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[parent] lamellar field (Definition)

A vector field $ \vec{F} = \vec{F}(x,\,y,\,z)$, defined in an open set $ D$ of $ \mathbb{R}^3$, is lamellar if the condition

$\displaystyle \nabla\!\times\!\vec{F} = \vec{0}$
is satisfied in every point $ (x,\,y,\,z)$ of $ D$.

Here, $ \nabla\!\times\!\vec{F}$ is the curl or rotor of $ \vec{F}$. The condition is equivalent with both of the following:

The scalar potential has the expression
$\displaystyle u = \int_{P_0}^P\vec{F}\cdot d\vec{s},$
where the point $ P_0$ may be chosen freely, $ P = (x,\,y,\,z)$.

Note. In physics, $ u$ is in general replaced with $ V = -u$. If the $ \vec{F}$ is interpreted as a force, then the potential $ V$ is equal to the work made by the force when its point of application is deplaced from $ P_0$ to infinity.



"lamellar field" is owned by pahio.
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See Also: curl free field, Poincaré lemma, vector potential

Other names:  lamellar, irrotational, conservative, laminar
Also defines:  scalar potential, potential, rotor

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Cross-references: infinity, expression, domain, simply connected, partial derivatives, continuous, vanish, curve, contractible, line integrals, equivalent, point, open set, vector field
There are 42 references to this entry.

This is version 14 of lamellar field, born on 2004-10-11, modified 2007-12-04.
Object id is 6360, canonical name is LaminarField.
Accessed 7102 times total.

Classification:
AMS MSC26B12 (Real functions :: Functions of several variables :: Calculus of vector functions)

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