 42 ◦ . If the Sun’s longitude is 102 ◦ , calculate the change in the<br />

star’s longitude due to aberration.<br />

2. A star has a celestial longitude of 0 ◦ . What is the star’s apparent longitude on (i) March 21st, (ii) June 21st,<br />

(iii) September 21st, (iv) December 21st<br />

3. Given that the constant of aberration for an observer on Earth is 20·′′ 49 <strong>and</strong> that the distance of Mars from<br />

the Sun is 1·5 astronomical units, calculate the value of the constant of aberration for an observer on Mars<br />

assuming circular orbits.<br />

4. Find the present longitude of the point which will be the First Point of Aries 5200 years hence. Show that<br />

the north celestial pole will then be about 27 ◦ from the present pole.<br />

5. The star 36 Draconis is near the north pole of the ecliptic. Neglecting its parallax, at what part of the year<br />

will (i) its right ascension, (ii) its north declination, be (a) maximum, (b) minimum, due to aberration<br />

6. Show that for a star whose true position is on the celestial equator, the change in its declination due to<br />

aberration is<br />

−κ sin ε cos λ ⊙<br />

where κ is the constant of aberration. ε is the obliquity of the ecliptic <strong>and</strong> λ ⊙ the longitude of the Sun.<br />

7. Calculate the displacements in celestial longitude <strong>and</strong> latitude, due to aberration, of a star in celestial latitude<br />

+20 ◦ , the Sun’s longitude at the instant concerned being the same as that of the star.<br />

If the stellar parallax is 0·′′ 32, what are the corresponding displacements due to parallax<br />

8. The celestial latitude <strong>and</strong> longitude of a star at the present time are 5 ◦ 14 ′ N, 327 ◦ 47 ′ . Calculate the time<br />

which must elapse before the star becomes an equatorial star.<br />

9. Show that at any place, <strong>and</strong> at any instant, there is a position of a star such that the effect of annual aberration<br />

is equal <strong>and</strong> opposite to that of refraction. Find the zenith distance of the star at midnight on the shortest day,<br />

given that the ratio of the constants of refraction <strong>and</strong> aberration is 2·85.<br />

10. Assuming the obliquity of the ecliptic to be constant, show that 13 000 years hence a star whose present<br />

coordinates are 18 h <strong>and</strong> 47 ◦ S will then lie on the celestial equator. What will then be its corresponding right<br />

ascension<br />

11. If at a place in north latitude φ, the star in problem 10 just comes above the horizon at the present date at<br />

upper culmination, find (i) the value of φ, (ii) the star’s altitude at upper culmination 13 000 years hence at<br />

the same place.<br />

12. The present equatorial coordinates of a star are 3 h <strong>and</strong> 0 ◦ . Calculate when next the star’s declination will be<br />

zero.<br />

13. If the date in the year when Sirius rises just after sunset changes by one day in 71 years, calculate<br />

(approximately) the value of the constant of precession, <strong>and</strong> the difference in the lengths of the tropical<br />

<strong>and</strong> sidereal years, given that the length of the tropical year is 365·2422 mean solar days.<br />

14. Calculate (i) the ecliptic coordinates, (ii) the equatorial coordinates, referred to the present pole <strong>and</strong> equator,<br />

of the point on the celestial sphere which will, after one-third of the precessional period, become the north<br />

celestial pole.<br />

15. The present ecliptic longitude <strong>and</strong> latitude of a star are 32 ◦ <strong>and</strong> 25 ◦ N, respectively. Find the declination <strong>and</strong><br />

right ascension of the star at its minimum distance from the pole <strong>and</strong> calculate the time when this will occur.

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