Curl of Gradient is Zero

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Definition

Let $\map {\R^3} {x, y, z}$ denote the real Cartesian space of $3$ dimensions..

Let $\map U {x, y, z}$ be a scalar field on $\R^3$.


Then:

$\map \curl {\grad U} = \mathbf 0$

where:

$\curl$ denotes the curl operator
$\grad$ denotes the gradient operator.


Proof

From Curl Operator on Vector Space is Cross Product of Del Operator and definition of the gradient operator:

\(\ds \grad \mathbf U\) \(=\) \(\ds \nabla U\)
\(\ds \map \curl {\grad U}\) \(=\) \(\ds \nabla \times \paren {\nabla U}\)

where $\nabla$ denotes the del operator.


Hence we are to demonstrate that:

$\nabla \times \paren {\nabla U} = \mathbf 0$


Let $\tuple {\mathbf i, \mathbf j, \mathbf k}$ be the standard ordered basis on $\R^3$.


Then:

\(\ds \nabla \times \paren {\nabla U}\) \(=\) \(\ds \nabla \times \paren {\dfrac {\partial U} {\partial x} \mathbf i + \dfrac {\partial U} {\partial y} \mathbf j + \dfrac {\partial U} {\partial z} \mathbf k}\) Definition of Gradient Operator
\(\ds \) \(=\) \(\ds \paren {\dfrac \partial {\partial y} \dfrac {\partial U} {\partial z} - \dfrac \partial {\partial z} \dfrac {\partial U} {\partial y} } \mathbf i + \paren {\dfrac \partial {\partial z} \dfrac {\partial U} {\partial x} - \dfrac \partial {\partial x} \dfrac {\partial U} {\partial z} } \mathbf j + \paren {\dfrac \partial {\partial x} \dfrac {\partial U} {\partial y} - \dfrac \partial {\partial y} \dfrac {\partial U} {\partial x} } \mathbf k\) Definition of Curl Operator
\(\ds \) \(=\) \(\ds \paren {\dfrac {\partial^2 U} {\partial y \partial z} - \dfrac {\partial^2 U} {\partial z \partial y} } \mathbf i + \paren {\dfrac {\partial^2 U} {\partial z \partial x} - \dfrac {\partial^2 U} {\partial x \partial z} } \mathbf j + \paren {\dfrac {\partial^2 U} {\partial x \partial y} - \dfrac {\partial^2 U} {\partial y \partial x} } \mathbf k\)


From Clairaut's Theorem:

$\dfrac {\partial^2 U} {\partial x \partial y} = \dfrac {\partial^2 U} {\partial y \partial x}$

and the same mutatis mutandis for the other partial derivatives.

The result follows.

$\blacksquare$


Physical Interpretation

From Vector Field is Expressible as Gradient of Scalar Field iff Conservative, the vector field given rise to by $\grad F$ is conservative.

The characteristic of a conservative field is that the contour integral around every simple closed contour is zero.

Since the curl is defined as a particular closed contour contour integral, it follows that $\map \curl {\grad F}$ equals zero.


Examples

Electrostatic Field

Let $R$ be a region of space in which there exists an electric potential field $F$.

From Electric Force is Gradient of Electric Potential Field, the electrostatic force $\mathbf V$ experienced within $R$ is the negative of the gradient of $F$:

$\mathbf V = -\grad F$

Hence from Curl of Gradient is Zero, the curl of $\mathbf V$ is zero.


Sources