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Learning Intention 1

State Newton's Law of Universal Gravitation

  • Understand that every mass attracts every other mass
  • State the formula and identify each quantity with correct units
Learning Intention 2

Calculate Gravitational Force and Field Strength

  • Apply $F = \dfrac{GMm}{r^2}$ to solve force problems
  • Calculate $g$ at any distance from a planet's centre
Learning Intention 3

Apply the Inverse Square Law

  • Explain how force varies with distance ($F \propto 1/r^2$)
  • Predict force changes when separation changes
Think First — Estimate

Estimate the gravitational force between you (60 kg) and Earth. What about between you and the person next to you (1 m away)?

Year 12 Physics Module 5: Advanced Mechanics 45 min Lesson 10 of 18 IQ3: Gravitational Fields

Newton's Law of Universal Gravitation

State and apply Newton's Law of Universal Gravitation. Calculate gravitational field strength and understand the inverse square law.

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1

Newton's Law

Every mass attracts every other mass with a force proportional to the product of their masses and inversely proportional to the square of their separation

Universal Gravitation

Universal Gravitation

Gravitation Detailed

Gravitation Detailed

Newton's Law of Universal Gravitation states that every particle of matter in the universe attracts every other particle with a force that is directly proportional to the product of their masses and inversely proportional to the square of the distance between their centres:

Σ

Newton's Law of Universal Gravitation

$F = \dfrac{GMm}{r^2}$ gravitational force between two masses (N)
$G = 6.67 \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$ universal gravitational constant

where:

  • $F$ = gravitational force (N) — always attractive
  • $G$ = universal gravitational constant = $6.67 \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$
  • $M$, $m$ = masses of the two objects (kg)
  • $r$ = centre-to-centre distance between the masses (m)

The force acts along the line joining the centres of the two masses. It is a mutual force — if mass $M$ exerts a force on mass $m$, then mass $m$ exerts an equal and opposite force on mass $M$ (Newton's third law).

The Inverse Square Relationship

The force is inversely proportional to the square of the distance:

$F \propto \dfrac{1}{r^2}$

This means:

  • If $r$ doubles, $F$ becomes $\dfrac{1}{4}$ (one-quarter)
  • If $r$ triples, $F$ becomes $\dfrac{1}{9}$ (one-ninth)
  • If $r$ is halved, $F$ becomes $4$ times larger
Key Insight

The inverse square law means gravitational force drops rapidly with distance. At twice the distance, the force is not half — it is one-quarter. At ten times the distance, the force is one-hundredth. This rapid fall-off explains why we only notice gravitational attraction from very large masses (planets, stars) and not from everyday objects.

Worked Example — Force Between Two People

Calculate the gravitational force between two 70 kg people standing 1.0 m apart (centre to centre).

GIVEN

$M = 70 \text{ kg}$, $m = 70 \text{ kg}$, $r = 1.0 \text{ m}$, $G = 6.67 \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$

FIND

$F$ (gravitational force between the two people)

METHOD

Use Newton's Law: $F = \dfrac{GMm}{r^2}$

ANS

$F = \dfrac{(6.67 \times 10^{-11}) \times 70 \times 70}{(1.0)^2}$

$F = \dfrac{6.67 \times 10^{-11} \times 4900}{1.0}$

$F = 3.27 \times 10^{-7} \text{ N}$

This force is negligible — about the weight of a single bacterium. It is far too small to feel, which is why we do not notice gravitational attraction between everyday objects.

2

Gravitational Field Strength

The gravitational force per unit mass at a point in space

The gravitational field strength $g$ at a point is defined as the gravitational force per unit mass experienced by a small test mass placed at that point:

Σ

Gravitational Field Strength

$g = \dfrac{F}{m}$ field strength = force per unit mass (N/kg or m/s$^2$)
$g = \dfrac{GM}{r^2}$ field strength at distance $r$ from a mass $M$

where $r$ is the centre-to-centre distance from the centre of the massive object (e.g. planet) to the point where the field strength is being calculated. For a point at height $h$ above a planet's surface:

$r = R + h$

where $R$ is the radius of the planet and $h$ is the altitude above the surface.

