Barycentre: Difference between revisions

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In geometry, the barycentre or centre of mass or centre of gravity^[1] of a system of particles or a rigid body is a point at which various systems of force may be deemed to act. The gravitational attraction of a mass is centred at its barycentre (hence the term "centre of gravity"), and the (classical) angular momentum of the mass resolves into components related to the rotation of the body about its barycentre and the angular movement of the barycentre.

The barycentre is located as an "average" of the masses involved. For a system of n point particles of mass $m_{i}$ located at position vectors $\mathbf {x} _{i}$ , the barycentre ${\bar {\mathbf {x} }}$ is defined by

\left(\sum _{i=1}^{n}m_{i}\right){\bar {\mathbf {x} }}=\sum _{i=1}^{n}m_{i}\mathbf {x} _{i}.\,

For a solid body B with mass density $\rho (\mathbf {x} )$ at position $\mathbf {x}$ , with total mass

M=\iiint _{B}\rho (\mathbf {x} )\mathrm {d} \mathbf {x} ,\,

the barycentre is given by

M{\bar {\mathbf {x} }}=\iiint _{B}\mathbf {x} \rho (\mathbf {x} )\mathrm {d} \mathbf {x} .\,

Notes

↑ In physics, mass and gravitation describe two slightly but importantly different concepts: While the centre of mass ${\bar {\mathbf {x} }}_{m}$ is defined like ${\bar {\mathbf {x} }}$ above as a spatial average of masses, the centre of gravity can be expressed similarly as a spatial average of the forces $F_{i}$ involved: ${\bar {\mathbf {x} }}_{F}=\left(\sum _{i=1}^{n}F_{i}\right){\bar {\mathbf {x} }}=\sum _{i=1}^{n}m_{i}a_{i}\mathbf {x} _{i}.\,$ Hence, ${\bar {\mathbf {x} }}_{m}$ and ${\bar {\mathbf {x} }}_{F}$ are generally only identical if the gravitational field (as expressed in terms of the acceleration $a_{i}$ ) is constant for all $\mathbf {x} _{i}$ , such that $F_{i}=am_{i}$ . The point on which forces may be deemed to act is then naturally ${\bar {\mathbf {x} }}_{F}$ and not ${\bar {\mathbf {x} }}_{m}$ .

[1] In physics, mass and gravitation describe two slightly but importantly different concepts: While the centre of mass ${\bar {\mathbf {x} }}_{m}$ is defined like ${\bar {\mathbf {x} }}$ above as a spatial average of masses, the centre of gravity can be expressed similarly as a spatial average of the forces $F_{i}$ involved: ${\bar {\mathbf {x} }}_{F}=\left(\sum _{i=1}^{n}F_{i}\right){\bar {\mathbf {x} }}=\sum _{i=1}^{n}m_{i}a_{i}\mathbf {x} _{i}.\,$ Hence, ${\bar {\mathbf {x} }}_{m}$ and ${\bar {\mathbf {x} }}_{F}$ are generally only identical if the gravitational field (as expressed in terms of the acceleration $a_{i}$ ) is constant for all $\mathbf {x} _{i}$ , such that $F_{i}=am_{i}$ . The point on which forces may be deemed to act is then naturally ${\bar {\mathbf {x} }}_{F}$ and not ${\bar {\mathbf {x} }}_{m}$ .

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-In [[geometry]], the '''barycentre''' or '''centre of mass''' or '''centre of gravity'''<ref>In [[physics]], [[mass]] and [[gravitation]] describe two slightly but importantly different concepts: While the centre of mass <math> \bar\mathbf{x}_m </math> is defined as <math> \bar\mathbf{x} </math>  above, the centre of gravity can be expressed similarly as an average of the forces <math> F_i </math> involved: <math> \bar\mathbf{x}_F = \left( \sum_{i=1}^n F_i \right) \bar\mathbf{x} = \sum_{i=1}^n m_i a_i \mathbf{x}_i . \,</math> Hence, <math> \bar\mathbf{x}_m </math> and <math> \bar\mathbf{x}_F </math> are generally only identical if the gravitational field (as expressed in terms of the [[acceleration]] <math> a_i </math>) is constant for all <math> \mathbf{x}_i </math>, such that <math> F_i = a m_i </math>. The point on which forces may be deemed to act is then naturally <math> \bar\mathbf{x}_F </math> and not <math> \bar\mathbf{x}_m </math>.</ref> of a system of particles or a rigid body is a [[mass point|point]] at which various systems of [[force]] may be deemed to act.  The [[gravitational attraction]] of a mass is centred at its barycentre (hence the term "centre of gravity"), and the [[angular momentum (classical)|(classical) angular momentum]] of the mass resolves into components related to the rotation of the body about its barycentre and the angular movement of the barycentre.
+In [[geometry]], the '''barycentre''' or '''centre of mass''' or '''centre of gravity'''<ref>In [[physics]], [[mass]] and [[gravitation]] describe two slightly but importantly different concepts: While the centre of mass <math> \bar\mathbf{x}_m </math> is defined like <math> \bar\mathbf{x} </math>  above as a spatial average of masses, the centre of gravity can be expressed similarly as a spatial average of the forces <math> F_i </math> involved: <math> \bar\mathbf{x}_F = \left( \sum_{i=1}^n F_i \right) \bar\mathbf{x} = \sum_{i=1}^n m_i a_i \mathbf{x}_i . \,</math> Hence, <math> \bar\mathbf{x}_m </math> and <math> \bar\mathbf{x}_F </math> are generally only identical if the gravitational field (as expressed in terms of the [[acceleration]] <math> a_i </math>) is constant for all <math> \mathbf{x}_i </math>, such that <math> F_i = a m_i </math>. The point on which forces may be deemed to act is then naturally <math> \bar\mathbf{x}_F </math> and not <math> \bar\mathbf{x}_m </math>.</ref> of a system of particles or a rigid body is a [[mass point|point]] at which various systems of [[force]] may be deemed to act.  The [[gravitational attraction]] of a mass is centred at its barycentre (hence the term "centre of gravity"), and the [[angular momentum (classical)|(classical) angular momentum]] of the mass resolves into components related to the rotation of the body about its barycentre and the angular movement of the barycentre.
 The barycentre is located as an "average" of the masses involved.  For a system of ''n'' point particles of mass <math>m_i</math> located at position vectors <math>\mathbf{x}_i</math>, the barycentre <math>\bar\mathbf{x}</math> is defined by

Barycentre: Difference between revisions

Revision as of 21:52, 10 January 2009

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