Mechanics → Work and Energy → Work-Energy Theorem
Work-Energy Theorem
Statement
The work done by a net force on a particle is equal to the change in its kinetic energy.
Mathematical Form
$$ W = \Delta K $$
Kinetic Energy
$$ K = \frac{1}{2}mv^2 $$
Derivation
From Newton’s second law:
$$ F = ma $$
Using:
$$ a = \frac{dv}{dt}, \quad v = \frac{dx}{dt} $$
We write:
$$ a = v \frac{dv}{dx} $$
So:
$$ F = m v \frac{dv}{dx} $$
Multiply both sides by $dx$:
$$ F dx = m v dv $$
Integrate:
$$ \int F dx = \int m v dv $$
$$ W = \frac{1}{2}mv^2 - \frac{1}{2}mu^2 $$
Thus:
$$ W = \Delta K $$