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Theory

Kinetic Energy

Moving bodies carry energy proportional to mass and speed squared.

Kinetic energy is the energy associated with motion. In classical mechanics, translational kinetic energy grows with mass and with the square of speed, which is why speed changes have a disproportionately large effect on energy.

Definition (translation)

For a body of mass m moving with speed v:

K = 1/2 m v^2

The SI unit is the joule (J).

Work–energy theorem

Net work done on a body equals the change in its kinetic energy:

W_net = ∫ F · dr = ΔK

This connects forces (dynamics) to energy changes without explicitly solving for motion as a function of time.

Relation to momentum

For constant mass, p = m v, so kinetic energy can be written as

K = p^2 / (2m)

This is useful when momentum is the natural conserved quantity (collisions) but you want an energy estimate.

Rotational kinetic energy

For rotation with angular speed ω and moment of inertia I:

K_rot = 1/2 I ω^2

For rigid-body motion, total kinetic energy splits into translation of the center of mass plus rotation about it.

Collisions and energy

In an isolated system, momentum is conserved. Kinetic energy is conserved only for elastic collisions. In inelastic collisions, some kinetic energy is converted to internal energy (heat), sound, permanent deformation, etc.

Common pitfalls

  • K depends on speed (a scalar), not velocity direction, and is always ≥ 0.
  • Doubling speed quadruples kinetic energy.

Related Theories

Beginner

#conservation

Conservation of Energy
In ideal systems, energy changes form but total mechanical energy stays constant.
Beginner

#momentum

Momentum
A vector quantity that measures motion and is conserved in isolated systems.
Intermediate

#collision

Elastic Collision
Elastic collisions preserve both momentum and kinetic energy.
Intermediate

#conservation

Conservation of Momentum
Total momentum stays constant in a closed system, even during collisions.