Work at an Angle
Work at an Angle
- Forces are often not lined up with the motion: a rope pulls upward at an angle while the box slides along the floor.
- Only the part of the force along the motion does work. One cosine handles it.
Only the along-the-motion part counts
Symbols
- = work done (J)
- = force (N)
- = displacement (m)
- = angle between the force and the displacement (no unit (degrees or radians))
- is the component of the force along the motion: the resolving skill from lesson 1.9.
- Three special cases follow at once. Force along the motion: , full work. Force at 90°: , zero work. Force against the motion: , negative work (the force takes energy away).
- Friction and drag point against the motion, so they do negative work: a 12 N friction force over 3.0 m takes away .
Worked example
One change: gravity on a slope
A stone of weight 5.0 N rolls 50 m down a slope, dropping a vertical height of 30 m. Find the work done by gravity.
- Gravity acts vertically, so only the vertical part of the movement counts: 30 m, not 50 m.
- .
Answer
Worked example
Exam version: pulled by a kite wire
A skier moves at a constant 4.4 m s⁻¹ for 30 s, pulled by a wire at 30° above the horizontal with tension 140 N. Find the work done by the tension. (9702/22/F/M/20 Q3(b)(i))
- Displacement first: .
- Only the horizontal part of the tension does work: .
Answer
Common mistake
Multiplying the full force by the full path length without checking directions. First ask: how far did the object move along this force's direction? A weight moved horizontally p and vertically q does work , not the diagonal (9702/13/O/N/24 Q19).
- A useful zero: throw a ball up to height h and let it come back to the same height. Gravity did negative work going up and equal positive work coming down: total zero (9702/11/O/N/24 Q18).