| Display title | Physics:Von Kármán swirling flow |
| Default sort key | Von Kármán swirling flow |
| Page length (in bytes) | 18,169 |
| Namespace ID | 3020 |
| Namespace | Physics |
| Page ID | 407246 |
| Page content language | en - English |
| Page content model | wikitext |
| Indexing by robots | Allowed |
| Number of redirects to this page | 0 |
| Counted as a content page | Yes |
| HandWiki item ID | None |
| Edit | Allow all users (infinite) |
| Move | Allow all users (infinite) |
| Page creator | imported>JTerm |
| Date of page creation | 03:45, 5 February 2024 |
| Latest editor | imported>JTerm |
| Date of latest edit | 03:45, 5 February 2024 |
| Total number of edits | 1 |
| Recent number of edits (within past 90 days) | 0 |
| Recent number of distinct authors | 0 |
Description | Content |
Article description: (description)
This attribute controls the content of the description and og:description elements. | Von Kármán swirling flow is a flow created by a uniformly rotating infinitely long plane disk, named after Theodore von Kármán who solved the problem in 1921. The rotating disk acts as a fluid pump and is used as a model for centrifugal fans or compressors. This flow is classified under the category... |
