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Year 12 Specialist (Unit 3 & 4) Modelling motion

Force

20 practice questions 0 video lessons Theory + worked examples

Study force for Year 12 Specialist Mathematics in Queensland (QCAA). A force is a vector measured in newtons, so several forces on a body combine by vector addition into a single resultant that governs how the body moves.

You will learn to work with momentum, the resultant of concurrent forces, weight and the normal reaction, and to apply Newton’s laws — the foundation for modelling motion under forces later in the course.

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Theory

Force in Year 12 Specialist Mathematics (QCAA, Queensland) treats a force as a vector measured in newtons. This page covers momentum \(p=mv\), the resultant of concurrent forces, weight \(W=mg\), the normal reaction and applied force, Newton’s second law \(F=ma\), and Newton’s third law of action and reaction. Take \(g=9.8\) m/s\(^2\).

A force is a push or pull measured in newtons (N). Because it has a magnitude and a direction, a force is a vector, written in component form as \(\mathbf{F}=F_x\mathbf{i}+F_y\mathbf{j}\). Several forces acting at the same point are called concurrent forces.

The momentum of a body of mass \(m\) moving with velocity \(v\) is \(p=mv\) (units kg\(\,\)m/s). Along a line, take one direction as positive so that a velocity in the opposite direction is negative. The impulse delivered by a force equals the change in momentum, \(\Delta p=m(v_2-v_1)\).

The resultant force is the vector sum of all forces acting on a body, \(\mathbf{R}=\sum\mathbf{F}\). For two perpendicular forces the magnitude follows from Pythagoras, \(|\mathbf{R}|=\sqrt{F_x^{\,2}+F_y^{\,2}}\). A body is in equilibrium exactly when the resultant is the zero vector, \(\sum\mathbf{F}=\mathbf{0}\); otherwise it accelerates.

The weight of a body is the force of gravity on it, \(W=mg\), acting vertically down. The normal reaction \(N\) is the support force a surface pushes back with, perpendicular to the surface. Newton’s second law links the resultant force to acceleration, \(\mathbf{F}=m\mathbf{a}\), while Newton’s third law says every action has an equal and opposite reaction that acts on the other body.

Free-body diagram of a particle A small block has three forces drawn from its centre: the normal reaction N points straight up, the weight W equals m g points straight down, and an applied force F points to the right. The upward and downward forces are vertical while the applied force is horizontal. m N W = mg F
Free-body diagram: the weight \(\mathbf{W}=m\mathbf{g}\) acts down, the normal reaction \(\mathbf{N}\) acts up, and an applied force \(\mathbf{F}\) acts horizontally.
Resultant of two perpendicular forces From a point O, a 6 newton force points east and an 8 newton force points north. The dashed resultant is the diagonal of the rectangle they form, running from O to the opposite corner, with magnitude 10 newtons. O 6 N 8 N R = 10 N
The resultant of \(6\) N east and \(8\) N north is the diagonal of the rectangle, \(|\mathbf{R}|=\sqrt{6^2+8^2}=10\) N.

Momentum of a body, and the impulse as its change in momentum:

\[ p=mv,\qquad \Delta p=m(v_2-v_1) \]
p=mv

The resultant of concurrent forces, and its magnitude when the components are perpendicular:

\[ \mathbf{R}=\sum\mathbf{F},\qquad |\mathbf{R}|=\sqrt{F_x^{\,2}+F_y^{\,2}} \]
|R|=Fx2+Fy2

Weight, and Newton’s second law relating the resultant force to acceleration:

\[ W=mg,\qquad \mathbf{F}=m\mathbf{a} \]
F=ma
Equilibrium or not. If \(\sum\mathbf{F}=\mathbf{0}\) the body stays at rest or moves at constant velocity; if the resultant is non-zero, the body accelerates in the direction of \(\mathbf{R}\) with \(a=\dfrac{|\mathbf{R}|}{m}\). Take \(g=9.8\) m/s\(^2\).

Working with forces

  1. Identify every force on the body — weight \(W=mg\) down, the normal reaction \(N\), any tension or applied force — and draw a free-body diagram.
  2. Add the forces as vectors to get the resultant \(\mathbf{R}=\sum\mathbf{F}\); for perpendicular forces use \(|\mathbf{R}|=\sqrt{F_x^{\,2}+F_y^{\,2}}\).
  3. Apply the law you need: \(p=mv\) for momentum, \(\Delta p=m(v_2-v_1)\) for impulse, or \(\mathbf{F}=m\mathbf{a}\) to link the resultant to the acceleration.
  4. Check equilibrium: a zero resultant means no acceleration; a non-zero resultant gives acceleration \(a=\dfrac{|\mathbf{R}|}{m}\) in the direction of \(\mathbf{R}\).
Example 1 — Momentum \(p=mv\)
A truck of mass \(2000\) kg travels in a straight line at \(8\) m/s. Find the magnitude of its momentum.
Solution

Momentum is mass times velocity:

\(p\)\(=\)\(mv\)
\(=\)\(2000 \times 8\)
\(=\)\(16\,000\)

The momentum is \(16\,000\) kg m/s.

