Condition for Vector Field to satisfy Poisson's Equation
Theorem
Let $\mathbf V$ be a vector field over a region of space $R$.
Then:
- $\mathbf V$ is conservative but not solenoidal
- $\mathbf V$ is the gradient of a scalar field $F$ over $R$ which satisfies Poisson's equation over $R$:
- $\nabla^2 F = \phi$
- where $\phi$ is a function which is not identically zero.
Proof
Sufficient Condition
Let $\mathbf V$ be conservative but not solenoidal.
From Vector Field is Expressible as Gradient of Scalar Field iff Conservative:
- $\mathbf V = \grad F$
for some scalar field $F$ over $R$.
Because $\mathbf V$ is not solenoidal, we have:
- $\exists \mathbf v \in R: \operatorname {div} \mathbf v \ne 0$
that is:
- $\operatorname {div} \grad F \ne 0$
for at least some $\mathbf v \in R$.
Hence by Laplacian on Scalar Field is Divergence of Gradient:
- $\nabla^2 F = \phi$
where:
Hence $F$ satisfies Poisson's equation.
$\Box$
Necessary Condition
Let $\mathbf V$ be the gradient of a scalar field $F$ over $R$ which satisfies Poisson's equation:
- $\nabla^2 F = \phi$
where $\phi$ is not identically zero.
Thus $F$ is such that:
- $\mathbf V = \grad F$
and from Vector Field is Expressible as Gradient of Scalar Field iff Conservative it follows that $\mathbf V$ is conservative.
Then by Laplacian on Scalar Field is Divergence of Gradient:
- $\exists \mathbf v \in R: \operatorname {div} \grad F \ne 0$
That is:
- $\exists \mathbf v \in R: \operatorname {div} \mathbf V \ne 0$
and so by definition $\mathbf V$ is specifically not solenoidal.
$\blacksquare$
Sources
- 1951: B. Hague: An Introduction to Vector Analysis (5th ed.) ... (previous) ... (next): Chapter $\text {V}$: Further Applications of the Operator $\nabla$: $7$. The Classification of Vector Fields: $\text {(ii)}$