IP Physics Notes (Upper Secondary, Year 3-4): 4) Turning Forces
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Quick recap -- A turning effect appears when a force acts with an offset from a pivot. Balance comes from matching clockwise and anticlockwise moments while keeping the net force zero.
Moment of a Force
- The moment (torque) of a force measures its turning effect about a pivot: \( \tau = F d_\perp \), where \( d_\perp \) is the perpendicular distance from the pivot to the force's line of action.
- SI unit: \( \pu{N.m} \). It is a vector quantity whose sense is clockwise or anticlockwise around the pivot.
- Increase moment by raising the force magnitude, pushing further from the pivot, or pushing perpendicular to the lever arm. Oblique pushes need resolving into the perpendicular component first.
- Three classic lever classes:
- Class 1 (pivot between effort and load, e.g., seesaw) can magnify force or distance.
- Class 2 (load between pivot and effort, e.g., wheelbarrow) always multiplies effort.
- Class 3 (effort between pivot and load, e.g., tweezers) trades force multiplication for larger movement.
Principle of Moments
- For a body in rotational equilibrium about a point: \[ \sum \tau_{\text{clockwise}} = \sum \tau_{\text{anticlockwise}} \]
- Equilibrium also requires zero resultant force: \( \sum \vec{F} = \vec{0} \). Both translational and rotational conditions must hold simultaneously.
- Problem-solving flow:
- Draw the lever, marking all forces and pivot locations.
- Replace angled forces with perpendicular components about the pivot.
- Take moments about the pivot (or any convenient point) and equate clockwise/anticlockwise terms.
- Use \( \sum \vec{F} = \vec{0} \) if additional unknown forces remain.
Common Moment Scenarios
- Balanced beam: equal masses on a metre rule satisfy \( m_1 g d_1 = m_2 g d_2 \).
- Door or wrench: wider grip (larger \( d_\perp \)) reduces required force for the same torque.
- Human arm: biceps attach close to the elbow, so muscles exert large forces to generate modest torques -- a Class 3 lever case study.
Centre of Gravity
- The centre of gravity (COG) is the point where the entire weight of a body may be considered to act.
- Uniform, symmetrical objects have their COG at the geometric centre. Irregular shapes need experimental determination.
- Suspend-and-plumb method for a flat irregular lamina:
- Drill three small holes near the edge, far apart.
- Suspend the lamina from the first hole using a pin and let it hang freely.
- Hang a plumb line from the same pin; mark the vertical traced by the string.
- Repeat from the other holes; the intersection of the lines locates the COG.
- The object settles with its COG vertically beneath the suspension point because any offset would create an unbalanced moment and cause rotation.
Stability and Equilibrium Types
- Stability depends on how the COG moves relative to the base when the object is tilted.
- Stable equilibrium: after a small tilt, the COG rises and its vertical line falls inside the base. Weight creates a restoring moment back to the original position.
- Unstable equilibrium: the COG shifts beyond the base, so weight produces an overturning moment that topples the object.
- Neutral equilibrium: the COG remains at the same height regardless of position (e.g., a ball on a flat surface); no net moment develops.
- Improve stability by lowering the COG or widening the base so the vertical line through the COG remains within support boundaries.
Worked Example: Uniform Beam with Hanging Masses
A light, uniform \( \pu{1.2 m} \) beam is pivoted \( \pu{0.30 m} \) from its left end. A ( \pu{25 N} ) weight hangs \( \pu{0.10 m} \) from the left end. Find the distance from the pivot to the point where a ( \pu{15 N} ) weight must hang on the right to balance the beam.
- The beam's own weight acts at its centre; because it is light, neglect it (or treat it as already balanced by the pivot).
- Distance of the ( \pu{25 N} ) weight from the pivot: \( d_1 = \pu{0.30 m} - \pu{0.10 m} = \pu{0.20 m} \).
- Take moments about the pivot. Define clockwise as positive. The left weight produces an anticlockwise moment, the right weight produces clockwise. \[ 15 \times d_2 = 25 \times 0.20 \]
- Solve: \( d_2 = \dfrac{25 \times 0.20}{15} \approx \pu{0.33 m} \).
- Measure \( \pu{0.33 m} \) to the right of the pivot (i.e., about ( \pu{0.63 m} ) from the left end) to achieve balance.
Key Takeaways
- Treat every moment problem with a clear diagram and perpendicular distances.
- Equilibrium requires both zero net force and matched clockwise/anticlockwise moments.
- Locate the COG experimentally with the suspend-and-plumb method, then reason about stability via how the COG shifts relative to the object's base.