A.2.3—Free-body diagrams

Syllabus
First assessment 2025
Objective
Level
HL

Draw a Labelled Free-Body Diagram

Isolate one body

A free-body diagram shows only the chosen body and the external forces acting on it. Replace the body with a point or simple shape and choose useful axes.

Draw actual forces

Use arrows from the body, label each interaction and draw the direction physically. Typical labels include weight mgmg, normal force NN, tension TT, friction and drag.

Resolve only when needed

If a force is angled, resolve it into the chosen axes. Then apply Fx=max\sum F_x=ma_x and Fy=may\sum F_y=ma_y to the same body.

Common trap

Do not draw velocity, acceleration or a force exerted by the chosen body on its surroundings as forces acting on the chosen body.

A.2.3 Exam Analysis

Assessment in practice

2 marks
How it is assessed

The evidence asks for a labelled diagram of a ball supported by a tension, rewarding the correct force labels, directions and omission of non-forces.

Command terms

Draw

What earns marks

Choose the stated object, draw only external forces, label weight and tension/normal/contact forces, and orient them correctly. Resolve angled forces only after the free-body diagram is complete.

Watch for

Including velocity or acceleration as arrows, or drawing the reaction force on the supporting body instead of the force on the chosen ball.

Representative question

Question 1

[Maximum number: 2]

Draw a labelled free-body diagram of the forces on the ball.

Retrieve the A.2 Forces and Momentum Model

Build the force model

Choose the system, draw a labelled free-body diagram, classify the interactions and resolve components. Apply Newton’s laws with the correct boundary: contact forces, field forces, friction, tension, buoyancy and restoring forces each have their own direction and conditions.

Track momentum

Use ec p=m ec v, ec J=\Delta ec p and momentum conservation only after checking external impulse. Distinguish elastic and inelastic collisions, explosions and energy transfer.

Track circular motion

The inward resultant provides ac=v2/r=ω2ra_c=v^2/r=\omega^2r. It may come from tension, gravity, normal, friction or a field force. Angular and linear descriptions are linked by v=ωr=2πr/Tv=\omega r=2\pi r/T.

Final checks

Ask: Which body is the system? Which forces are external? Is mass constant? Is acceleration uniform or radial? Is kinetic energy conserved, transferred or increased?