• Pixel-art sticker of Ellipsa, personifying Kepler's First Law, with the caption “Not A Circle. An Ellipse.”

IndexRelativity & CosmosSticker

Ellipsa

Kepler's First Law Physics

\[r = \frac{a(1-e^2)}{1+e\cos\theta}\]
Regular price $4.99 USD
Regular price Sale price $4.99 USD
Sale Sold out

Meet Ellipsa, a planet tracing an ellipse with her star at one focus, as Kepler published in 1609. Earth's orbit is only slightly stretched, with e ≈ 0.0167: about 147.1 million km at perihelion and 152.1 million km at aphelion. Pixel-art kiss-cut sticker in 2, 3, 4 and 6 inches; equation, symbols and sources in the physics panel below.

Size
Surface

Flat $6 shipping worldwideMade to order, ships in 2–5 business days

Details

Size3″ × 3″

3″ × 3″ kiss-cut sticker.

Shipping

Flat $6 shipping on every order, worldwide, whatever's in it.

Delivery times & where we ship

Returns & replacements21 days

Every item is printed to order, so we can’t accept returns or exchanges for change of mind, or if you ordered the wrong size or colour.

Print defect, misprint, damage or the wrong item? We’ll send a free replacement, or a refund if you prefer. Report it within 21 days of delivery with a photo; no need to send it back.

Full refund & replacement policy

The physics

Meet Ellipsa, a planet tracing an ellipse with her star sitting at one focus.

Johannes Kepler, working from Tycho Brahe's careful observations of Mars, published in 1609 that planets move on ellipses with the Sun at one focus, not at the centre. Newton later showed that this follows from an inverse-square law of gravity. In polar form the orbit is r = a(1 − e²)/(1 + e cos θ), where θ is measured from the closest point, perihelion.

Earth's orbit has a ≈ 149.6 million km and e ≈ 0.0167. At perihelion, θ = 0, r = a(1 − e) ≈ 147.1 million km. At aphelion, θ = 180°, r = a(1 + e) ≈ 152.1 million km, a difference of about 5 million km.

The same equation describes comets on long, stretched orbits, satellites around Earth, and binary stars, and it is used to plan spacecraft trajectories.

Earth's seasons do not come from this distance change; we are closest to the Sun in early January. The sticker uses e = 0.6 to make the shape obvious. Real orbits also shift slowly because of other planets' pulls.

Equations

\[r = \frac{a(1-e^2)}{1+e\cos\theta}\]
Symbols
SymbolMeaningUnit
\(r\) distance from the Sun \(\mathrm{m}\)
\(a\) semi-major axis \(\mathrm{m}\)
\(e\) eccentricity —
\(\theta\) angle from closest approach \(\mathrm{rad}\)