This post expands on a small part of the post Demystifying the Analemma by M. Tirado.

Apparent solar declination given δ by

δ = sin^{−1}( sin(ε) sin(θ) )

where ε is axial tilt and θ is the angular position of a planet. See Tirado’s post for details. Here I want to unpack a couple things from the post. One is that that declination is approximately

δ = ε sin(θ),

the approximation being particular good for small ε. The other is that the more precise equation approaches a triangular wave as ε approaches a right angle.

Let’s start out with ε = 23.4° because that is the axial tilt of the Earth. The approximation above is a variation on the approximation

sin φ ≈ φ

for small φ when φ is measured in radians. More on that here.

An angle of 23.4° is 0.4084 radians. This is not particularly small, and yet the approximation above works well. The approximation above amounts to approximating sin^{−1}(*x*) with *x*, and Taylor’s theorem tells the error is about *x*³/6, which for *x* = sin(ε) is about 0.01. You can’t see the difference between the exact and approximate equations from looking at their graphs; the plot lines lie on top of each other.

Even for a much larger declination of 60° = 1.047 radians, the two curves are fairly close together. The approximation, in blue, slightly overestimates the exact value, in gold.

This plot was produced in Mathematica with

ε = 60 Degree Plot[{ε Sin[θ] ], ArcSin[Sin[ε] Sin[θ]]}, {θ, 0, 2π}]

As ε gets larger, the curves start to separate. When ε = 90° the gold curve becomes exactly a triangular wave.

**Update**: Here’s a plot of the maximum approximation error as a function of ε.