Difference between revisions of "heat dissipation"
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== thermal conductivity of materials == | == thermal conductivity of materials == | ||
− | ;Diamond: | + | ;Diamond: 2200 W/(m·K) -- Note that thermal conductivity is not constant across all isotopes or environmental conditions. The <sup>12</sup>C (99.9%) isotope thermal conductivity is 33.2 W/(cm·K), and at low temperature that rises to 410 W/(cm·K) at 104 K. |
;Copper: 401 W·m−1·K−1 | ;Copper: 401 W·m−1·K−1 | ||
;Beryllium: specific heat (1925 J·kg<sup>−1</sup>·K<sup>−1</sup>) and thermal conductivity (216 W·m<sup>−1</sup>·K<sup>−1</sup>) | ;Beryllium: specific heat (1925 J·kg<sup>−1</sup>·K<sup>−1</sup>) and thermal conductivity (216 W·m<sup>−1</sup>·K<sup>−1</sup>) | ||
;Aluminum: 167 W/m-K | ;Aluminum: 167 W/m-K |
Latest revision as of 12:39, 12 October 2014
Heat dissipation, heat sinks, cooling, thermal management
thermal conductivity of materials
- Diamond
- 2200 W/(m·K) -- Note that thermal conductivity is not constant across all isotopes or environmental conditions. The 12C (99.9%) isotope thermal conductivity is 33.2 W/(cm·K), and at low temperature that rises to 410 W/(cm·K) at 104 K.
- Copper
- 401 W·m−1·K−1
- Beryllium
- specific heat (1925 J·kg−1·K−1) and thermal conductivity (216 W·m−1·K−1)
- Aluminum
- 167 W/m-K