Curl of Gradient is Zero
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
- 1951: B. Hague: An Introduction to Vector Analysis (5th ed.) ... (previous) ... (next): Chapter $\text {V}$: Further Applications of the Operator $\nabla$: $2$. The Operator $\curl \grad$: $(5.3)$
- 1968: Murray R. Spiegel: Mathematical Handbook of Formulas and Tables ... (previous) ... (next): $\S 22$: Miscellaneous Formulas involving $\nabla$: $22.43$