Car on a Banked Track Simulation: Minimum Speed

Minimum-speed case: friction points up the slope. Fc is the Available inward 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 inward force: 0 N
Required mv²/r: 0 N
Min speed: 0 m/s
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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 Available 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

Minimum Speed on a Banked Track

For the minimum-speed case, the car tends to slide down the bank, so friction acts up the slope. The inward net force is the inward component of the normal force minus the outward component of friction.

Fnet inward = N sinθ − f cosθ
N cosθ + f sinθ = mg
Fnet inward = mv2/r

Using vertical equilibrium and f = μN:

N cosθ + f sinθ = mg

What Students Learn

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