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A Level · Cambridge (CIE) · 9702

Analyse circular and geostationary orbits

Relate gravitational attraction to centripetal acceleration and identify the defining properties of a geostationary orbit.

Section 13 · Gravitational fields

Gravitational fields · Cambridge International AS & A Level Physics 9702 · 13.2

A Level; Cambridge International Physics 9702, 2025–2027 syllabus, Topic 13. These original explanations and calculations are study aids; full timed assessment and human subject-teacher review remain outstanding.

Before you begin

  • Use Newton's laws, circular motion, vectors, scientific notation and SI units.

Work on paper. Try each question before revealing help, and explain why your method works.

Quick readiness check

What supplies the centripetal resultant for a satellite in a circular orbit?

What you will learn

  • Analyse a circular orbit by equating gravity and the required centripetal resultant
  • Relate orbital speed and radius to the central mass
  • State the period, direction and equatorial plane of a geostationary orbit

Gravity supplies the orbital resultant

For a satellite of mass m orbiting a much larger mass M at radius r, the gravitational force is GMm/r². In a circular orbit, this supplies the inward centripetal resultant mv²/r.

Equating these expressions gives v² = GM/r. The satellite mass cancels: for a given central mass and orbital radius, the circular orbital speed does not depend on the satellite's mass. The orbit radius is measured from the centre of the planet.

Geostationary satellites remain above one longitude

A geostationary satellite has an orbital period of 24 hours, moves from west to east and travels in a circular orbit directly above Earth's Equator. Its angular speed matches Earth's rotation, so it remains above the same point on the surface.

A polar orbit or a period unlike Earth's rotation cannot remain fixed above one place. Do not confuse a satellite that merely passes over the same region with a geostationary satellite.

GMm/r² = mv²/r · geostationary: 24 h, west to east, above the Equator

Pause and explain

Which description is required for a geostationary satellite?

Put the idea to work

Worked example

A satellite orbits a planet of mass 6.0 × 10²⁴ kg at radius 7.0 × 10⁶ m. Estimate its circular speed.

Show the worked solution
  1. Equate gravity to centripetal force to get v = √(GM/r).
  2. Substitute G = 6.67 × 10⁻¹¹ N m² kg⁻².
  3. Check that the result has units m s⁻¹.

Answer v ≈ √(6.67 × 10⁻¹¹ × 6.0 × 10²⁴ / 7.0 × 10⁶) ≈ 7.6 × 10³ m s⁻¹.

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From guided practice to a new situation

Write your answer and reasoning first. Use a hint only if you are stuck. The model solution is for self-checking; your written work is not automatically marked.

1 · Guided

Starting from gravity and centripetal force, show the equation for the speed of a satellite in a circular orbit.

Give me a hint

Set GMm/r² equal to mv²/r and cancel common factors carefully.

Compare my reasoning
  1. GMm/r² = mv²/r.
  2. Cancel m and multiply by r.
  3. v² = GM/r, so v = √(GM/r).

The circular orbital speed is v = √(GM/r).

Look for these in your work

  • Two force expressions equated
  • Satellite mass cancelled
  • Speed relation derived
2 · Independent

A planet's mass is unchanged and an orbit radius increases from r to 4r. Compare the circular orbital speeds.

Give me a hint

Use v² = GM/r and compare speeds, not squared speeds.

Compare my reasoning
  1. At 4r, v₂² = GM/(4r) = v₁²/4.
  2. Take the square root of the ratio.
  3. v₂ = v₁/2.

The circular orbital speed at 4r is half the speed at r.

Look for these in your work

  • Radius ratio applied
  • Square-root step included
  • Speed ratio stated
3 · Transfer

A satellite is 24 hours from completing an orbit but travels west to east in a plane tilted away from the Equator. Is it geostationary? Explain.

Give me a hint

Check the complete definition, including orbital plane, rather than using period alone.

Compare my reasoning
  1. Its period matches 24 hours.
  2. A geostationary orbit must also be directly above the Equator and move west to east.
  3. The tilted orbital plane fails the equatorial condition, so it is not geostationary.

No. The 24-hour period and direction are insufficient because its orbit is not above the Equator.

Look for these in your work

  • Period checked
  • Equatorial requirement applied
  • Conclusion justified

Common mistakes

  • Using a satellite's height above a planet where orbital radius is needed
  • Assuming orbital force depends on satellite mass after it cancels
  • Describing any 24-hour orbit as geostationary without its direction and plane
Recall without your notes

What can you explain now?

What supplies the centripetal resultant for a satellite in a circular orbit?

Compare with the explanation

Gravitational attraction

The inward gravitational force bends the satellite's velocity into a circular path.

After trying it yourself, choose your next review. This is your self-assessment.

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Make it stick

How does equating gravity and centripetal force explain the speed of a circular orbit?

If you needed the solution, close it and solve the problem again from a blank page. A correct answer is stronger when you can explain the reason for each step.

Keep learning Physics

Course scope and assessment

One hundred and sixty-two original lessons cover all 12 published subject-content outcomes in Topic 1 (sections 1.1–1.4), all nine outcomes in Topic 2 (section 2.1), all 13 outcomes in Topic 3 (sections 3.1–3.3), all 13 outcomes in Topic 4 (sections 4.1–4.3), all 11 outcomes in Topic 5 (sections 5.1–5.2), all 10 outcomes in Topic 6 (sections 6.1–6.2), all 16 outcomes in Topic 7 (sections 7.1–7.5), all 12 outcomes in Topic 8 (sections 8.1–8.4), all 15 outcomes in Topic 9 (sections 9.1–9.3), all 16 outcomes in Topic 10 (sections 10.1–10.3), all 18 outcomes in Topic 11 (sections 11.1–11.2), all seven outcomes in Topic 12 (sections 12.1–12.2), all 12 outcomes in Topic 13 (sections 13.1–13.4), all eight outcomes in Topic 14 (sections 14.1–14.3), and all nine outcomes in Topic 15 (sections 15.1–15.3), plus all four outcomes in Topic 16 (sections 16.1–16.2), and all ten outcomes in Topic 17 (sections 17.1–17.3), plus all 12 outcomes in Topic 18 (sections 18.1–18.5), all nine outcomes in Topic 19 (sections 19.1–19.3), all 19 outcomes in Topic 20 (sections 20.1–20.5), and all eight outcomes in Topic 21 (sections 21.1–21.2), and all 17 outcomes in Topic 22 (sections 22.1–22.4), and all 13 outcomes in Topic 23 (sections 23.1–23.2), and all 16 outcomes in Topic 24 (sections 24.1–24.3), and all 11 outcomes in Topic 25 (sections 25.1–25.3), of the 2025–2027 syllabus. Each lesson has guided, independent and application practice with explained answers. All 25 syllabus topics now have mapped teaching and practice; the 2028–2030 changes outside Topics 23–25 still need reconciliation. Online study cannot demonstrate supervised Paper 3 laboratory competence. Paper 5 planning and analysis, full timed cumulative assessment and human subject-teacher review remain outstanding.

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