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Irrotational flow occurs where the curl of the velocity of the fluid is zero everywhere. That is when \nabla\times \vec = 0 Similarly, if it is assumed that the fluid is incompressible: \rho(x,y,z,t) = \rho \text Then, starting with the
continuity equation A continuity equation or transport equation is an equation that describes the transport of some quantity. It is particularly simple and powerful when applied to a conserved quantity, but it can be generalized to apply to any extensive quantity. ...
: \frac + \nabla\cdot(\rho\vec) = 0 The condition of incompressibility means that the time derivative of the density is 0, and that the density can be pulled out of the divergence, and divided out, thus leaving the continuity equation for an incompressible system: \nabla\cdot\vec = 0 Now, the
Helmholtz decomposition In physics and mathematics, in the area of vector calculus, Helmholtz's theorem, also known as the fundamental theorem of vector calculus, states that any sufficiently smooth, rapidly decaying vector field in three dimensions can be resolved into ...
can be used to write the velocity as the sum of the gradient of a scalar potential and as the curl of a vector potential. That is: \vec = -\nabla\phi + \nabla\times\vec Note that imposing the condition that \nabla\times\vec = 0 implies that \nabla\times(\nabla\times \vec) = 0 The curl of the gradient is always 0. Note that the curl of the curl of a function is only uniformly 0 for the vector potential being 0 itself. So, by the condition of irrotational flow: \vec = -\nabla\phi And then using the continuity equation \nabla\cdot\vec = 0, the scalar potential can be substituted back in to find Laplace's Equation for irrotational flow: Note that the
laplace equation In mathematics and physics, Laplace's equation is a second-order partial differential equation named after Pierre-Simon Laplace, who first studied its properties. This is often written as \nabla^2\! f = 0 or \Delta f = 0, where \Delta = \n ...
is a well-studied linear partial differential equation. Its solutions are infinite; however, most solutions can be discarded when considering physical systems, as boundary conditions completely determine the velocity potential. Examples of common boundary conditions include the velocity of the fluid, determined by \vec= -\nabla\phi, being 0 on the boundaries of the system. There is a great amount of overlap with
electromagnetism In physics, electromagnetism is an interaction that occurs between particles with electric charge. It is the second-strongest of the four fundamental interactions, after the strong force, and it is the dominant force in the interactions o ...
when solving this equation in general, as the Laplace equation also models the
electrostatic potential Electrostatics is a branch of physics that studies electric charges at rest ( static electricity). Since classical times, it has been known that some materials, such as amber, attract lightweight particles after rubbing. The Greek word for a ...
in a vacuum.The Feynman Lectures on Physics Vol. II Ch. 12: Electrostatic Analogs
/ref> There are many reasons to study irrotational flow, among them; *Many real-world problems contain large regions of irrotational flow. *It can be studied analytically. *It shows us the importance of
boundary layers In physics and fluid mechanics, a boundary layer is the thin layer of fluid in the immediate vicinity of a bounding surface formed by the fluid flowing along the surface. The fluid's interaction with the wall induces a no-slip boundary condi ...
and viscous forces. *It provides us tools for studying concepts of
lift Lift or LIFT may refer to: Physical devices * Elevator, or lift, a device used for raising and lowering people or goods ** Paternoster lift, a type of lift using a continuous chain of cars which do not stop ** Patient lift, or Hoyer lift, mobil ...
and drag.


See also

* Irrotational vector fields * Irrotational vortices *
Potential flow around a circular cylinder In mathematics, potential flow around a circular cylinder is a classical solution for the flow of an inviscid, incompressible fluid around a cylinder that is transverse to the flow. Far from the cylinder, the flow is unidirectional and uniform. T ...


References

{{reflist Fluid mechanics