A.2.7—Frictional force
- Syllabus
- First assessment 2025
- Objective
- —
- Level
- SL
Friction follows the contact
Friction acts parallel to the contact surface and opposes relative motion or the tendency of surfaces to move relative to each other.
Static friction adapts
Before slipping, static friction has whatever value is needed up to a maximum:
Ff≤μsN
It is not automatically equal to μsN; that value occurs at impending motion.
Dynamic friction during sliding
Once surfaces slide, the model gives
Ff=μdN
Use the normal force for the actual contact and combine friction with the other forces along the surface.
Common trap
Do not use the dynamic coefficient before motion begins, or assume static friction is always at its maximum.
[ 2 ]
Show that the minimum force needed to accelerate the box is about 4 N .
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=mec v, ec J=\Deltaec 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=ω2r. It may come from tension, gravity, normal, friction or a field force. Angular and linear descriptions are linked by v=ωr=2πr/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?