Thermal Conductivity of Common Metals

Thermal conductivity (κ, in W/m·K) measures how effectively a material conducts heat. In metals, heat conduction is dominated by free electron transport, governed by the Wiedemann–Franz law, which relates electrical conductivity and thermal conductivity via the Lorenz number. This makes metals excellent thermal conductors, though the degree varies significantly based on electron mobility, crystal structure, and impurity content.

The table below summarizes the thermal conductivity of several common metals at room temperature (approximately 300 K), based on standard bulk, annealed samples. All values are approximate and can vary depending on alloying, grain size, and temperature.

Metal Thermal Conductivity (W/m·K) Notes
Silver 429 Highest among pure metals
Copper 401 Widely used due to high κ and low cost
Gold 318 High κ, but expensive
Aluminum 237 Lightweight, good thermal conductor
Brass 109 Alloy; lower κ due to scattering
Iron 80 Ferromagnetic effects influence κ
Steel (plain) ~50 Alloy-dependent, generally low
Titanium 22 Low κ despite metallic bonding
Lead 35 Low κ due to heavy atoms, soft lattice
Stainless Steel 16 High alloying reduces electron mobility
Mercury 8.3 Liquid at room temp; poor metal κ

 

Discussion

Silver is the most thermally conductive metal due to its high electron mobility and minimal scattering. Copper is nearly as conductive but much cheaper, making it a standard in thermal and electrical applications. Alloys like brass and steel show significantly reduced conductivity due to increased electron scattering from disorder and impurity atoms.

Thermal conductivity is not solely dictated by atomic mass or density; rather, it's a complex interplay between electronic structure and phonon scattering. Metals with high thermal conductivity are often also excellent electrical conductors, but exceptions arise when lattice vibrations dominate, especially in alloys or at high temperatures.

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