# Solenoidal vector field

In vector calculus a **solenoidal vector field** (also known as an **incompressible vector field**, a **divergence-free vector field**, or a **transverse vector field**) is a vector field **v** with divergence zero at all points in the field:

A common way of expressing this property is to say that the field has no sources or sinks. The field lines of a solenoidal field are either closed loops or end at infinity.

## PropertiesEdit

The fundamental theorem of vector calculus states that any vector field can be expressed as the sum of an irrotational and a solenoidal field. The condition of zero divergence is satisfied whenever a vector field **v** has only a vector potential component, because the definition of the vector potential **A** as:

automatically results in the identity (as can be shown, for example, using Cartesian coordinates):

The converse also holds: for any solenoidal **v** there exists a vector potential **A** such that (Strictly speaking, this holds only subject to certain technical conditions on **v**, see Helmholtz decomposition.)

The divergence theorem gives the equivalent integral definition of a solenoidal field; namely that for any closed surface, the net total flux through the surface must be zero:

- ,

where is the outward normal to each surface element.

## EtymologyEdit

*Solenoidal* has its origin in the Greek word for solenoid, which is σωληνοειδές (sōlēnoeidēs) meaning pipe-shaped, from σωλην (sōlēn) or pipe. In the present context of solenoidal it means constrained as if in a pipe, so with a fixed volume.

## ExamplesEdit

- The magnetic field
**B**(see Maxwell's equations) - The velocity field of an incompressible fluid flow
- The vorticity field
- The electric field
**E**in neutral regions ( ); - The current density
**J**where the charge density is unvarying, . - The magnetic vector potential
**A**in Coulomb gauge