At Earth's Surface

At Earth's surface, $r = R_{\text{Earth}} = 6.37 \times 10^6 \text{ m}$:

$g = \dfrac{GM}{R^2} = \dfrac{(6.67 \times 10^{-11}) \times (5.97 \times 10^{24})}{(6.37 \times 10^6)^2} = 9.83 \text{ m/s}^2$

This value ($9.83 \text{ m/s}^2$) is close to the commonly quoted $9.8 \text{ m/s}^2$. The small difference arises from Earth's rotation and the fact that Earth is not a perfect sphere.

At Height $h$ Above the Surface

For a point at altitude $h$ above a planet's surface, the field strength $g'$ can be found in two equivalent ways:

Field Strength at Altitude

$g' = \dfrac{GM}{(R + h)^2}$ direct calculation using $r = R + h$
$g' = g \times \left(\dfrac{R}{R + h}\right)^2$ ratio method using surface value $g$
Important

Always use $r = R + h$ (centre-to-centre distance) in gravitational calculations. A common HSC error is to use the altitude $h$ directly instead of the distance from the centre. The gravitational force depends on distance from the centre of the attracting mass, not from its surface.

Worked Example — Field Strength at 300 km Altitude

Calculate the gravitational field strength at an altitude of 300 km above Earth's surface. Use $R_{\text{Earth}} = 6371 \text{ km}$, $g_{\text{surface}} = 9.8 \text{ m/s}^2$.

GIVEN

$R = 6371 \text{ km} = 6.371 \times 10^6 \text{ m}$, $h = 300 \text{ km} = 3.00 \times 10^5 \text{ m}$, $g = 9.8 \text{ m/s}^2$

FIND

$g'$ (gravitational field strength at altitude $h$)

METHOD

Use the ratio method: $g' = g \times \left(\dfrac{R}{R + h}\right)^2$

Note: $r = R + h = 6371 + 300 = 6671 \text{ km}$

ANS

$g' = 9.8 \times \left(\dfrac{6371}{6671}\right)^2$

$g' = 9.8 \times (0.9550)^2$

$g' = 9.8 \times 0.9120$

$g' = 8.94 \text{ m/s}^2$

Even at the altitude of the International Space Station (~400 km), gravitational field strength is still about 88% of its surface value. Astronauts are in free fall, not "zero gravity."

3

The Inverse Square Law

How gravitational force decreases with distance

The inverse square law is one of the most important patterns in physics. If a quantity spreads out uniformly in three-dimensional space from a point source, its intensity falls off as the inverse square of the distance.

Visualising the Inverse Square Law

Imagine gravitational force spreading out uniformly over the surface of an expanding sphere centred on the source mass. The surface area of a sphere is $4\pi r^2$, so as the sphere expands, the same total force is spread over an area that increases as $r^2$. The force per unit area therefore decreases as $1/r^2$.

Inverse Square Law — Distance vs Force

If distance becomes $3 \times$, force becomes $\dfrac{1}{3^2} = \dfrac{1}{9}$

If distance becomes $4 \times$, force becomes $\dfrac{1}{4^2} = \dfrac{1}{16}$

If distance becomes $\tfrac{1}{2} \times$, force becomes $\dfrac{1}{(1/2)^2} = 4 \times$

Graphical Representation

When we plot gravitational force $F$ against distance $r$, we get a curve that decreases rapidly:

  • Graph of $F$ vs $r$: a hyperbolic curve that approaches zero asymptotically
  • Graph of $F$ vs $\dfrac{1}{r^2}$: a straight line through the origin with gradient $GMm$

The linear relationship between $F$ and $1/r^2$ is powerful because it allows us to verify the inverse square law experimentally — plotting measured force against $1/r^2$ should yield a straight line.

