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Newton's law of universal gravitation (SACE Stage 2 Physics)

Syllabus dot point

“Apply Newton's law of universal gravitation and the concept of gravitational field strength to interactions between masses.”

9 min read

Quick answer

Every pair of masses attracts with a force F=Gm1m2r2F = G\dfrac{m_1 m_2}{r^2}, where G=6.67×10−11 N m2kg−2G = 6.67\times10^{-11}\ \text{N m}^2\text{kg}^{-2} and rr is the centre-to-centre separation. The force is an inverse-square law. Gravitational field strength is the force per unit mass, g=GMr2g = G\dfrac{M}{r^2}, which equals the free-fall acceleration.

Jump to a section
  1. What this dot point is asking
  2. The law
  3. Gravitational field strength
  4. Why it matters
  5. How SACE assesses this
  6. Exam-style questions

What this dot point is asking

You need to apply Newton's law of universal gravitation to calculate the attractive force between two masses, understand its inverse-square dependence, and relate it to gravitational field strength.

Force between Earth and a satellite

A 500 kg satellite orbits at a height of 2000 km above Earth's surface

Earth's mass M=5.97×1024 kgM = 5.97\times10^{24}\ \text{kg} and radius =6.37×106 m= 6.37\times10^6\ \text{m}. Find the gravitational force on the satellite.

Orbital radius (centre to satellite):

r=6.37×106+2.00×106=8.37×106 m.r = 6.37\times10^6 + 2.00\times10^6 = 8.37\times10^6\ \text{m}.

Force:

F=GMmr2=6.67×10−11×(5.97×1024)(500)(8.37×106)2F = G\frac{Mm}{r^2} = 6.67\times10^{-11}\times\frac{(5.97\times10^{24})(500)}{(8.37\times10^6)^2}

F=6.67×10−11×2.99×10277.00×1013≈2.8×103 N.F = 6.67\times10^{-11}\times\frac{2.99\times10^{27}}{7.00\times10^{13}} \approx 2.8\times10^3\ \text{N}.

This force is the centripetal force that keeps the satellite in orbit.

The law

Newton's law of universal gravitation

F=Gm1m2r2F = G\frac{m_1 m_2}{r^2}

FF is the attractive force on each mass (N), m1m_1 and m2m_2 the masses (kg), rr the distance between their centres (m), and G=6.67×10−11 N m2kg−2G = 6.67\times10^{-11}\ \text{N m}^2\text{kg}^{-2} the universal gravitational constant.

Key features:

  • The force is always attractive and acts along the line joining the two centres.
  • It is mutual: by Newton's third law each mass pulls the other with the same magnitude, regardless of how different the masses are.
  • It follows an inverse-square law: doubling the separation reduces the force to a quarter; tripling it reduces it to a ninth.
  • It is directly proportional to each mass: doubling one mass doubles the force.

For spherical bodies such as planets, rr is measured from centre to centre, so for an object on Earth's surface rr is the radius of the Earth.

Gravitational field strength

A mass creates a gravitational field around it. The field strength gg at a point is the force per unit mass placed there.

Gravitational field strength

g=Fm=GMr2g = \frac{F}{m} = G\frac{M}{r^2}

gg has units N kg−1\text{N kg}^{-1}, numerically equal to the free-fall acceleration in m s−2\text{m s}^{-2}. MM is the mass producing the field. Field strength also obeys the inverse-square law, so it weakens with the square of the distance from the centre.

This is why g≈9.8 N kg−1g \approx 9.8\ \text{N kg}^{-1} at Earth's surface, and falls off as you move to higher altitude or orbit. At twice Earth's radius from the centre, gg has fallen to a quarter of its surface value.

Why it matters

This single law explains the fall of an apple and the orbit of the Moon: the same gravitational interaction governs both. Combined with the centripetal force requirement, it underpins satellite and planetary orbits (covered in the next dot point), and the field-strength idea connects the abstract force law to the everyday acceleration of free fall.

