# Difference between revisions of "Conservation of Angular Momentum"

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==Proof of conservation== | ==Proof of conservation== | ||

− | The [[derivative]] of angular momentum with respect to time is equal to the sum of the external moments (or torque <math>\vec {\tau}</math>) applied to the system. Differentiating angular momentum gives: | + | The [[derivative]] of angular momentum with respect to time is equal to the sum of the external moments (or [[torque]] <math>\vec {\tau}</math>) applied to the system. Differentiating angular momentum gives: |

<math>\vec {\tau} = \vec r \times \vec F + \vec{\dot{r}} \times p</math> | <math>\vec {\tau} = \vec r \times \vec F + \vec{\dot{r}} \times p</math> |

## Revision as of 15:54, 9 December 2016

The **conservation of angular momentum** is a fundamental concept of physics along with other conservation laws such as those of energy and linear momentum. It states that the angular momentum of a system remains constant unless changed through an action of external forces.

In Newtonian mechanics, the angular momentum of a point mass about a point is defined as where is the position vector of the point mass with respect to the point of reference and is the linear momentum vector of the point mass.

The principle of angular momentum can be applied to a system of particles by summing the angular momentum of each particle about the same point. This can be represented as:

where

- is the total angular momentum of the system
- is the angular momentum of the i
^{th}particle

## Proof of conservation

The derivative of angular momentum with respect to time is equal to the sum of the external moments (or torque ) applied to the system. Differentiating angular momentum gives:

For a constant radius, the second term is zero. Hence From this, it can be concluded that in the absence of an external moment, angular momentum must be conserved.