Car on a Banked Track Simulation

Fc is the net inward component of real forces, not an extra force.

Controls:

Mass (kg):
5002000
Radius (m):
50200
Bank Angle:
5°45°
Friction μ:
00.8
Speed (m/s):
560
N: 0 N
f: 0 N
Available Fnet inward: 0 N
Required mv²/r: 0 N
Max speed: 0 m/s
Home
Student:
Max speed:

Car on a Banked Track Physics Simulation

This interactive 3D physics simulation demonstrates circular motion on a banked track. Students can explore how the normal force, friction, weight, and inward net force determine the maximum speed of a car moving around a curve.

Centripetal Force Is Not a Separate Force

In circular motion, the centripetal force is the net inward force. It is not an additional force placed on the force diagram. For a car on a banked track, the real forces are weight, normal force, and friction.

Fnet inward = mv2/r

Maximum Speed on a Banked Track

For the maximum-speed case, the car tends to slide up the bank, so friction acts down the slope. The inward force is the sum of the inward components of the normal force and friction.

Fnet inward = N sinθ + f cosθ

Using vertical equilibrium and f = μN:

N cosθ − f sinθ = mg

What Students Learn

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