• Pixel-art sticker of Warmohm, personifying Temperature Coefficient of Resistance, with the caption “Heat My Wire, I Resist More.”

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Warmohm

Temperature Coefficient of Resistance Physics

\[R = R_0 (1 + \alpha \Delta T)\]
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Meet Warmohm, a coil of wire who resists current more as he heats up. Hotter atoms vibrate harder and scatter electrons more. Copper rises about 0.0039 per kelvin, so warming by 100 K adds about 39 percent. A glowing tungsten filament exceeds ten times its cold resistance. Pixel-art kiss-cut sticker in 2, 3, 4 and 6 inches; equation, symbols and sources in the physics panel below.

Size
Surface

Flat $6 shipping worldwideMade to order, ships in 2–5 business days

Details

Size3″ × 3″

3″ × 3″ kiss-cut sticker.

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Flat $6 shipping on every order, worldwide, whatever's in it.

Delivery times & where we ship

Returns & replacements21 days

Every item is printed to order, so we can’t accept returns or exchanges for change of mind, or if you ordered the wrong size or colour.

Print defect, misprint, damage or the wrong item? We’ll send a free replacement, or a refund if you prefer. Report it within 21 days of delivery with a photo; no need to send it back.

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The physics

Meet Warmohm, a coil of wire who resists current more and more as he heats up.

In a metal, current is carried by free electrons. As the metal gets hotter, its atoms vibrate harder and the electrons bump into them more often. So the resistance rises with temperature.

Over a moderate range the rise is close to a straight line, R = R₀(1 + αΔT), where α is the temperature coefficient. For copper α ≈ 0.0039 per kelvin. Warming a copper wire by 100 K raises its resistance by about 39 percent.

A tungsten lamp filament is far more extreme. It runs near 2800 K and its resistance when glowing is more than ten times its value when cold. That is why old bulbs usually blew at the moment they were switched on, when a big surge of current rushed in.

Platinum resistance thermometers use this effect to measure temperature with great accuracy. Semiconductors go the other way, with a resistance that falls as they heat, and they are used as thermistors.

Equations

\[R = R_0 (1 + \alpha \Delta T)\]
Symbols
SymbolMeaningUnit
\(R\) resistance \(\mathrm{Ω}\)
\(R_0\) resistance at reference temperature \(\mathrm{Ω}\)
\(\alpha\) temperature coefficient \(\mathrm{1/K}\)
\(\Delta T\) temperature change \(\mathrm{K}\)