Writing gives and . Constant streamfunction means constant radius, so streamlines are circles. The tangential velocity is , and its anticlockwise circulation is .
Use an opposite vortex at as the image of the vortex at one:
On the two distances are equal, so and the wall is a streamline. Its velocity follows from : at the wall and .
The Bernoulli equation gives . Relative to the ambient pressure force, the fluid's excess force on the wall is in the positive direction. Using the supplied integral,
Thus the wall is attracted toward the fluid and vortex. Subtracting the uniform ambient pressure isolates the finite force due to the vortex.
For incompressible planar flow define the streamfunction by , . A velocity potential satisfies , when the flow is irrotational; the differential condition is . The complex potential of a two-dimensional potential flow is , with derivative .
For , its derivative is . This gives outward radial velocity , whose flux across a circle is . It is therefore the stated line source.
Superposition gives
For positive , the stagnation points are
They lie on the real axis, one upstream of the source and the other downstream of the sink. Streamlines are level sets of . The dividing streamline passes through both stagnation points and forms a Rankine oval enclosing the source and sink; outside, streamlines tend to uniform horizontal flow.
Figure 1.
A representative source-sink pair in a uniform stream, with two stagnation points and a dividing Rankine oval
. Details.
For an observation point in the wire's plane, both and lie in that plane. Their cross product is normal to it, and the Biot-Savart law integrates only such normal vectors. Thus the field is perpendicular to the plane at every point off the wire.
At the centre, all four sides contribute in the same normal direction by the right-hand rule. A single side is distance from the centre, so its contribution is
Multiplying by four gives
where is the oriented normal fixed by the current.
Take an admissible variation with on the boundary. Differentiating the functional at an extremum gives
Integration by parts removes the derivatives from ; the boundary term vanishes. The fundamental lemma of the calculus of variations yields
For the specified squared-gradient energy this is , so is harmonic. The affine function is harmonic and satisfies the boundary data.
To verify a global minimum, write with zero boundary trace. Then
The middle term vanishes by integration by parts, since and at the boundary. Hence , and
This proves minimality directly, rather than relying only on a necessary Euler-Lagrange equation.

Pinned article: Introduction to the OurBigBook Project

Welcome to the OurBigBook Project! Our goal is to create the perfect publishing platform for STEM subjects, and get university-level students to write the best free STEM tutorials ever.
Everyone is welcome to create an account and play with the site: ourbigbook.com/go/register. We belive that students themselves can write amazing tutorials, but teachers are welcome too. You can write about anything you want, it doesn't have to be STEM or even educational. Silly test content is very welcome and you won't be penalized in any way. Just keep it legal!
We have two killer features:
  1. topics: topics group articles by different users with the same title, e.g. here is the topic for the "Fundamental Theorem of Calculus" ourbigbook.com/go/topic/fundamental-theorem-of-calculus
    Articles of different users are sorted by upvote within each article page. This feature is a bit like:
    • a Wikipedia where each user can have their own version of each article
    • a Q&A website like Stack Overflow, where multiple people can give their views on a given topic, and the best ones are sorted by upvote. Except you don't need to wait for someone to ask first, and any topic goes, no matter how narrow or broad
    This feature makes it possible for readers to find better explanations of any topic created by other writers. And it allows writers to create an explanation in a place that readers might actually find it.
    Figure 1.
    Screenshot of the "Derivative" topic page
    . View it live at: ourbigbook.com/go/topic/derivative
  2. local editing: you can store all your personal knowledge base content locally in a plaintext markup format that can be edited locally and published either:
    This way you can be sure that even if OurBigBook.com were to go down one day (which we have no plans to do as it is quite cheap to host!), your content will still be perfectly readable as a static site.
    Figure 5. . You can also edit articles on the Web editor without installing anything locally.
    Video 3.
    Edit locally and publish demo
    . Source. This shows editing OurBigBook Markup and publishing it using the Visual Studio Code extension.
  3. https://raw.githubusercontent.com/ourbigbook/ourbigbook-media/master/feature/x/hilbert-space-arrow.png
  4. Infinitely deep tables of contents:
    Figure 6.
    Dynamic article tree with infinitely deep table of contents
    .
    Descendant pages can also show up as toplevel e.g.: ourbigbook.com/cirosantilli/chordate-subclade
All our software is open source and hosted at: github.com/ourbigbook/ourbigbook
Further documentation can be found at: docs.ourbigbook.com
Feel free to reach our to us for any help or suggestions: docs.ourbigbook.com/#contact