α = (1/L)(∂L/∂T)for which L is the gauge length, T is the temperature, and the dimensions are usually (1/°C). The following table lists the thermal expansion coefficient at room temperature (20°C) for a variety of materials.
| Material | α (10-6/°C) | Material | α (10-6/°C) |
| Ethanol | 250 | Carbon steel | 10.8 |
| Water | 69 | Glass | 8.5 |
| Mercury | 61 | Alumina | 7.8 |
| Aluminium | 23 | Tungsten | 4.5 |
| Stainless steel | 17.3 | Borosilicate glass | 3.3 |
| Copper | 17 | Invar | 1.2 |
| Nickel | 13 | Diamond | 1 |
| Concrete | 12 | Fused quartz | 0.59 |
![]() | The crystal structure of scandium fluoride. Drawing by author, rendered with Inkscape. |
Principle of negative thermal expansion in scandium fluoride. The fluorine atoms vibrate in a transverse direction to the scandium atoms to pull them together. Drawing by author, rendered with Inkscape.
One curious finding is that the restoring force of the fluorine vibration is a function of the fourth power of the displacement. This quartic oscillation is unlike the quadratic (second power) oscillation that's found in atomic vibrations and harmonic oscillators.[7] Says Brent Fultz, study coauthor and Professor of Materials Science and Applied Physics at Caltech, "A nearly pure quantum quartic oscillator has never been seen in atom vibrations in crystals."[7]
The research team speculates that quartic oscillator materials may also be good thermal insulating materials. NTE materials can be combined with other materials to produce zero expansion materials, at least over a small temperature range. Such materials would be useful in optics, but also things as mundane as dental restoration.[6]