Mechanics of deformable solids Definition
Föppl–von Kármán equations
Builds on Kirchhoff–Love plate theoryBiharmonic plate equationAiry stress functionGaussian curvature
Definition
Let be the mid-plane of a thin isotropic plate of thickness , with Young's modulus , Poisson's ratio and bending stiffness . Let be the transverse load per unit area, the deflection and an Airy stress function for the membrane forces, so that For functions on put The Föppl–von Kármán equations are
Remarks
Here , which is twice the linearised Gaussian curvature of the deflected surface. The first equation is vertical equilibrium, in which the membrane forces act on the curvature; the second is the compatibility of the in-plane strains.
Example: if , the equations reduce to with , the plane stress problem of a flat plate. For a cylindrical bending one has , so is allowed: the plate can bend into a cylinder without stretching.
Non-example: the pair and is the linear biharmonic plate equation; it fails the second equation whenever has non-zero Gaussian curvature, such as with .
Sign conventions for and differ between texts.
Reading path
To understand this page from the ground up, read these 5 pages in order. The foundations come first.
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- no evidence level
- Airy stress function concept
- Biharmonic plate equation concept
- Gaussian curvature concept
- Kirchhoff–Love plate theory concept
- Föppl–von Kármán equations definition
Further reading
About this page
| Tag | GWR4DGJR23 |
|---|---|
| URI | m2://GWR4DGJR23 |
| Kind | definition |
| Writing | W0 stub |
| MSC | 74K20, 74B20, 74G60 |
| Defines | Föppl–von Kármán equations |
| Uses | Kirchhoff–Love plate theory, Biharmonic plate equation, Airy stress function, Gaussian curvature |
| Changed | 3 November 2026 |
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