Abstract
Compressively-stressed elastic films on finite-thickness viscous substrates can undergo a buckling instability that relieves stresses but destroys the planarity of the film. A linear-stability analysis is performed to determine the onset and maximally unstable mode of this buckling instability as a function of misfit strain, viscous layer thickness, and viscosity. We find that the onset of the buckling instability of the film on a glass layer is the same as that for a compressively stressed free-standing film. However, the maximally unstable wavelength increases as the glass layer thickness increases. Comparisons with experimental data are provided.
| Original language | English |
|---|---|
| Pages (from-to) | 2482-2484 |
| Journal | Applied Physics Letters |
| Volume | 78 |
| Issue number | 17 |
| Online published | 13 Apr 2001 |
| DOIs | |
| Publication status | Published - 23 Apr 2001 |
| Externally published | Yes |
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