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In vector calculus, curl is a vector operator that shows a vector field's tendency to rotate about a point.
A vector field which has zero curl everywhere is called irrotational.
In mathematics the curl is noted by:
where <math>\nabla<math> is the vector differential operator del, and F is the vector field the curl is being applied to.
Expanded in Cartesian coordinates, <math>\nabla \times F<math> is, for F composed of [Fx, Fy, Fz]:
{\partial F_z / \partial y} - {\partial F_y / \partial z} \\ {\partial F_x / \partial z} - {\partial F_z / \partial x}\\ {\partial F_y / \partial x} - {\partial F_x / \partial y} \end{pmatrix}<math>
A simple way to remember the expanded form of the curl is to think of it as:
{\partial / \partial x} \\ {\partial / \partial y} \\ {\partial / \partial z} \end{pmatrix} \times F<math>
or as the determinant of the following matrix:
{\partial / \partial x} & {\partial / \partial y} & {\partial / \partial z} \\ F_x & F_y & F_z \end{pmatrix}<math>
where i, j, and k are the unit vectors for the x, y, and z axes, respectively.
Note that the result of the curl operator acting on a vector field is not really a vector, it is a pseudovector. This means that it takes on opposite values in left-handed and right-handed coordinate systems (see Cartesian coordinate system). (Conversely, the curl of a pseudovector is a vector.)