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Educora
BeginnerGrades 7–1022 min9 / 44

Gravity, weight and weightlessness

Learn universal gravitation, the force of gravity (F = m · g) and how it changes with height, the difference between mass and weight, weight in a lift and on a bridge, weightlessness and g-load — with DİM-style tasks.

Check yourself
In this lesson you will learn
  • Use the law of gravitation and the height dependence of g in ratio problems
  • Tell the force of gravity from weight, and mass from weight
  • Calculate weight in an accelerating lift and on a bridge
  • Explain weightlessness and g-load

Stand on bathroom scales in the lift of a tall building. When the lift starts going up the scales show more, and when it starts going down they show less — yet your mass has not changed. An astronaut on a space station is even “weightless”, although the Earth still pulls on them. In this lesson you will learn to tell the force of gravity from weight and to calculate when weight grows or shrinks.

Universal gravitation and the force of gravity

Newton found that every body in the Universe attracts every other body. The gravitational force is proportional to the product of the masses and inversely proportional to the square of the distance between their centres. The force that makes an apple fall also keeps the Moon in orbit. Planets and satellites are covered in the lesson «Circular motion and gravitation».

F = G · m₁ · m₂ / r²F = G · m₁ · m₂ / r²
where:
  • Fgravitational force, in N
  • m₁, m₂masses of the bodies, in kg
  • rdistance between the centres, in m
  • Ggravitational constant, 6.67 · 10⁻¹¹ N · m² / kg²: the pull between two 1 kg bodies 1 m apart

The force with which the Earth pulls bodies towards itself is the force of gravity. It acts on the body itself, points vertically down towards the Earth’s centre and is proportional to the mass. At the Earth’s surface g = G · M / R² ≈ 9.8 N/kg (10 N/kg in problems). Further from the Earth, g gets smaller.

F = m · g, gh = g₀ · R² / (R + h)²F = m · g, gh = g₀ · R² / (R + h)²
where:
  • mmass of the body, in kg
  • g₀free-fall acceleration at the Earth’s surface
  • ghfree-fall acceleration at height h
  • Rradius of the Earth (≈ 6400 km)

The force of gravity and how it depends on height.

The Earth creates a gravitational field around itself. The field strength at a point is the force on a 1 kg body placed there: g = F / m (N/kg). So g has two meanings: the field strength (N/kg) and the free-fall acceleration (m/s²) — the units are the same, because 1 N/kg = 1 m/s².

Example 1: on the Earth and on the Moon

Murad has a mass of 50 kg. Find the force of gravity on him on the Earth (g = 9.8 N/kg) and on the Moon (g = 1.6 N/kg). What is Murad’s mass on the Moon?

Show solution
On the Earth: F = 50 · 9.8 = 490 N. On the Moon: F = 50 · 1.6 = 80 N.
Mass is a property of the body itself and does not change: it is still 50 kg on the Moon.
Example 2: ratio problems

1) The distance between two bodies is tripled. How does the gravitational force change?
2) What is g at a height R above the Earth’s surface (R is the Earth’s radius; g₀ = 10 m/s²)?
3) At what height is the free-fall acceleration 9 times smaller than at the surface?

Show solution
1) F ~ 1/r² → it becomes 3² = 9 times smaller.
2) g = g₀ · R² / (2R)² = g₀ / 4 = 2.5 m/s².
3) (R + h)² / R² = 9 → R + h = 3R → h = 2R (≈ 12,800 km).

Weight and mass

Definition
Weight

The force (W) with which a body, pulled by the Earth, presses on its support or pulls on its hanger. Weight acts on the support, while the force of gravity acts on the body itself. By Newton’s third law the weight equals the normal force: W = N. At rest or in uniform motion W = mg. (Many English textbooks simply call mg the weight; here we use the stricter meaning that DİM uses.)

PropertyMassWeight
What is it?a measure of inertiaa force on the support
UnitkgN
Instrumentbalancespring balance
On the Moon or in a liftstays the samechanges

Weight in an accelerating lift

Two forces act on a body in a lift: mg (down) and the normal force N (up). If the acceleration points up, Newton’s second law gives N − mg = ma, so N = m(g + a). If it points down, N = m(g − a). The weight is W = N. The ratio of the weight to mg is called the g-load (overload) n.

