| Display title | Physics:Kelvin–Voigt material |
| Default sort key | Kelvin-Voigt Material |
| Page length (in bytes) | 5,189 |
| Namespace ID | 3020 |
| Namespace | Physics |
| Page ID | 404857 |
| 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>WikiEd2 |
| Date of page creation | 04:46, 5 February 2024 |
| Latest editor | imported>WikiEd2 |
| Date of latest edit | 04:46, 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. | A Kelvin-Voigt material, also called a Voigt material, is the most simple model viscoelastic material showing typical rubbery properties. It is purely elastic on long timescales (slow deformation), but shows additional resistance to fast deformation. It is named after the British physicist and engineer... |
