l l' F D ω GMST + π φ0 PERIOD ΔUT1 ΔD Δω (deg.) (hours) Fi Gi Fi' Gi' Fi" Gi" Q1 -1 0 -2 0 -2 1 -90 26.868 0.02 0.05 -1.4 2.8 1.2 -2.4 O1 0 0 -2 0 -2 1 -90 25.819 0.12 0.16 -7.1 9.4 6.0 -7.9 P1 0 0 -2 2 -2 1 -90 24.066 0.03 0.05 -1.8 3.2 1.5 -2.7 K1 0 0 0 0 0 1 90 23.935 0.09 0.18 -5.4 11.2 4.6 -9.4 N2 -1 0 -2 0 -2 2 0 12.658 -0.04 -0.02 4.5 -1.8 -3.8 1.6 M2 0 0 -2 0 -2 2 0 12.421 -0.16 -0.07 19.6 -8.7 -16.6 7.4 S2 0 0 -2 2 -2 2 0 12.000 -0.08 0.00 9.5 -0.5 -8.1 0.4 K2 0 0 0 0 0 2 0 11.967 -0.02 0.00 2.5 -0.5 -2.1 0.4 Delaunay arguments (IERS Conventions 2000, from Simon et al., 1994, Astron. Astrophys. 282, 663-683): Mean anomaly of the Moon : l = 134°.963 402 51 + 1 717 915 923.2178" t + 31".879 2 t2 + 0".051 635 t3 - 0".000 244 70 t4 Mean anomaly of the Sun : l'= 357°.529 109 18 + 129 596 581.0481" t - 0".553 2 t2 - 0".000 136 t3 - 0".000 011 49 t4 F = L - Ω with L mean longitude of the Moon F = 93°.272 090 62 + 1 739 527 262.8478" t - 12".751 2 t2 - 0".001 037 t3 + 0".000 004 17 t4 Mean elongation of the Moon from the Sun : D = 297°.850 195 47 + 1 602 961 601.2090" t - 6".370 6 t2 + 0".006 593 t3 - 0".000 031 69 t4 Mean longitude of the ascending node of the Moon : Ω = 125°.044 555 01 - 6 962 890.543 1" t + 7".472 2 t2 + 0".007 702 t3 - 0".000 059 39 t4 where t is measured un Julian Centuries of 36525 days of 86400 seconds of Dynamical Time since J2000.0. Rotation angle in arcseconds : Greenwich Mean Sidereal Time + 180° GMST + π = (67310.54841 + (876600d0*3600 + 8640184.812866) t + 0.093104 t2 - 6.2 10-6 * t3 )*15 + 648000.0 where t is measured un Julian Centuries of 36525 days of 86400 seconds of Dynamical Time since J2000.0.