Solids
| ΔL | = | L0 | α | ΔT | linear | |
| ΔA | = | A0 | 2α | ΔT | areal | |
| ΔL | = | L0 | 3α | ΔT | volumetric |
Liquids
ΔV = βV0ΔT
Liquids have higher expansivities than solids
β ≈ 10−3/K, 3α ≈ 10−5/K
Gases
[check out the gas laws]
behavior of gases is more complicated, gases will expand as much as pressure will allow
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Plutonium undergoes more phase transitions at ordinary pressures than any other element. As plutonium is heated it transforms through six different crystal structures before melting — α [alpha], β [beta], γ [gamma], Δ [delta], Δ′ [delta prime], and ε [epsilon]. Physical properties like density and thermal expansion vary significantly from phase to phase making it one of the more difficult metals to machine and work. The metallurgy of plutonium is best left to the experts.
Notes form LLNL that must be paraphrased. "One of plutonium's unique physical properties is that the pure metal exhibits six solid-state phase transformations before reaching its liquid state, passing from alpha, beta, gamma, delta, delta-prime, to epsilon. Large volume expansions and contractions occur between the stable room-temperature alpha phase and the element's liquid state. Another unusual feature is that unalloyed plutonium melts at a relatively low temperature, approximately 640 ℃, to yield a liquid of higher density than the solid from which it melts. In addition, the elastic properties of the delta face-centered cubic (fcc) phase of plutonium are highly directional (anisotropic). That is, the elasticity of the metal varies widely along different crystallographic directions by as much as a factor of six to seven."
| The Physics Hypertextbook © 1998–2013 Glenn Elert |
No condition is permanent.