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USNO Circular 179 - U.S. Naval Observatory

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48 PRECESSION & NUTATION<br />

S1 = sin (ɛ)<br />

S2 = sin (−∆ψ)<br />

S3 = sin (−ɛ − ∆ɛ)<br />

then the nutation matrix can also be written:<br />

⎛<br />

N(t) =<br />

⎜<br />

⎝<br />

C1 = cos (ɛ)<br />

C2 = cos (−∆ψ) (5.20)<br />

C3 = cos (−ɛ − ∆ɛ)<br />

C2 S2C1 S2S1<br />

−S2C3 C3C2C1 − S1S3 C3C2S1 + C1S3<br />

S2S3 −S3C2C1 − S1C3 −S3C2S1 + C3C1<br />

⎞<br />

⎟<br />

⎠ (5.21)<br />

Where high accuracy is not required, coordinates corrected for nutation in right ascension and<br />

declination can be obtained from<br />

αt ≈ αm + ∆ψ (cos ɛ ′ + sin ɛ ′ sin αm tan δm) − ∆ɛ cos αm tan δm<br />

δt ≈ δm + ∆ψ sin ɛ ′ cos αm + ∆ɛ sin αm (5.22)<br />

where (αm, δm) are coordinates with respect to the mean equator and equinox of date (precession<br />

only), (αt, δt) are the corresponding coordinates with respect to the true equator and equinox of<br />

date (precession + nutation), and ɛ ′ is the true obliquity. Note the tan δm factor in right ascension<br />

that makes these formulas unsuitable for use close to the celestial poles.<br />

The traditional formula for the equation of the equinoxes (the difference between apparent and<br />

mean sidereal time) is ∆ψ cos ɛ ′ , but in recent years this has been superceded by the more accurate<br />

version given in eq. 2.14.<br />

5.4.3 Alternative Combined Transformation<br />

The following matrix, C(t), combines precession, nutation, and frame bias and is used to transform<br />

vectors from the GCRS to the Celestial Intermediate Reference System (CIRS). The CIRS is defined<br />

by the equator of the CIP and an origin of right ascension called the Celestial Intermediate Origin<br />

(CIO). The CIO is discussed extensively in Chapter 6. There, the CIRS is symbolized Eσ; it is<br />

analogous to the true equator and equinox of date, but with a different right ascension origin.<br />

The matrix C(t) is used in the sense<br />

r CIRS = C(t) r GCRS<br />

(5.23)<br />

and the components of C(t), as given in the IERS Conventions (2003) and The Astronomical<br />

Almanac, are<br />

⎛<br />

⎞<br />

C(t) = R3(−s)<br />

⎜<br />

⎝<br />

1 − bX 2 −bXY −X<br />

−bXY 1 − bY 2 −Y<br />

X Y 1 − b(X 2 + Y 2 )<br />

⎟<br />

⎠ (5.24)<br />

where X and Y are the dimensionless coordinates of the CIP in the GCRS (unit vector components),<br />

b = 1/(1 + Z), Z = √ 1 − X 2 − Y 2 , and s is the CIO locator, a small angle described in Chapter 6.<br />

All of these quantities are functions of time. R3 is a standard rotation around the z axis; see<br />

“Abbreviations and Symbols Frequently Used” for a precise definition.

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