W = m(g + a) — a up; W = m(g − a) — a down; n = W / (mg)W = m(g + a) — a up; W = m(g − a) — a down; n = W / (mg)
where:
  • amagnitude of the lift’s acceleration, in m/s²
  • ng-load: n > 1 — weight increased, n = 0 — weightlessness
Motion of the liftAccelerationWeight
speeds up going upupW > mg
moves uniformly or stands stilla = 0W = mg
brakes while going updownW < mg
speeds up going downdownW < mg
brakes while going downupW > mg
falls freelya = gW = 0
Example 3: scales in a lift

Aysel, whose mass is 50 kg, stands on scales in a lift. What do the scales show (in newtons) when the lift a) starts going up with an acceleration of 2 m/s², b) starts going down with an acceleration of 2 m/s², c) moves at constant speed? What is the g-load in case a)?

Show solution
a) W = 50 · (10 + 2) = 600 N. b) W = 50 · (10 − 2) = 400 N. c) W = mg = 500 N.
n = 600 / 500 = 1.2 — Aysel feels 1.2 times “heavier”.
Example 4 (multiple choice): a lift braking on its way down

A lift moving down brakes with a deceleration of 3 m/s² as it approaches a floor. Find the weight of a 70 kg person in the lift (g = 10 m/s²).
A) 490 N B) 700 N C) 910 N D) 210 N E) 1400 N

Show solution
The lift moves down but slows down → the acceleration points up.
W = m(g + a) = 70 · 13 = 910 N (C).
A (490 N) is the mistake of looking at the velocity and writing W = m(g − a).

A car on a convex or concave bridge

If a bridge is an arc of a circle, the car moves along a circle and its centripetal acceleration a = v² / R points to the centre (see «Circular motion and gravitation»). At the top of a convex bridge the centre is below — the acceleration points down and the weight drops. At the bottom of a concave bridge the centre is above — the weight grows.

W = m(g − v² / R) — convex; W = m(g + v² / R) — concaveW = m(g − v² / R) — convex; W = m(g + v² / R) — concave
where:
  • vspeed of the car, in m/s
  • Rradius of curvature of the bridge, in m

When v = √(g · R), W = 0 at the top of a convex bridge — weightlessness.

Example 5: convex and concave bridges

A 2 t car drives at 15 m/s over a bridge with a radius of curvature of 45 m. With what force does it press on the bridge a) at the top of a convex bridge, b) at the bottom of a concave bridge? c) At what speed would the car be weightless at the top of the convex bridge?

Show solution
a = v² / R = 225 / 45 = 5 m/s².
a) W = 2000 · (10 − 5) = 10 kN.
b) W = 2000 · (10 + 5) = 30 kN.
c) v = √(g · R) = √450 ≈ 21 m/s.

Weightlessness and g-load

When a body and its support move under gravity alone (a = g, down), the body does not press on the support: W = m(g − g) = 0. This is weightlessness. A jumping athlete in the air, a freely falling lift and a space station in orbit are all weightless: the station is constantly “falling” around the Earth. The force of gravity still acts! During a rocket launch or a tight aircraft turn, on the contrary, a g-load (n > 1) appears.

Example 6: an aircraft in a vertical loop

An aircraft flies a vertical loop of radius 500 m and passes its lowest point at 100 m/s. Find the force with which the 80 kg pilot presses on the seat and the g-load.

Show solution
a = v² / R = 10,000 / 500 = 20 m/s², directed to the centre, i.e. up.
W = m(g + a) = 80 · 30 = 2400 N; n = 2400 / 800 = 3 — the pilot feels three times “heavier”.
Example 7 (multiple choice): I–II–III statements

Which statements are true? I. In weightlessness the force of gravity on a body is zero. II. Weight acts on the support or the hanger. III. In a lift accelerating upwards a body’s weight is greater than mg.
A) only I B) only II C) II and III D) I and III E) I, II, III

Show solution
I is false: in weightlessness only the weight is zero, the force of gravity is still mg. II is true. III is true: W = m(g + a) > mg.
Answer: C.

Key points

  • F = G · m₁ · m₂ / r²; the force of gravity is F = mg, and g falls with height: gh = g₀R² / (R + h)².
  • Gravity acts on the body, weight acts on the support; at rest the weight equals mg.
  • In a lift the weight is m(g ± a): “+” for acceleration up, “−” for down; the direction of the velocity does not matter.
  • On a convex bridge the weight is m(g − v²/R); on a concave one, m(g + v²/R).
  • In weightlessness (a = g) the weight is zero, but gravity still acts.

Check yourself

12 questions. Every correct answer earns XP.

1 / 12
What happens in a state of weightlessness?