Example 2 — Resultant of perpendicular forces
Two concurrent forces act at right angles: \(5\) N due east and \(12\) N due north. Find the resultant force and its magnitude.
Solution

Add the forces as vectors (east is \(\mathbf{i}\), north is \(\mathbf{j}\)):

\(\mathbf{R}\)\(=\)\(5\mathbf{i}+12\mathbf{j}\)

Perpendicular components combine by Pythagoras:

\(|\mathbf{R}|\)\(=\)\(\sqrt{5^2+12^2}\)
\(=\)\(\sqrt{25+144}\)
\(=\)\(\sqrt{169}\)
\(=\)\(13\)

The resultant is \(5\mathbf{i}+12\mathbf{j}\) N, of magnitude \(13\) N.

Resultant of two perpendicular forces From a point O, a 6 newton force points east and an 8 newton force points north. The dashed resultant is the diagonal of the rectangle they form, running from O to the opposite corner, with magnitude 10 newtons. O 6 N 8 N R = 10 N
Example 3 — Weight and Newton’s second law
A crate of mass \(6\) kg rests on the ground. Take \(g=9.8\) m/s\(^2\). (i) Find its weight. (ii) A single horizontal resultant force of \(18\) N then acts on it. Find its acceleration.
Solution

(i) Weight is the force of gravity, \(W=mg\):

\(W\)\(=\)\(mg\)
\(=\)\(6 \times 9.8\)
\(=\)\(58.8\)

(ii) Rearrange \(F=ma\) to make the acceleration the subject:

\(a\)\(=\)\(\dfrac{F}{m}\)
\(=\)\(\dfrac{18}{6}\)
\(=\)\(3\)

(i) The weight is \(58.8\) N. \;\; (ii) The acceleration is \(3\) m/s\(^2\).

Example 4 — Impulse (change in momentum)
A \(0.4\) kg ball travelling at \(5\) m/s strikes a wall and rebounds at \(3\) m/s in the opposite direction. Find the magnitude of the change in its momentum.
Solution

Change in momentum \(\Delta p=m(v_2-v_1)\); take the initial direction positive, so the rebound velocity is negative:

\(\Delta p\)\(=\)\(0.4\,(-3-5)\)
\(=\)\(0.4 \times (-8)\)
\(=\)\(-3.2\)
\(|\Delta p|\)\(=\)\(3.2\)

The change in momentum has magnitude \(3.2\) kg m/s.

Common pitfalls

Adding force magnitudes directly. Perpendicular forces of \(6\) N and \(8\) N give a resultant of \(\sqrt{6^2+8^2}=10\) N, not \(6+8=14\) N. Only forces along the same line add as numbers.
Forgetting the sign of a reversed velocity. When a ball rebounds, its velocity changes direction, so in \(\Delta p=m(v_2-v_1)\) the two velocities have opposite signs — the speeds add inside the bracket.
Confusing weight with mass. Mass is in kilograms; weight is a force, \(W=mg\), in newtons. A \(5\) kg mass has weight \(5\times9.8=49\) N.
Pairing the wrong forces as action and reaction. A Newton’s third-law pair is equal and opposite but acts on two different bodies. The weight and the normal reaction on one block are not a pair — they act on the same body.

Frequently asked questions

What is the formula for momentum?

Momentum is \(p=mv\), the mass times the velocity, measured in kilogram metres per second. Along a line, choose a positive direction so a velocity the other way counts as negative.

How do you find the resultant of two perpendicular forces?

Add them as vectors, then take the magnitude with Pythagoras: \(|\mathbf{R}|=\sqrt{F_x^{\,2}+F_y^{\,2}}\). For \(6\) N and \(8\) N at right angles this is \(\sqrt{36+64}=10\) N.

What is the difference between mass and weight?

Mass is the amount of matter in kilograms; weight is the gravitational force on that mass, \(W=mg\), in newtons. With \(g=9.8\) m/s\(^2\), a \(5\) kg mass weighs \(49\) N.

What does Newton’s third law say?

Every action has an equal and opposite reaction, and the two forces act on different bodies. If the Earth pulls a book down, the book pulls the Earth up with an equal and opposite force.

How is impulse related to momentum?

The impulse of a force equals the change in momentum it produces, \(\Delta p=m(v_2-v_1)\). For a rebound, the initial and final velocities have opposite signs.

When is a body in equilibrium?

A body is in equilibrium when the resultant force is the zero vector, \(\sum\mathbf{F}=\mathbf{0}\); it then stays at rest or moves at constant velocity. A non-zero resultant produces acceleration \(a=\dfrac{|\mathbf{R}|}{m}\).