Other Inverse Square Laws in Physics

The inverse square law applies to any phenomenon where a quantity radiates uniformly from a point source in three dimensions:

  • Gravitational force: $F = \dfrac{GMm}{r^2}$
  • Electrostatic force (Coulomb's law): $F = \dfrac{kq_1q_2}{r^2}$
  • Light intensity: $I = \dfrac{P}{4\pi r^2}$ where $P$ is the power of the source

Worked Example — Weight at Distance 2R from Earth's Centre

A 60 kg astronaut weighs 600 N at Earth's surface. What would they weigh at a distance of $2R_{\text{Earth}}$ from Earth's centre (i.e. at altitude $R_{\text{Earth}}$ above the surface)?

GIVEN

$F_{\text{surface}} = 600 \text{ N}$, $r_{\text{surface}} = R$, $r_{\text{new}} = 2R$

FIND

$F_{\text{new}}$ (gravitational force at $r = 2R$)

METHOD

Use the inverse square law: $F \propto \dfrac{1}{r^2}$. Since $r$ doubles, $F$ becomes $\dfrac{1}{4}$.

Alternatively: $\dfrac{F_{\text{new}}}{F_{\text{surface}}} = \left(\dfrac{R}{2R}\right)^2 = \left(\dfrac{1}{2}\right)^2 = \dfrac{1}{4}$

ANS

$F_{\text{new}} = \dfrac{F_{\text{surface}}}{4} = \dfrac{600}{4}$

$F_{\text{new}} = 150 \text{ N}$

At one Earth radius above the surface, the astronaut's weight is only one-quarter of their surface weight. Note that $g$ at this altitude would be $g' = 9.8/4 = 2.45 \text{ m/s}^2$.

Essential Formulae — Universal Gravitation

$F = \dfrac{GMm}{r^2}$ Newton's Law of Universal Gravitation (N)
$G = 6.67 \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$ universal gravitational constant
$g = \dfrac{GM}{r^2} = \dfrac{F}{m}$ gravitational field strength (N/kg or m/s$^2$)
$g' = g \times \left(\dfrac{R}{R + h}\right)^2$ field strength at altitude $h$ above a planet's surface
$F \propto \dfrac{1}{r^2}$ inverse square law — force varies as $1/r^2$
$r = R + h$ centre-to-centre distance (always use this!)

Common Misconceptions

"Gravity is a property of Earth only" — No. Every mass attracts every other mass. The Earth-Moon system, the Sun and its planets, and even you and your pen all exert gravitational forces on each other. The force is just too small to notice for everyday objects.

"There's no gravity in space" — No. Gravity extends to infinity — there is no cutoff distance. At the altitude of the ISS (~400 km), gravitational field strength is still about 88% of its surface value. Astronauts are in free fall (constantly falling toward Earth while moving forward so fast that they miss it), not in "zero gravity." The correct term is microgravity.

"$g$ is constant everywhere" — No. $g$ varies with altitude (decreases with height), latitude (Earth's rotation and equatorial bulge mean $g$ is slightly less at the equator), and local geology (density variations in Earth's crust). The standard value $g = 9.8 \text{ m/s}^2$ is an average at sea level at mid-latitudes.

Real World: The Cavendish Experiment

Weighing the Earth (1797–1798)

In 1797–1798, British scientist Henry Cavendish performed one of the most elegant experiments in the history of physics. Using a torsion balance — a thin wire suspended with small lead spheres that could twist in response to tiny forces — Cavendish measured the gravitational attraction between laboratory-scale masses.

Two small spheres (about 2 inches in diameter) were attached to the ends of a rod suspended by a thin wire. Two large spheres (about 12 inches in diameter) were placed near the small spheres. The gravitational attraction between the large and small masses caused the wire to twist by a measurable amount. By measuring this tiny twist, Cavendish calculated the gravitational constant $G$.

The forces involved were incredibly small — around $10^{-7}$ N — comparable to the gravitational force between two people standing 1 m apart. Yet Cavendish measured them with remarkable precision.

