Angled Forces: Cones, Pendulums & Banking
Angled Forces: Cones, Pendulums & Banking
- The current flagship question: a ball on a string, in a cone, or a banking aircraft, where one tilted force does two jobs at once.
The two-line resolve
- Split the tilted force (tension, contact force or lift) into components. The mark scheme wants exactly two lines:
- Vertically: the vertical component balances the weight, so there is no vertical resultant: .
- Horizontally: the horizontal component is the resultant, pointing at the centre: (9702/42/F/M/25 Q1(b)).
- Divide the two equations and the force size cancels: , or .
Worked example
Exam version: a ball inside a smooth cone
A steel ball rolls in a horizontal circle of radius 0.15 m inside a frictionless cone whose wall makes 52° with the horizontal, so the contact force is tilted at 52° from the vertical direction of the resolve. Show that the speed is about 1.4 m s⁻¹, then find ω. (9702/42/F/M/25 Q1)
- Two lines: vertical component of contact force = weight; horizontal component = . Dividing: .
- .
- .
Answer
The follow-up one-marker: with the same surface angle the acceleration is fixed, so going faster needs a bigger radius ().
- The same resolve, different actors: a conical pendulum on a string (, radius = ) (9702/41/M/J/23 Q2); an aircraft banking (vertical part of lift balances weight, horizontal part turns the plane); a banked road (the normal contact force leans inward).
Common mistake
Check which line the angle is measured from. A cone wall at 52° to the horizontal and a string at 27° to the vertical put the sin and cos in different places. Draw the triangle before writing the two lines.