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This lesson covers orbital motion, gravitational force, and how gravity keeps planets, moons, and satellites in orbit, as required by the AQA GCSE Physics specification (4.8.1). This is a Physics-only topic. You need to understand how gravity provides the centripetal force for orbital motion, how orbital speed and radius are related, and the difference between circular and elliptical orbits.
Gravity is a non-contact force of attraction between any two objects that have mass. Every object with mass exerts a gravitational pull on every other object with mass. The strength of the gravitational force depends on:
A gravitational field is the region around a mass where another mass would experience a gravitational force. The gravitational field of a planet or star extends to infinity, but it becomes weaker with distance.
The gravitational field strength (g) at a point is the force per unit mass acting on an object at that point:
g = F / m
where:
| Location | Gravitational Field Strength (N/kg) |
|---|---|
| Earth (surface) | 9.8 |
| Moon (surface) | 1.6 |
| Mars (surface) | 3.7 |
| Jupiter (surface) | 24.8 |
| Sun (surface) | 274 |
Exam Tip: On Earth, g = 9.8 N/kg (often rounded to 10 N/kg in calculations). This means that every kilogram of mass experiences a gravitational force (weight) of 9.8 N. Weight = mass x gravitational field strength (W = mg). Do not confuse mass (kg) with weight (N).
It is essential to distinguish between mass and weight:
| Quantity | Definition | Unit | Changes with location? |
|---|---|---|---|
| Mass | The amount of matter in an object | kg | No — mass is the same everywhere |
| Weight | The gravitational force acting on an object | N | Yes — depends on gravitational field strength |
The equation linking weight, mass, and gravitational field strength is:
W = m x g
For example, an astronaut with a mass of 80 kg:
The astronaut's mass is always 80 kg, but their weight changes depending on the gravitational field strength at their location.
An orbit is the path of one object around another due to gravity. For example:
An orbiting object is constantly falling towards the larger body due to gravitational attraction. However, it also has a velocity at right angles to the direction of the gravitational force. The combination of:
produces a curved path — an orbit.
If the object were moving in a straight line, it would fly off into space. If it had no tangential velocity, it would fall straight towards the central body. The balance between these two produces the circular (or elliptical) orbital path.
Exam Tip: Gravity provides the centripetal force needed for orbital motion. A common exam question asks: "What provides the centripetal force for a planet orbiting the Sun?" The answer is: the gravitational attraction between the Sun and the planet. Do not say "centripetal force" as if it is a separate force — it is gravity acting as the centripetal force.
For an object moving in a circular orbit, a centripetal force is needed to keep it moving in a circle. This centripetal force is directed towards the centre of the circle (towards the larger body).
In the case of orbital motion:
graph TD
A["Central Body (e.g. Sun)"] --- B["Gravitational Force (centripetal force)"]
B --- C["Orbiting Body (e.g. Planet)"]
C --- D["Tangential Velocity"]
D --- E["Curved Orbital Path"]
style A fill:#f39c12,color:#fff
style C fill:#3498db,color:#fff
style B fill:#e74c3c,color:#fff
There is a clear relationship between the orbital speed, orbital radius, and orbital period of an orbiting object.
This is because:
| Planet | Average Distance from Sun (AU) | Orbital Period (years) | Average Orbital Speed (km/s) |
|---|---|---|---|
| Mercury | 0.39 | 0.24 | 47.4 |
| Venus | 0.72 | 0.62 | 35.0 |
| Earth | 1.00 | 1.00 | 29.8 |
| Mars | 1.52 | 1.88 | 24.1 |
| Jupiter | 5.20 | 11.86 | 13.1 |
| Saturn | 9.54 | 29.46 | 9.7 |
| Uranus | 19.19 | 84.01 | 6.8 |
| Neptune | 30.07 | 164.8 | 5.4 |
Exam Tip: Notice the pattern: as the distance from the Sun increases, the orbital period increases and the orbital speed decreases. If asked to explain why, state that at greater distances the gravitational force is weaker, so a lower speed is needed to maintain a stable orbit. Conversely, at shorter distances, the stronger gravitational pull requires a faster orbital speed.
In a perfectly circular orbit, the distance between the orbiting object and the central body is constant. The orbital speed is also constant. While no real orbit is perfectly circular, many planetary orbits are very nearly circular (Earth's orbit has an eccentricity of only about 0.017).
For a circular orbit:
An elliptical orbit is an elongated, oval-shaped orbit. In an elliptical orbit:
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