Section 1.6: Equilibrium and Stability
This section explores the conditions for equilibrium in rigid bodies and the concepts of stability, including stable, unstable, and neutral equilibrium.
Key Concepts:
- Equilibrium Conditions: \( \sum \vec{F} = 0 \) and \( \sum \tau = 0 \)
- Stable Equilibrium: Small displacement causes restoring force/torque back to equilibrium.
- Unstable Equilibrium: Small displacement increases deviation from equilibrium.
- Neutral Equilibrium: Small displacement does not change the potential energy.
- Center of Gravity (CG) and its role in stability.
Example 1
A uniform rod of length 2 m rests on a horizontal surface. Find the condition for it to remain in equilibrium when a 5 kg mass is placed at 0.5 m from one end.
Torque about pivot: \( \tau = m g x \)
For equilibrium: Sum of clockwise and counterclockwise torques = 0.
Example 2
A cone rests on a horizontal surface. Determine whether it is in stable, unstable, or neutral equilibrium.
Check CG: If CG rises when displaced → unstable; if lowers → stable; if remains → neutral.
Practice Problems
- A uniform ladder of length 5 m rests against a smooth wall and rough floor. Find the angle for equilibrium.
- A cylinder rests on a horizontal surface. Determine its type of equilibrium.
- A beam is supported at two points. Where should a 10 kg mass be placed for equilibrium?
- A uniform rod of length 3 m is balanced on a pivot at its center. Is it stable?
- Determine stability of a book resting on its edge vs flat.
- A triangular prism rests on a surface. Predict stability based on CG.
- Two rods intersect at a pivot. Find force required to maintain equilibrium with attached weights.
- Compute torque on a seesaw with different masses for equilibrium.
- A sphere rests on a plane. Determine if small tilt increases/decreases potential energy.
- A wheel with CG above axle is slightly tilted. Classify equilibrium type.