Solve Fourier's law of heat conduction (q = k·A·ΔT/L) in any direction, build series and parallel thermal resistances, convert conductivity units, look up 34 materials, and back out k from guarded hot plate measurements. Everything runs in your browser.
Steady-state, one-dimensional conduction — ignores edge effects, convection, and radiation. Sign of q follows ΔT.
Same heat flows through every layer. Rtotal = Σ Li/(ki·A).
Each path sees the full ΔT (e.g. studs vs. insulation bays). 1/Rtotal = Σ 1/Ri.
Representative room-temperature (~20 °C) values in W/(m·K), spot-checked against the CRC Handbook of Chemistry & Physics. Real products vary — check manufacturer datasheets for certified values. Lower k = better insulator.
| Material | Category | k, W/(m·K) | k, BTU/(hr·ft·°F) | Note |
|---|---|---|---|---|
| Diamond | Metals & high conductors | 2000 | 1156 | natural, ~2200 max |
| Silver | Metals & high conductors | 429 | 247.9 | highest of the metals |
| Copper | Metals & high conductors | 401 | 231.7 | CRC 401 |
| Gold | Metals & high conductors | 317 | 183.2 | |
| Aluminium | Metals & high conductors | 237 | 136.9 | CRC 237 |
| Tungsten | Metals & high conductors | 174 | 100.5 | |
| Zinc | Metals & high conductors | 116 | 67.02 | |
| Brass | Metals & high conductors | 109 | 62.98 | alloy, varies |
| Nickel | Metals & high conductors | 91 | 52.58 | |
| Iron (pure) | Metals & high conductors | 80 | 46.22 | CRC 80.2 |
| Platinum | Metals & high conductors | 72 | 41.6 | |
| Bronze | Metals & high conductors | 60 | 34.67 | alloy, varies |
| Cast iron | Metals & high conductors | 55 | 31.78 | |
| Carbon steel | Metals & high conductors | 50 | 28.89 | |
| Lead | Metals & high conductors | 35 | 20.22 | |
| Titanium | Metals & high conductors | 22 | 12.71 | |
| Stainless steel | Metals & high conductors | 16 | 9.245 | austenitic ~16 |
| Mercury | Liquids | 8.3 | 4.796 | liquid metal |
| Quartz | Other solids | 6.5 | 3.756 | crystalline |
| Marble | Other solids | 2.8 | 1.618 | |
| Ice (0 C) | Other solids | 2.2 | 1.271 | at 0 C |
| Concrete | Other solids | 1.7 | 0.9822 | dense, varies |
| Glass (soda-lime) | Other solids | 1 | 0.5778 | window glass |
| Brick | Other solids | 0.72 | 0.416 | common clay |
| Water (20 C) | Liquids | 0.6 | 0.3467 | 0.598 at 20 C |
| Polyethylene (HDPE) | Other solids | 0.42 | 0.2427 | |
| PTFE (Teflon) | Other solids | 0.25 | 0.1444 | |
| Rubber | Other solids | 0.15 | 0.08667 | natural |
| Wood (pine) | Other solids | 0.12 | 0.06933 | across grain |
| Engine oil | Liquids | 0.145 | 0.08378 | at 20 C |
| Glass wool insulation | Insulation & gases | 0.04 | 0.02311 | still air trapped |
| Air (still, 20 C) | Insulation & gases | 0.026 | 0.01502 | 0.0262 at 300 K |
| Polyurethane foam | Insulation & gases | 0.025 | 0.01444 | rigid board |
| Silica aerogel | Insulation & gases | 0.015 | 0.008667 | among the lowest solids |
Reference lab method (ASTM C177): clamp a flat specimen of thickness L between a metered hot plate and a cold plate; at steady state, k = q·L/(A·ΔT). Use the metered (guarded) area for A.
Heat conducted through a flat slab is proportional to the material's conductivity k, the area A, and the temperature difference ΔT, and inversely proportional to the thickness L. Units must be consistent: with k in W/(m·K), A in m², ΔT in K, and L in m, q comes out in watts.
Worked example: a copper plate (k = 401 W/(m·K)), area 0.01 m², with 50 K across 0.02 m of thickness, conducts q = 401 × 0.01 × 50 / 0.02 = 10,025 W. Swap copper for glass (k = 1.0) and the same slab passes only 25 W.
Resistance is the conduction analog of electrical resistance: q = ΔT/R. Stack layers in series by adding (brick 0.1 m/k=0.72 plus insulation 0.05 m/k=0.04 gives r = 0.139 + 1.25 = 1.389 m²·K/W); combine side-by-side paths in parallel with 1/R = Σ 1/Ri (paths of 2 and 3 K/W give 1.2 K/W).
The exact bridges: 1 W/(m·K) = 0.5778 BTU/(hr·ft·°F); 1 BTU/(hr·ft·°F) = 1.7307 W/(m·K). For temperature differences, 1 °F = 5/9 K, so ΔT converts by simple scaling (no 32 °F offset).
The reference method (ASTM C177) measures heater power q through a specimen of known L and metered area A at a steady ΔT, then k = q·L/(A·ΔT). Example: 2.5 W through 0.025 m thickness, 0.04 m² area, 10 K drop → k = 0.15625 W/(m·K).
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