Estimate the gravitational force between you (60 kg) and Earth. What about between you and the person next to you (1 m away)?
State and apply Newton's Law of Universal Gravitation. Calculate gravitational field strength and understand the inverse square 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
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:
where:
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 force is inversely proportional to the square of the distance:
$F \propto \dfrac{1}{r^2}$
This means:
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.
Calculate the gravitational force between two 70 kg people standing 1.0 m apart (centre to centre).
$M = 70 \text{ kg}$, $m = 70 \text{ kg}$, $r = 1.0 \text{ m}$, $G = 6.67 \times 10^{-11} \text{ N m}^2 \text{ kg}^{-2}$
$F$ (gravitational force between the two people)
Use Newton's Law: $F = \dfrac{GMm}{r^2}$
$F = \dfrac{(6.67 \times 10^{-11}) \times 70 \times 70}{(1.0)^2}$
$F = \dfrac{6.67 \times 10^{-11} \times 4900}{1.0}$
$F = 3.27 \times 10^{-7} \text{ N}$
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.
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:
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, $r = R_{\text{Earth}} = 6.37 \times 10^6 \text{ m}$:
$g = \dfrac{GM}{R^2} = \dfrac{(6.67 \times 10^{-11}) \times (5.97 \times 10^{24})}{(6.37 \times 10^6)^2} = 9.83 \text{ m/s}^2$
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.
For a point at altitude $h$ above a planet's surface, the field strength $g'$ can be found in two equivalent ways:
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.
Calculate the gravitational field strength at an altitude of 300 km above Earth's surface. Use $R_{\text{Earth}} = 6371 \text{ km}$, $g_{\text{surface}} = 9.8 \text{ m/s}^2$.
$R = 6371 \text{ km} = 6.371 \times 10^6 \text{ m}$, $h = 300 \text{ km} = 3.00 \times 10^5 \text{ m}$, $g = 9.8 \text{ m/s}^2$
$g'$ (gravitational field strength at altitude $h$)
Use the ratio method: $g' = g \times \left(\dfrac{R}{R + h}\right)^2$
Note: $r = R + h = 6371 + 300 = 6671 \text{ km}$
$g' = 9.8 \times \left(\dfrac{6371}{6671}\right)^2$
$g' = 9.8 \times (0.9550)^2$
$g' = 9.8 \times 0.9120$
$g' = 8.94 \text{ m/s}^2$
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."
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.
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 $1/r^2$.
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 $\dfrac{1}{(1/2)^2} = 4 \times$
When we plot gravitational force $F$ against distance $r$, we get a curve that decreases rapidly:
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.
The inverse square law applies to any phenomenon where a quantity radiates uniformly from a point source in three dimensions:
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)?
$F_{\text{surface}} = 600 \text{ N}$, $r_{\text{surface}} = R$, $r_{\text{new}} = 2R$
$F_{\text{new}}$ (gravitational force at $r = 2R$)
Use the inverse square law: $F \propto \dfrac{1}{r^2}$. Since $r$ doubles, $F$ becomes $\dfrac{1}{4}$.
Alternatively: $\dfrac{F_{\text{new}}}{F_{\text{surface}}} = \left(\dfrac{R}{2R}\right)^2 = \left(\dfrac{1}{2}\right)^2 = \dfrac{1}{4}$
$F_{\text{new}} = \dfrac{F_{\text{surface}}}{4} = \dfrac{600}{4}$
$F_{\text{new}} = 150 \text{ N}$
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 $g' = 9.8/4 = 2.45 \text{ m/s}^2$.
"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.
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%.
1 Calculate the gravitational force between two spheres of mass 1000 kg and 500 kg whose centres are 2 m apart.
2 Find the gravitational field strength at 1000 km above Earth's surface. Use $R_{\text{Earth}} = 6371 \text{ km}$ and $g_{\text{surface}} = 9.8 \text{ m/s}^2$.
3 If Earth shrank to half its current radius (keeping the same mass), what would the gravitational field strength at the new surface be?
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:
1. The gravitational constant $G$ is:
2. If the distance between two masses triples, the gravitational force becomes:
3. Gravitational field strength $g$ at a point is defined as:
4. The weight of an object at $2R$ from Earth's centre (where $R$ = Earth's radius) is:
5. Two identical spheres experience force $F$ when touching. If the distance between their centres doubles, the force becomes:
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 $3.84 \times 10^8 \text{ m}$.
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 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.
$F = \dfrac{GMm}{r^2}$
$F = \dfrac{(6.67 \times 10^{-11}) \times (5.97 \times 10^{24}) \times (7.35 \times 10^{22})}{(3.84 \times 10^8)^2}$
$F = \dfrac{2.93 \times 10^{37}}{1.47 \times 10^{17}}$
$F = 1.98 \times 10^{20} \text{ N}$ (1 mark for method, 1 mark for answer)
This enormous force keeps the Moon in orbit around Earth.
$g_{\text{Mars}} = \dfrac{GM}{R^2}$
$g_{\text{Mars}} = \dfrac{(6.67 \times 10^{-11}) \times (6.42 \times 10^{23})}{(3.40 \times 10^6)^2}$ (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).
$F = \dfrac{GMm}{r^2} = \dfrac{(6.67 \times 10^{-11}) \times 1 \times 2}{(0.5)^2}$ (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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