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Bimetallic strip

Two-sided strip that coils when heated or cooled

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Through Thermal expansion, Thermometer and Steel

The invention of the bimetallic strip is generally credited to John Harrison, an eighteenth-century clockmaker who made it for his third marine chronometer (H3) of 1759 to compensate for temperature-induced changes in the balance spring. Harrison's invention is recognized in the memorial to him in Westminster Abbey, England.

Characteristics

The strip consists of two strips of different metals which expand at different rates as they are heated, usually steel and copper, or in some cases steel and brass. The strips are joined throughout their length by riveting, brazing or welding. The different expansions force the flat strip to bend one way if heated, and in the opposite direction if cooled below its initial temperature. The metal with the higher coefficient of thermal expansion is on the outer side of the curve when the strip is heated and on the inner side when cooled. The sideways displacement of the strip is much larger than the small lengthways expansion in either of the two metals.

In some applications, the bimetal strip is used in the flat form. In others, it is wrapped into a coil for compactness. The greater length of the coiled version gives improved sensitivity.

The radius of curvature R of a bimetallic strip depends on temperature T according the formula derived by French physicist Yvon Villarceau in 1863 in his research for improving the precision of clocks:

1R−1R0=32a(α2−α1)(T−T0)h=32aΔϵh,

where h=h1+h2 is the total thickness of the bimetal and a=1+(E1h12−E2h22)2/(4E1h1E2h2h2) is a dimensionless coefficient. For each metallic strip: Ei is the Young modulus, αi is the coefficient of thermal expansion and hi is the thickness. The formula can also be rewritten as a function of the thermal misfit strain Δϵ=(α2−α1)(T−T0). And if the modulus and height are similar, we simply have a≃1.

An equivalent formula can be derived from the beam theory.

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