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Astronomy / Earth

Seasons and obliquity

Why summer is warm: not because the Earth is closer to the Sun (it is closer in January) but because the axis leans, and a leaning hemisphere gets a higher Sun for longer. The Earth on its orbit with its axis fixed in space, lit from where the Sun is; an observer at any latitude with the day's Sun arc over the horizon; day length, noon altitude and daily insolation from the geometry, and the two hemispheres through the year.

Seasons and obliquity — Actual application image
Actual application image

What happens

The Earth is nearest the Sun in January. That is not when the north is warm, so distance is not the reason - the axis is. It leans 23.4° and points the same way in space all year, so in June the northern hemisphere is tipped toward the Sun: the Sun climbs higher at noon, stays up longer, and puts more energy on each square metre of ground. Six months later the same lean tips it away. The tilt changes Munich's daily sunlight five-fold between June and December; the changing distance changes it by seven percent, and the wrong way round for the north. Slide the obliquity to zero and the seasons vanish; slide it to 90° and the poles take turns facing the Sun. Tick the observer's sky to see the day's Sun arc from the ground.

Equations used in the module
Equations
δ = asin(sin ε · sin λ)
H = acos(−tan φ · tan δ)
Q = (S₀/π)(a/r)² (H sin φ sin δ + cos φ cos δ sin H)
r/a = (1 − e²)/(1 + e cos ν)
day length = 24 H/π,   noon altitude = 90° − |φ − δ|

Related experiments

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Eclipse geometry and Saros — Actual application image

Astronomy / Earth

Eclipse geometry and Saros

Why a new moon is usually not an eclipse, what decides total against annular, and why the pattern repeats every eighteen years and eleven days. The Moon's orbit tilted 5° with its line of nodes, the umbra and penumbra as cones that reach the Earth or fall short, an observer at any latitude who sees the discs at their true sizes, and a table of the run's eclipses with the one a Saros later beside each. An idealised orbital model - circular orbits, mean motions - so it explains eclipses and dates none.

Saturn's rings — Actual application image

Astronomy

Saturn's rings

A ring is not a disc: every particle keeps its own Kepler period, so the inner edge laps the outer and any pattern shears away. Where the gaps are is a separate question, and the resonance circles answer it.

Exoplanet observatory — Actual application image

Astronomy

Exoplanet observatory

Reveal an unseen planet with transit photometry and stellar radial velocity. Record noisy observations, infer radius and mass, and explore the limits of those inferences.