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Solar Motion Corrections to μ and vr
Suppose a star has known α, δ, μα , μδ ,π and vr.
Furthermore suppose that the known celestial
coordinates of the solar apex are A and D
and the solar motion is v¤ . Unknown
quantities to be determined are τ, the
proper motion component normal to the
great circle passing through the star,
apex and antapex; υ, the proper motion
component in the direction of the
antapex and τ', υ' and vr.', the values
of τ, υ and vr after corrections for solar
motion. Also initially unknown are the
auxiliary quantities λ, the angular
separation of the star and the apex, and
-ψ, the position angle of the apex with
respect to the star.One can use the following three relationships,
derived from spherical trigonometry, to obtain the
values of λ and ψ:cos λ = sin D sin δ + cos D cos δ cos (α - A) (1)
sin λ sin ψ = cos D sin (α - A) (2)
sin λ cos ψ = sin D cos δ - cos D sin δ cos (α - A). (3)
Equation (1) yields a unique value for λ (since 0° £ λ £ 180°). Equation 2 yields a value for sin ψ and equation (3) yields a value for
cos ψ, from which a unique solution can be obtained for ψ (0° £ ψ < 360°). Once λ and ψ are determined the following five relationships, obtained from the above figure, yield the values of τ, υ, τ', υ' and vr':τ = 15 μα cos δ cos ψ + μδ sin ψ (4)
υ = 15 μα cos δ sin ψ - μδ cos ψ (5)
τ' = τ (6)
υ' = υ - v¤ sin(λ)π / 4.74 (7)
and
vr.' = vr. + v¤ cos λ. (8)
Note the unit conventions assumed in these equations: μα [s/yr], μδ ["/yr], π ["], vr [km/s], v¤ [km/s], τ ["/yr], υ ["/yr], τ' ["/yr], υ' ["/yr] and vr' [km/s].

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