How SACE assesses this

SACE Stage 2 gravitation questions are almost always direct substitutions into F=Gm1m2r2F = \dfrac{Gm_1 m_2}{r^2}, usually with real astronomical bodies (a moon and its planet, or a probe and the Sun) and data given in scientific notation. The two recurring traps are squaring the separation correctly and keeping every quantity in SI units. A second common part asks you to explain the mutual, equal-and-opposite nature of the force using Newton's third law, where the symmetry of the formula in m1m_1 and m2m_2 is the key point. Quote the formula, substitute with units, square rr as a separate step, and state the answer to an appropriate number of significant figures.

Common errors
Using surface distance instead of centre-to-centre
For a body above a planet, rr is the planet's radius plus the height, measured from the planet's centre.
Forgetting the inverse square
It is r2r^2 in the denominator, not rr. A common error is to halve the force when the distance doubles, instead of quartering it.
Thinking the larger mass feels a larger force
The forces on the two masses are equal and opposite. The Earth pulls you with the same force you pull the Earth; you accelerate more only because your mass is far smaller.

Confusing gg as field strength with gg as acceleration. They are numerically equal and have equivalent units, but field strength (N kg−1\text{N kg}^{-1}) is the more general idea.

Exam-style questions

Questions in the style of SACE Board exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.

SACE 2023-style4 marks
Titan has a mass of 1.35×1023 kg1.35\times10^{23}\ \text{kg} and Saturn has a mass of 5.68×1026 kg5.68\times10^{26}\ \text{kg}. (a) Calculate the magnitude of the gravitational force between Titan and Saturn when their centres are separated by 1.24×109 m1.24\times10^9\ \text{m}. (b) Explain how the gravitational forces are consistent with Newton's third law of motion.
Show worked answer →

(a) Apply Newton's law of universal gravitation, F=Gm1m2r2F = \dfrac{Gm_1 m_2}{r^2}, with G=6.67×10−11 N m2kg−2G = 6.67\times10^{-11}\ \text{N m}^2\text{kg}^{-2}.

F=(6.67×10−11)(1.35×1023)(5.68×1026)(1.24×109)2=5.114×10391.538×1018=3.33×1021 N.F = \dfrac{(6.67\times10^{-11})(1.35\times10^{23})(5.68\times10^{26})}{(1.24\times10^9)^2} = \dfrac{5.114\times10^{39}}{1.538\times10^{18}} = 3.33\times10^{21}\ \text{N}.
(2 marks)

(b) Newton's third law states forces occur in equal and opposite pairs. Titan pulls on Saturn and Saturn pulls on Titan with the same magnitude in the opposite direction. The expression Gm1m2r2\dfrac{Gm_1 m_2}{r^2} is symmetric in the two masses, so each body feels the same magnitude force regardless of the mass difference. (2 marks)

SACE 2024-style2 marks
Tethys is a moon of Saturn with a mass of 6.17×1020 kg6.17\times10^{20}\ \text{kg}, orbiting Saturn (mass 5.65×1026 kg5.65\times10^{26}\ \text{kg}) at an orbital radius of 2.95×108 m2.95\times10^8\ \text{m}. Calculate the magnitude of the gravitational force between Tethys and Saturn.
Show worked answer →

Apply F=Gm1m2r2F = \dfrac{Gm_1 m_2}{r^2} with G=6.67×10−11 N m2kg−2G = 6.67\times10^{-11}\ \text{N m}^2\text{kg}^{-2}.

Numerator: (6.67×10−11)(6.17×1020)(5.65×1026)=2.325×1037(6.67\times10^{-11})(6.17\times10^{20})(5.65\times10^{26}) = 2.325\times10^{37}.
Denominator: (2.95×108)2=8.70×1016(2.95\times10^8)^2 = 8.70\times10^{16}.

F=2.325×10378.70×1016=2.67×1020 N.F = \dfrac{2.325\times10^{37}}{8.70\times10^{16}} = 2.67\times10^{20}\ \text{N}.

1 mark for correct substitution, 1 mark for the answer of about 2.67×1020 N2.67\times10^{20}\ \text{N}.

Practise this

Sources & how we know this

ExamExplained