Physics·TPC

Banked Curves (Ideal Angle)

BINAS 35A3Tsokos Ch. 6.2

Overview

A banked road allows a vehicle to turn without friction. At the ideal banking angle θ for speed v: horizontal component of N provides centripetal force; vertical component balances weight. N cosθ = mg (vertical). N sinθ = mv²/r (centripetal). Dividing: tanθ = v²/(rg). At this angle, no friction needed. Above ideal speed: friction acts inward. Below ideal speed: friction acts outward. Exam tip: derive by resolving N into components — do NOT try to memorise; derive it every time.

Banked curves — how banking helps

On a flat road, friction provides centripetal force — if the road is icy (μ ≈ 0), cars cannot turn. Banked roads are tilted so the normal force N has a horizontal component pointing inward: N sin θ = mv²/r. The vertical component supports the weight: N cos θ = mg. Dividing: tan θ = v²/(rg). At this specific speed, no friction is needed. At other speeds, friction must provide the additional centripetal force.

mNN sin θ = mv²/rN cos θ = mgθ
Worked Examples
Common Mistakes
  • Using sin θ instead of tan θ in the formula tan θ = v²/(rg)
  • Forgetting that the formula is only valid for the 'ideal' frictionless speed