Presets
Planet tracked from Earth
Live readouts
Gear-train designer
Independent checks
Geocentric longitude over ±1.5 years
The science
Each planet follows a Kepler ellipse: M = 2π(t/T) + M0, E − e sin E = M (solved by Newton iteration), r = a(1 − e cos E), true anomaly from tan(ν/2) = √((1+e)/(1−e)) tan(E/2). Kepler's third law T² = a³ (years, AU) links size and period; the clockwork orrery realises the period ratios with meshing gears, whose speeds obey teethA ωA = teethB ωB.
Seen from Earth, an outer planet appears to loop backwards (retrograde) around opposition, when Earth overtakes it on the inside track; Mercury and Venus loop around inferior conjunction. The synodic period is 1/Tsyn = |1/T1 − 1/T2|.
Simplifications: all orbits coplanar (so no latitude), two-body Kepler orbits with no mutual perturbations, orbital elements fixed at J2000 values, so dates are illustrative rather than ephemeris-grade. Gear ratios: best rational approximation with both tooth counts within the chosen limit.