[gamb, phib, psib, epsa] = ERFA.pfw06(date1, date2)
Precession angles, IAU 2006 (Fukushima-Williams 4-angle formulation).
date1,date2 double TT as a 2-part Julian Date (Note 1)
gamb double F-W angle gamma_bar (radians)
phib double F-W angle phi_bar (radians)
psib double F-W angle psi_bar (radians)
epsa double F-W angle epsilon_A (radians)
- The TT date date1+date2 is a Julian Date, apportioned in any convenient way between the two arguments. For example, JD(TT)=2450123.7 could be expressed in any of these ways, among others:
date1 date2
2450123.7 0.0 (JD method)
2451545.0 -1421.3 (J2000 method)
2400000.5 50123.2 (MJD method)
2450123.5 0.2 (date & time method)
The JD method is the most natural and convenient to use in cases where the loss of several decimal digits of resolution is acceptable. The J2000 method is best matched to the way the argument is handled internally and will deliver the optimum resolution. The MJD method and the date & time methods are both good compromises between resolution and convenience.
e = J2000.0 ecliptic pole,
p = GCRS pole,
E = mean ecliptic pole of date,
and P = mean pole of date,
the four Fukushima-Williams angles are as follows:
gamb = gamma_bar = epE
phib = phi_bar = pE
psib = psi_bar = pEP
epsa = epsilon_A = EP
- The matrix representing the combined effects of frame bias and precession is:
PxB = R_1(-epsa).R_3(-psib).R_1(phib).R_3(gamb)
- The matrix representing the combined effects of frame bias, precession and nutation is simply:
NxPxB = R_1(-epsa-dE).R_3(-psib-dP).R_1(phib).R_3(gamb)
where dP and dE are the nutation components with respect to the ecliptic of date.
Hilton, J. et al., 2006, Celest.Mech.Dyn.Astron. 94, 351
eraObl06 mean obliquity, IAU 2006
This revision: 2021 May 11
Copyright (C) 2013-2021, NumFOCUS Foundation. Derived, with permission, from the SOFA library.