| Display title | Physics:Carreau fluid |
| Default sort key | Carreau fluid |
| Page length (in bytes) | 2,317 |
| Namespace ID | 3020 |
| Namespace | Physics |
| Page ID | 444967 |
| 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>Carolyn |
| Date of page creation | 06:35, 5 February 2024 |
| Latest editor | imported>Carolyn |
| Date of latest edit | 06:35, 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. | Carreau fluid in physics is a type of generalized Newtonian fluid where viscosity, $ \mu _{\operatorname {eff} } $, depends upon the shear rate, $ {\dot {\gamma }} $, by the following equation:
$ \mu _{\operatorname {eff} }({\dot {\gamma }})=\mu _{\operatorname {\inf } }+(\mu _{0}-\mu _{\operatorname... |
