Astronomy Lab · Orbital mechanics

Why Don't Planets Move at Constant Speed?

A planet does not simply travel around the Sun at one fixed speed. Its orbit is an ellipse, its distance from the Sun changes, and so does its orbital velocity. Johannes Kepler found the mathematical pattern behind that motion more than four centuries ago.

The key idea: a planet moves fastest when it is closest to the Sun and slowest when it is farthest away. Kepler's laws describe this motion; Newton's law of gravity later explained why it happens.
From circles to ellipses

Three astronomers changed our view of planetary motion

Copernicus placed the planets in orbit around the Sun. Tycho Brahe then accumulated exceptionally precise observations of planetary positions. Johannes Kepler used those observations — especially of Mars — to discover that planetary orbits are not perfect circles.

1543

Copernicus

The heliocentric model places Earth and the other planets in motion around the Sun.

1609

Kepler's first two laws

In Astronomia Nova, Kepler describes elliptical orbits and the equal-area rule.

1619

Kepler's third law

Kepler reveals the mathematical relationship between orbital period and orbital size.

Kepler's three laws

The rules behind planetary orbits

1

Orbits are ellipses

Every planet follows an elliptical orbit with the Sun located at one focus — not at the centre of the ellipse.

2

Equal areas in equal times

A line from the Sun to the planet sweeps equal areas during equal intervals of time. The planet therefore moves faster near perihelion and slower near aphelion.

3

P² is proportional to a³

The farther a planet is from the Sun, the longer it takes to complete its orbit according to a precise mathematical relation.

Interactive experiment

Watch Kepler's second law in action

Move the planet around an exaggerated elliptical orbit. The orbit is deliberately more eccentric than Earth's so that the speed change is easy to see.

Move around the orbit

Position Perihelion
Relative speed Fastest

The Sun is at a focus of the ellipse. When the planet is close to the Sun it must cover a greater length of orbit in a given time to sweep the same area.

Kepler's third law

Measure distance from orbital period

For planets orbiting the Sun, if the orbital period P is measured in Earth years and the semi-major axis a in astronomical units, Kepler's third law becomes particularly simple.

P² = a³
P = orbital period in years · a = semi-major axis in AU

This means we can estimate a planet's orbital size from nothing more than its period:

a = ∛(P²)
Example · Jupiter

How far is Jupiter from the Sun?

Jupiter takes about 11.86 Earth years to complete one orbit. Kepler's third law therefore gives:

a = ∛(11.86²) ≈ 5.20 AU
11.86 yr
Orbital period

One Jovian year.

≈5.20 AU
Semi-major axis

About 5.2 times Earth's orbital scale.

≈778 million km
Mean orbital scale

Approximately the Sun–Jupiter semi-major axis expressed in kilometres.

Try it yourself

Turn an orbital period into a distance

Enter an orbital period in Earth days. The calculator converts the period to years and applies Kepler's third law.

Orbital period 0.615 yr
Compared with Earth 0.62×
Semi-major axis 0.723 AU · ≈ 108 million km
Venus completes an orbit in about 224.7 days, giving a semi-major axis of about 0.723 AU.
Orbit size is drawn relative to Earth's 1 AU orbit. The drawing is schematic, not a full orbital simulation.
Orbital period vs synodic period

Why does Jupiter return to opposition every 399 days if its orbit takes nearly 12 years?

The orbital period measures one complete revolution around the Sun. The synodic period measures the time between repeated configurations as seen from Earth — for example, one opposition of Jupiter to the next.

Because Earth is moving too, we do not wait an entire Jovian year for Earth to catch Jupiter again. For an outer planet the relation is:

1 / S = 1 / PEarth − 1 / Pplanet

For Jupiter this gives a synodic period of roughly 399 days. For an inner planet such as Venus, the corresponding relationship uses the difference between the inner planet's faster orbital frequency and Earth's.

Kepler described it. Newton explained it.

Gravity provides the missing physics

Kepler's laws were empirical: they described planetary motion with remarkable accuracy without identifying the underlying force. Decades later, Isaac Newton showed that the same gravitational attraction that makes objects fall on Earth can account for planetary orbits.

That connection transformed celestial mechanics. The motions of planets, moons, comets and spacecraft could now be understood using the same physical principles.

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