This experiment became known as "weighing the Earth" because once $G$ is known, Earth's mass can be calculated from the known value of $g$:

$g = \dfrac{GM}{R^2} \implies M = \dfrac{gR^2}{G} = \dfrac{9.8 \times (6.37 \times 10^6)^2}{6.67 \times 10^{-11}} = 5.97 \times 10^{24} \text{ kg}$

The modern CODATA 2018 value is: $G = 6.67430(15) \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$, consistent with Cavendish's original measurement to within about 1%.

Activity

Gravitational Force Between Spheres

apply Newton's Law of Universal Gravitation

1 Calculate the gravitational force between two spheres of mass 1000 kg and 500 kg whose centres are 2 m apart.

Activity

Field Strength at Altitude

calculate gravitational field strength above Earth's surface

2 Find the gravitational field strength at 1000 km above Earth's surface. Use $R_{\text{Earth}} = 6371 \text{ km}$ and $g_{\text{surface}} = 9.8 \text{ m/s}^2$.

Activity

Shrunken Earth

apply the inverse square law to a hypothetical scenario

3 If Earth shrank to half its current radius (keeping the same mass), what would the gravitational field strength at the new surface be?

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Key Definitions

  • Newton's Law of Universal Gravitation: every mass attracts every other mass with $F = \dfrac{GMm}{r^2}$
  • Universal gravitational constant: $G = 6.67 \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$
  • Gravitational field strength: $g = \dfrac{F}{m} = \dfrac{GM}{r^2}$ (N/kg or m/s$^2$)
  • Inverse square law: $F \propto \dfrac{1}{r^2}$ — force decreases as the square of distance increases

Key Equations

  • $F = \dfrac{GMm}{r^2}$ — gravitational force (N)
  • $g = \dfrac{GM}{r^2}$ — field strength at distance $r$ from mass $M$
  • $g' = g \times \left(\dfrac{R}{R + h}\right)^2$ — field at altitude $h$
  • $r = R + h$ — always use centre-to-centre distance

Inverse Square Law Summary

  • $r \times 2 \implies F \div 4$
  • $r \times 3 \implies F \div 9$
  • $r \times 10 \implies F \div 100$
  • $r \div 2 \implies F \times 4$

Important Principles

  • Gravitational force is always attractive
  • Force acts along the line joining centres of mass
  • $r$ is centre-to-centre distance, not surface-to-surface
  • Gravity extends to infinity — there is no cutoff
  • Astronauts in orbit are in free fall, not "zero gravity"
  • Cavendish (1798) first measured $G$ using a torsion balance

Revisit Your Estimate

You estimated the gravitational force between you and Earth, and between you and the person next to you. Here are the answers:

You and Earth: $F = \dfrac{GMm}{R^2} = mg \approx 60 \times 9.8 = 588 \text{ N}$ (about 600 N, or roughly your weight).

You and a person 1 m away: $F = \dfrac{(6.67 \times 10^{-11}) \times 60 \times 60}{1^2} \approx 2.4 \times 10^{-7} \text{ N}$ — utterly negligible, about the weight of a bacterium.

This enormous difference shows why we feel Earth's gravity but not each other's.

Has your understanding changed? Write a revised explanation:

Interactive: Gravitation Explorer Interactive
Key Terms
Newton's Law of Universal Gravitation Every mass attracts every other mass: $F = \dfrac{GMm}{r^2}$
Universal gravitational constant ($G$) $6.67 \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$; measured by Cavendish in 1798
Gravitational field strength ($g$) Force per unit mass at a point: $g = \dfrac{F}{m} = \dfrac{GM}{r^2}$
Inverse square law A quantity that decreases as the square of distance increases: $F \propto \dfrac{1}{r^2}$
Centre-to-centre distance ($r$) The distance between the centres of two masses: $r = R + h$
Free fall Motion under gravity alone; astronauts in orbit are in free fall, not "zero gravity"

1. The gravitational constant $G$ is:

A $6.67 \times 10^{11} \text{ N m}^2 \text{ kg}^{-2}$
B $6.67 \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$
C $9.8 \text{ m/s}^2$
D $9.8 \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$

