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UNIT SYLLABUS

A.2 Forces and momentum

SL/HL 10 hours
This is the heart of mechanics: Newton's three laws tell you how forces change motion, and momentum gives you the bookkeeping tool that survives even violent collisions. You will learn to draw free-body diagrams — the single most valuable habit in physics — and to recognise the standard cast of forces: weight, normal force, friction, tension, spring force, drag and buoyancy. Conservation of momentum then lets you analyse collisions and explosions without knowing anything about the complicated forces inside them, and circular motion shows that a force perpendicular to velocity changes direction, not speed.

Guiding Questions

  • ? How can the forces acting on a system be represented both visually and algebraically?
  • ? How can Newton's laws be modelled mathematically?
  • ? How can knowledge of forces and momentum predict the behaviour of interacting bodies?
θ W = mg Fₖ Fƒ (friction) Constant velocity ⇒ resultant force = 0 Along slope: Fƒ = mg sinθ • Perpendicular: Fₖ = mg cosθ
Free-body diagram of a block on a rough incline: weight resolved into components, with the normal force and friction balancing them at constant velocity.

What the IB expects you to master

  • State and apply Newton's three laws, treating forces as interactions between bodies (third-law pairs act on different bodies).
  • Draw and analyse free-body diagrams to find resultant forces in one and two dimensions.
  • Use the contact forces: normal force, friction (FfμsFNF_f \le \mu_s F_N static, Ff=μdFNF_f = \mu_d F_N dynamic), tension, Hooke's law (FH=kxF_H = -kx), viscous drag (Fd=6πηrvF_d = 6\pi\eta r v) and buoyancy (Fb=ρVgF_b = \rho V g).
  • Use the field forces: gravitational (Fg=mgF_g = mg), electric and magnetic.
  • Apply conservation of linear momentum (p=mvp = mv) to elastic and inelastic collisions and to explosions, including their energy accounting.
  • Relate impulse to change of momentum (J=FΔt=ΔpJ = F\Delta t = \Delta p) and use F=Δp/ΔtF = \Delta p / \Delta t when mass changes.
  • Analyse uniform circular motion: centripetal acceleration a=v2/r=ω2ra = v^2/r = \omega^2 r, the centripetal force that causes it, and angular velocity ω\omega with v=ωrv = \omega r.

1 Key Formulas

Newton's second law
F=ma=ΔpΔtF = ma = \frac{\Delta p}{\Delta t}
Static friction
FfμsFNF_{f} \le \mu_{s} F_{N}
Dynamic friction
Ff=μdFNF_{f} = \mu_{d} F_{N}
Hooke's law
FH=kxF_{H} = -kx
Viscous drag (Stokes)
Fd=6πηrvF_{d} = 6\pi\eta r v
Buoyancy
Fb=ρVgF_{b} = \rho V g
Linear momentum
p=mvp = mv
Impulse
J=FΔt=ΔpJ = F\Delta t = \Delta p
Angular velocity
ω=2πT=2πf\omega = \frac{2\pi}{T} = 2\pi f
Linear speed (circular)
v=ωrv = \omega r
Centripetal acceleration
a=v2r=ω2r=4π2rT2a = \frac{v^{2}}{r} = \omega^{2} r = \frac{4\pi^{2}r}{T^{2}}
Centripetal force
F=mv2r=mω2rF = \frac{mv^{2}}{r} = m\omega^{2} r

2 Exam Preparation & Topic Explanations

Free-body diagrams that earn marks

Examiners award marks for correctly drawn and labelled free-body diagrams before any algebra begins. Draw the body as a point or simple box, include only forces acting ON the body, give each arrow a conventional label (WW or mgmg, FNF_N, FfF_f, TT), and make lengths roughly reflect magnitudes.

Then translate the diagram into equations along sensible axes — parallel and perpendicular to a slope, or radial and tangential for circular motion.

Pro Exam Strategy
  • Never draw "centripetal force" as an extra arrow — it is the resultant of the real forces (tension, gravity, friction, normal force).

  • In collision questions, always define a positive direction first and keep signs consistent.

  • Elastic collision = kinetic energy conserved; momentum is conserved in every collision.

  • For vertical circles, analyse the top and bottom points — those are the exam favourites.

3 MCQ Practice

Q1. A book rests on a table. According to Newton's third law, the reaction to the weight of the book is:

  • The normal force from the table on the book
  • The gravitational pull of the book on the Earth
  • The normal force from the book on the table
  • The friction between book and table

Q2. A 0.16 kg0.16\ \text{kg} cricket ball arrives at 30 m s130\ \text{m s}^{-1} and is hit straight back at 40 m s140\ \text{m s}^{-1}. The bat and ball are in contact for 0.02 s0.02\ \text{s}. What is the average force on the ball?

  • 80 N80\ \text{N}
  • 240 N240\ \text{N}
  • 560 N560\ \text{N}
  • 1120 N1120\ \text{N}

Q3. A car travels at constant speed around a horizontal circular bend. Which statement is correct?

  • There is no resultant force since the speed is constant
  • The resultant force acts towards the centre of the circle
  • The resultant force acts outwards, away from the centre
  • The resultant force acts in the direction of motion

4 Short Answer Questions

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