The Physics Hypertextbook™
© 1998-2008 by Glenn Elert -- A Work in Progress
All Rights Reserved -- Fair Use Encouraged
Solids
| ΔL | = | L0 | α | ΔT | linear | |
| ΔA | = | A0 | 2α | ΔT | superficial (areal) | |
| ΔL | = | L0 | 3α | ΔT | volumetric |
Liquids
ΔV = V0βΔT
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
| Coefficients of Thermal Expansion for Selected Materials | ||||
| material | linear α (10−6 K−1) |
material | volume β (10−6 K−1) |
|
|---|---|---|---|---|
| aluminium | 23.1 | alcohol, ethyl | 1120 | |
| barium ferrite | 10 | gasoline | 950 | |
| brass | 20.3 | jet fuel, kerosene | 990 | |
| carbon, diamond | 1.18 | mercury | 181 | |
| carbon, graphite ∥ | 6.5 | water, liquid (1 °C) | −50 | |
| carbon, graphite ⊥ | 0.5 | water, liquid (4 °C) | 0 | |
| chromium | 4.9 | water, liquid (10 °C) | 88 | |
| concrete | 8 ~ 12 | water, liquid (20 °C) | 207 | |
| copper | 16.5 | water, liquid (30 °C) | 303 | |
| germanium | 6.1 | water, liquid (40 °C) | 385 | |
| glass | 8.5 | water, liquid (50 °C) | 457 | |
| gold | 14.2 | water, liquid (60 °C) | 522 | |
| iron | 11.8 | water, liquid (70 °C) | 582 | |
| lead | 28.9 | water, liquid (80 °C) | 640 | |
| nickel | 13.3 | water, liquid (90 °C) | 695 | |
| platinum | 8.8 | |||
| plutonium | 54 | |||
| silicon | 4.68 | |||
| silver | 18.9 | |||
| solder, lead-tin | 25 | |||
| steel, stainless | 17.3 | |||
| steel, structural | 12 | |||
| tin | 22 | |||
| titanium | 8.5 | |||
| tungsten | 4.5 | |||
| uranium | 13.9 | |||
| water, ice (0 °C) | 51 | |||
| zinc | 30.2 | |||
Thermal Expansion of Water [magnify]
Thermal Expansion of Water [magnify]
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.
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 °C, 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. [LLNL]
Thermal Expansion of Plutonium [magnify]
| Data for the Oceans | |
|---|---|
| surface area | 3.61 × 1014 m2 |
| mean depth | 3794 m |
| mean temperature, overall | 3.5 °C |
| mean temperature, top 10% | 10 °C |
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