A vector operator is a differential operator used in vector calculus.[1] Vector operators include:

Defined in terms of del:

\begin{align} \operatorname{grad} &\equiv \nabla \\ \operatorname{div} &\equiv \nabla \cdot \\ \operatorname{curl} &\equiv \nabla \times \end{align}

The Laplacian operates on a scalar field, producing a scalar field:

\nabla^2 \equiv \operatorname{div}\ \operatorname{grad} \equiv \nabla \cdot \nabla

Vector operators must always come right before the scalar field or vector field on which they operate, in order to produce a result. E.g.

\nabla f

yields the gradient of f, but

f \nabla

is just another vector operator, which is not operating on anything.

A vector operator can operate on another vector operator, to produce a compound vector operator, as seen above in the case of the Laplacian.

See also

References

  1. ^ "12.2: Vector Operators". Physics LibreTexts. 2020-05-09. Retrieved 2025-05-14.

Further reading

  • H. M. Schey (1996) Div, Grad, Curl, and All That: An Informal Text on Vector Calculus, ISBN 0-393-96997-5.