2. If the distance between two masses triples, the gravitational force becomes:

A $\dfrac{1}{3}$ of the original
B $\dfrac{1}{9}$ of the original
C $3 \times$ the original
D $9 \times$ the original

3. Gravitational field strength $g$ at a point is defined as:

A Force per unit mass
B Force per unit distance
C Energy per unit mass
D Mass per unit force

4. The weight of an object at $2R$ from Earth's centre (where $R$ = Earth's radius) is:

A The same as at the surface
B Half the surface weight
C Quarter the surface weight
D Double the surface weight

5. Two identical spheres experience force $F$ when touching. If the distance between their centres doubles, the force becomes:

A $\dfrac{F}{2}$
B $\dfrac{F}{4}$
C $2F$
D $4F$
Apply Band 4 2 marks

Calculate the gravitational force between Earth ($M = 5.97 \times 10^{24} \text{ kg}$) and the Moon ($m = 7.35 \times 10^{22} \text{ kg}$). The average distance between their centres is $3.84 \times 10^8 \text{ m}$.

Apply Band 5 3 marks

Calculate the gravitational field strength at the surface of Mars ($M = 6.42 \times 10^{23} \text{ kg}$, $R = 3.40 \times 10^6 \text{ m}$). Compare your answer with Earth's surface gravity ($g = 9.8 \text{ m/s}^2$).

Evaluate Band 6 4 marks

Evaluate the statement: "The gravitational force between two everyday objects is too small to measure." Use calculations for a 1 kg and 2 kg mass separated by 0.5 m, and discuss the significance of the Cavendish experiment.

Model Answers

Question 1 (2 marks)

$F = \dfrac{GMm}{r^2}$

$F = \dfrac{(6.67 \times 10^{-11}) \times (5.97 \times 10^{24}) \times (7.35 \times 10^{22})}{(3.84 \times 10^8)^2}$

$F = \dfrac{2.93 \times 10^{37}}{1.47 \times 10^{17}}$

$F = 1.98 \times 10^{20} \text{ N}$ (1 mark for method, 1 mark for answer)

This enormous force keeps the Moon in orbit around Earth.

Question 2 (3 marks)

$g_{\text{Mars}} = \dfrac{GM}{R^2}$

$g_{\text{Mars}} = \dfrac{(6.67 \times 10^{-11}) \times (6.42 \times 10^{23})}{(3.40 \times 10^6)^2}$ (1 mark)

$g_{\text{Mars}} = \dfrac{4.28 \times 10^{13}}{1.16 \times 10^{13}}$

$g_{\text{Mars}} = 3.71 \text{ m/s}^2$ (1 mark)

Compared with Earth: $\dfrac{g_{\text{Mars}}}{g_{\text{Earth}}} = \dfrac{3.71}{9.8} = 0.378$

Mars gravity is approximately 38% of Earth's (or 0.378$g$) (1 mark for comparison).

Question 3 (4 marks)

$F = \dfrac{GMm}{r^2} = \dfrac{(6.67 \times 10^{-11}) \times 1 \times 2}{(0.5)^2}$ (1 mark for correct substitution)

$F = \dfrac{1.334 \times 10^{-10}}{0.25} = 5.34 \times 10^{-10} \text{ N}$ (1 mark for answer)

This force is extremely small — roughly equivalent to the weight of a single bacterium. On its own, this calculation suggests the statement could be true for everyday equipment (1 mark for analysis).

However, the Cavendish experiment (1798) demonstrated that forces of comparable magnitude ($\sim 10^{-7}$ N) can indeed be measured using a sensitive torsion balance. Cavendish measured the gravitational attraction between lead spheres in a laboratory setting, allowing him to calculate $G$ and subsequently "weigh the Earth." Modern experiments measure $G$ to parts per million. The statement was false in 1798 and is even more false today (1 mark for discussion of Cavendish and evaluation).

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