Misplaced Pages

Kinetic energy

Article snapshot taken from Wikipedia with creative commons attribution-sharealike license. Give it a read and then ask your questions in the chat. We can research this topic together.

This is an old revision of this page, as edited by Michael Hardy (talk | contribs) at 02:17, 25 July 2004 (The relationship between relativistic and classical kinetic energy.). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

Revision as of 02:17, 25 July 2004 by Michael Hardy (talk | contribs) (The relationship between relativistic and classical kinetic energy.)(diff) ← Previous revision | Latest revision (diff) | Newer revision → (diff)

Kinetic energy (also called vis viva, or living force) is energy possessed by a body by virtue of its motion. The kinetic energy of a body is equal to the amount of work needed to establish its velocity and rotation, starting from rest.

Equations

Definition

E k = v d p {\displaystyle E_{k}=\int \mathbf {v} \cdot \mathrm {d} \mathbf {p} }

In words the above equation states that the kinetic energy (Ek) is equal to the integral of the dot product of the velocity (v) of a body and the infinitesimal of the body's momentum (p).

Newtonian mechanics

For non-relativistic mechanics, the total kinetic energy of a body can be considered as the sum of the body's translational kinetic energy and its rotational energy, or angular kinetic energy:

E k = E t + E r {\displaystyle E_{k}=E_{t}+E_{r}\,\!}

where:

  • Ek is the total kinetic energy
  • Et is the translational kinetic energy
  • Er is the rotational kinetic energy

For the translational kinetic energy of a body with mass m, whose centre of mass is moving in a straight line with linear velocity v, we can use the Newtonian approximation:

E t = 1 2 m v 2 {\displaystyle E_{t}={\begin{matrix}{\frac {1}{2}}\end{matrix}}mv^{2}}


If a body is rotating, its rotational kinetic energy or angular kinetic energy is calculated from:

E r = 1 2 I ω 2 {\displaystyle E_{r}={\begin{matrix}{\frac {1}{2}}\end{matrix}}I\omega ^{2}} ,

where:

Relativistic mechanics

In Einstein's relativistic mechanics, (used especially for near-light velocities) the kinetic energy of a body is:

E k = m c 2 ( γ 1 ) = γ m c 2 m c 2 {\displaystyle E_{k}=mc^{2}(\gamma -1)=\gamma mc^{2}-mc^{2}\;\!}
γ = 1 1 ( v / c ) 2 {\displaystyle \gamma ={\frac {1}{\sqrt {1-(v/c)^{2}}}}}
E k = γ m c 2 m c 2 = ( 1 1 v 2 / c 2 1 ) m c 2 {\displaystyle E_{k}=\gamma mc^{2}-mc^{2}=\left({\frac {1}{\sqrt {1-v^{2}/c^{2}}}}-1\right)mc^{2}}
  • Ek is the kinetic energy of the body
  • v is the velocity of the body
  • m is its rest mass
  • c is the speed of light in a vacuum.
  • γmc is the total energy of the body
  • mc is the rest mass energy.

It is an edifying exercise to show that the ratio of this relativistic kinetic energy to the Newtonian kinetic energry given by (1/2)mv

lim v 0 ( 1 1 v 2 / c 2   1 ) m c 2 m v 2 / 2 = 1. {\displaystyle \lim _{v\to 0}{\left({\frac {1}{\sqrt {1-v^{2}/c^{2}\ }}}-1\right)mc^{2} \over mv^{2}/2}=1.}

Relativity theory states that the kinetic energy of an object grows towards infinity as its velocity approaches the speed of light, and thus that it is impossible to accelerate an object to this boundary.

Where gravity is weak, and objects move at much slower velocities than light (e.g. in everyday phenomena on Earth), Newton's formula is an excellent approximation of relativistic kinetic energy.

Heat as kinetic energy

Heat is a form of energy due to the total kinetic energy of molecules and atoms of matter. The relationship between heat, temperature and kinetic energy of atoms and molecules is the subject of statistical mechanics. Heat is more akin to work in that it represents a change in internal energy. The energy that heat represents specifically refers to the energy associated with the random translational motion of atoms and molecules in some identifiable matter within a system. The conservation of heat and work form the first law of thermodynamics.

See also

Category: