Difference between revisions of "Hodge star"
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| − | Let <math>M</math> be a Riemannian n | + | Let <math>M</math> be a [[Riemannian manifold]] in <math>n</math> dimensions with [[metric]] <math>g</math>. The '''Hodge star''' operator is a [[linear]] [[operator]] from i-[[differential form]]s to (n-i)-differential forms |
<math> | <math> | ||
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| − | defined as follows: Let <math>\phi_1,...,\phi_n</math> be a local orthonormal | + | defined as follows: Let <math>\phi_1,...,\phi_n</math> be a local orthonormal [[coframe]] (i.e., a collection of locally defined 1-forms which are [[orthonormal]] with respect to the induced metric on the [[cotangent]] space). Then we define |
<math> | <math> | ||
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<math>\phi_1\wedge\cdots\wedge\phi_i\wedge *(\phi_1\wedge\cdots\wedge\phi_i)</math> | <math>\phi_1\wedge\cdots\wedge\phi_i\wedge *(\phi_1\wedge\cdots\wedge\phi_i)</math> | ||
| − | is the volume form on <math>M</math>. To define the Hodge star operator for general forms, we simply extend the above definition by linearity. | + | is the [[volume]] form on <math>M</math>. To define the Hodge star operator for general forms, we simply extend the above definition by [[linearity]]. |
==Example== | ==Example== | ||
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* fdx + gdy = fdy - gdx | * fdx + gdy = fdy - gdx | ||
</math> | </math> | ||
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| + | [[Category:Mathematics]] | ||
Revision as of 16:58, July 14, 2008
| This article/section deals with mathematical concepts appropriate for a student in late university or graduate level. |
Let be a Riemannian manifold in dimensions with metric . The Hodge star operator is a linear operator from i-differential forms to (n-i)-differential forms
defined as follows: Let be a local orthonormal coframe (i.e., a collection of locally defined 1-forms which are orthonormal with respect to the induced metric on the cotangent space). Then we define
where the plus or minus is chosen so that
is the volume form on . To define the Hodge star operator for general forms, we simply extend the above definition by linearity.
Example
Give the standard metric so that is a coframe. Then the volume form is . Thus,
and
and in general