The work–energy principle
The work–energy principle is Newton's law viewed through energy. It replaces a time-by-time motion calculation with one account between a chosen start and finish.
Total work by the real forces equals the change in kinetic energy
Symbols
- = add the signed work done by all real forces; Σ means add (J)
- = change in kinetic energy; Δ means final value minus initial value (J)
If is the initial speed and is the final speed, then:
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- Choose the start and finish, then record and .
- List the real forces acting throughout that interval.
- Write one signed work term for each force.
- Set their total equal to final KE minus initial KE.
Common mistake
Distinguish work supplied from the energy that resistance removes
Worked example
A cyclist speeds up against resistance
A cyclist and bicycle have total mass 72 kg. Their speed rises from 8 m s⁻¹ to 16 m s⁻¹ over 100 m against a constant 28 N resistance. Find the work done by the cyclist.
The energy transferred by working against resistance is:
The cyclist supplies energy both to increase kinetic energy and to replace the energy dissipated by resistance.
(9709/42/M/J/24 Q1)Examiner note
On a slope, keep path distance and vertical height separate
For a body moving distance down a slope of angle , gravity does positive work . A constant resistance does work .
Key idea
A 10 kg block moves 4 m down a plane inclined at . Its initial speed is 3 m s⁻¹ and a constant 20 N resistance opposes the motion. Find its final speed.
