Laplacian vector field
In vector calculus, a Laplacian vector field is a vector field which is both irrotational and incompressible.<ref>Template:Cite book</ref> If the field is denoted as v, then it is described by the following differential equations:
- <math>\begin{align}
\nabla \times \mathbf{v} &= \mathbf{0}, \\
\nabla \cdot \mathbf{v} &= 0.
\end{align}</math>
Laplace's equationEdit
From the vector calculus identity <math>\nabla^2 \mathbf{v} \equiv \nabla (\nabla\cdot \mathbf{v}) - \nabla\times (\nabla\times \mathbf{v})</math> it follows that
- <math>\nabla^2 \mathbf{v} = \mathbf{0}</math>
that is, that the field v satisfies Laplace's equation.<ref>Template:Cite book</ref>
However, the converse is not true; not every vector field that satisfies Laplace's equation is a Laplacian vector field, which can be a point of confusion. For example, the vector field <math>{\bf v} = (xy, yz, zx)</math> satisfies Laplace's equation, but it has both nonzero divergence and nonzero curl and is not a Laplacian vector field.
Cauchy-Riemann equationsEdit
A Laplacian vector field in the plane satisfies the Cauchy–Riemann equations: it is holomorphic.
Potential of Laplacian fieldEdit
Suppose the curl of <math>\mathbf{u}</math> is zero, it follows that (when the domain of definition is simply connected) <math>\mathbf{u}</math> can be expressed as the gradient of a scalar potential (see irrotational field) which we define as <math>\phi</math>:
- <math> \mathbf{u} = \nabla \phi \qquad \qquad (1) </math>
since it is always true that <math> \nabla \times \nabla \phi = 0 </math>.<ref name=":0">{{#invoke:citation/CS1|citation |CitationClass=web }}</ref>
Other forms of <math> \mathbf{u} = \nabla \phi </math> can be expressed as
<math> u_{i} = \frac{\partial \phi}{\partial x _{1}} \quad ; \quad u = \frac{\partial \phi}{\partial x}, v = \frac{\partial \phi}{\partial y}, w = \frac{\partial \phi}{\partial z} </math>.<ref name=":0" />
When the field is incompressible, then
<math>\nabla \cdot u = 0 \quad \textrm{or} \quad \frac{\partial u_{j}}{\partial x_{j}} = 0 \quad \textrm{or} \quad \frac{\partial u}{\partial x} + \frac{\partial v}{\partial y} +\frac{\partial w}{\partial z} = 0</math>.<ref name=":0" />
And substituting equation 1 into the equation above yields
- <math> \nabla^2 \phi = 0.</math><ref name=":0" />
Therefore, the potential of a Laplacian field satisfies Laplace's equation.<ref name=":0" />
Potential flow theoryEdit
The Laplacian vector field has an impactful application in fluid dynamics. Consider the Laplacian vector field to be the velocity potential <math>\phi</math> which is both irrotational and incompressible.
Irrotational flow is a flow where the vorticity, <math>\omega</math>, is zero, and since <math>\omega = \nabla \times u </math>, it follows that the condition <math>\omega = 0</math> is satisfied by defining a quantity called the velocity potential <math>\phi</math>, such that <math>u = \nabla \phi</math>, since <math>\nabla \times \nabla \phi = 0</math> always holds true.<ref name=":0" />
Irrotational flow is also called potential flow.<ref name=":0" />
If the fluid is incompressible, then conservation of mass requires that
<math display="inline">\nabla \cdot u = 0 \quad \textrm{or} \quad \frac{\partial u_{j}}{\partial x_{j}} = 0 \quad \textrm{or} \quad \frac{\partial u}{\partial x} + \frac{\partial v}{\partial y} + \frac{\partial w}{\partial z} = 0</math>.<ref name=":1">{{#invoke:citation/CS1|citation |CitationClass=web }}</ref>
And substituting the previous equation into the above equation yields <math>\nabla ^2 \phi = 0</math> which satisfies the Laplace equation.<ref name=":1" />
In planar flow, the stream function <math>\psi</math> can be defined with the following equations for incompressible planar flow in the xy-plane:
<math>u = \frac{\partial \psi}{\partial y} \quad \textrm{and} \quad v = -\frac{\partial \psi}{\partial x}</math>.<ref name=":0" />
When we also take into consideration <math>u = \frac{\partial \phi}{\partial x} \quad \textrm{and} \quad v = \frac{\partial \phi}{\partial y}</math>, we are looking at the Cauchy-Reimann equations.<ref name=":0" />
These equations imply several characteristics of an incompressible planar potential flow. The lines of constant velocity potential are perpendicular to the streamlines (lines of constant <math>\psi</math>) everywhere.<ref name=":1" />
Further readingEdit
The Laplacian vector field theory is being used in research in mathematics and medicine. Math researchers study the boundary values for Laplacian vector fields and investigate an innovative approach where they assume the surface is fractal and then must utilize methods for calculating a well-defined integration over the boundary.<ref>Template:Cite journal</ref> Medical researchers proposed a method to obtain high resolution in vivo measurements of fascicle arrangements in skeletal muscle, where the Laplacian vector field behavior reflects observed characteristics of fascicle trajectories.<ref>Template:Cite journal</ref>