The Textbook of Architecture

Rules · Structure · Materials · Doors & windows

A stone lintel’s span is limited by its tension

A beam is squeezed along its top and stretched along its bottom; stone resists squeezing well but stretching badly, so a stone lintel must be deep in proportion to its span and cannot be long. Doubling the span quadruples the stress from its own weight.

σ ≈ ¾ ρ g L² ⁄ d (self-weight) · + ≈ 0.43 ρ g L³ ⁄ d² (a wall above)

Drag the span: the stress rises with its square. Add a wall above and it rises faster still. Open in Models ↗

A simply supported beam of span L and depth d carrying its own weight develops a bending stress at mid-span proportional to L²⁄d: make the lintel twice as long and it must be twice as deep merely to stay as safe. If a wall stands on it, the load itself grows with the span and the stress grows roughly with L³⁄d². Meanwhile the tensile strength of stone is only a few megapascals and varies from block to block with hidden flaws and bedding planes, so builders kept a large margin.

The result is visible everywhere in trabeated architecture. Clear spans between Egyptian and Greek columns are rarely more than three or four metres; the widest stone spans of antiquity, such as the central aisle of the Karnak hypostyle or the Propylaia at Athens, were achieved with deep, carefully chosen blocks, and some Greek architraves were secretly helped by iron bars. The model computes an indicative stress for the chosen span, depth and stone (indicative strengths with a factor of safety of three); raise the span and watch the lintel crack.

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Cite this page Chris Paton, “A stone lintel’s span is limited by its tension”, The Textbook of Architecture, https://textbookofarchitecture.com/rule/lintel-span-depth. Text, drawings and models licensed under CC BY-NC 4.0.