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{{about|the general concept in the mathematical theory of vector fields|the vector potential in electromagnetism|Magnetic vector potential|the vector potential in fluid mechanics|Stream function}} | |||
In [[vector calculus]], a '''vector potential''' is a [[vector field]] whose [[Curl (mathematics)|curl]] is a given vector field. This is analogous to a ''[[scalar potential]]'', which is a scalar field whose [[gradient]] is a given vector field. | |||
Formally, given a vector field '''v''', a ''vector potential'' is a vector field '''A''' such that | |||
:<math> \mathbf{v} = \nabla \times \mathbf{A}. </math> | |||
If a vector field '''v''' admits a vector potential '''A''', then from the equality | |||
:<math>\nabla \cdot (\nabla \times \mathbf{A}) = 0</math> | |||
([[divergence]] of the [[Curl (mathematics)|curl]] is zero) one obtains | |||
:<math>\nabla \cdot \mathbf{v} = \nabla \cdot (\nabla \times \mathbf{A}) = 0,</math> | |||
which implies that '''v''' must be a [[solenoidal vector field]]. | |||
==Theorem== | |||
Let | |||
:<math>\mathbf{v} : \mathbb R^3 \to \mathbb R^3</math> | |||
be a [[solenoidal vector field]] which is twice [[smooth function|continuously differentiable]]. Assume that '''v'''('''x''') decreases sufficiently fast as ||'''x'''||→∞. Define | |||
:<math> \mathbf{A} (\mathbf{x}) = \frac{1}{4 \pi} \nabla \times \int_{\mathbb R^3} \frac{ \mathbf{v} (\mathbf{y})}{\left\|\mathbf{x} -\mathbf{y} \right\|} \, d\mathbf{y}. </math> | |||
Then, '''A''' is a vector potential for '''v''', that is, | |||
:<math>\nabla \times \mathbf{A} =\mathbf{v}. </math> | |||
A generalization of this theorem is the [[Helmholtz decomposition]] which states that any vector field can be decomposed as a sum of a solenoidal vector field and an [[irrotational vector field]]. | |||
==Nonuniqueness== | |||
The vector potential admitted by a solenoidal field is not unique. If '''A''' is a vector potential for '''v''', then so is | |||
:<math> \mathbf{A} + \nabla m </math> | |||
where ''m'' is any continuously differentiable scalar function. This follows from the fact that the curl of the gradient is zero. | |||
This nonuniqueness leads to a degree of freedom in the formulation of electrodynamics, or gauge freedom, and requires [[Gauge fixing|choosing a gauge]]. | |||
== See also == | |||
* [[Fundamental theorem of vector analysis]] | |||
* [[Magnetic potential]] | |||
* [[Solenoid]] | |||
== References == | |||
* ''Fundamentals of Engineering Electromagnetics'' by David K. Cheng, Addison-Wesley, 1993. | |||
[[Category:Concepts in physics]] | |||
[[Category:Potentials]] | |||
[[Category:Vector calculus]] |
Revision as of 05:26, 7 March 2013
29 yr old Orthopaedic Surgeon Grippo from Saint-Paul, spends time with interests including model railways, top property developers in singapore developers in singapore and dolls. Finished a cruise ship experience that included passing by Runic Stones and Church.
In vector calculus, a vector potential is a vector field whose curl is a given vector field. This is analogous to a scalar potential, which is a scalar field whose gradient is a given vector field.
Formally, given a vector field v, a vector potential is a vector field A such that
If a vector field v admits a vector potential A, then from the equality
(divergence of the curl is zero) one obtains
which implies that v must be a solenoidal vector field.
Theorem
Let
be a solenoidal vector field which is twice continuously differentiable. Assume that v(x) decreases sufficiently fast as ||x||→∞. Define
Then, A is a vector potential for v, that is,
A generalization of this theorem is the Helmholtz decomposition which states that any vector field can be decomposed as a sum of a solenoidal vector field and an irrotational vector field.
Nonuniqueness
The vector potential admitted by a solenoidal field is not unique. If A is a vector potential for v, then so is
where m is any continuously differentiable scalar function. This follows from the fact that the curl of the gradient is zero.
This nonuniqueness leads to a degree of freedom in the formulation of electrodynamics, or gauge freedom, and requires choosing a gauge.
See also
References
- Fundamentals of Engineering Electromagnetics by David K. Cheng, Addison-Wesley, 1993.