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Beam deflection

A shelf that sags.

Load the middle of a plank and it bows — how much depends on the load, the span between supports, and the board's height cubed. Turn the same plank on its edge and that one term does almost all the work.

δ = PL3 4Ebh3
Load P P ∝ δ
5 kgdouble P · double the sag100 kg
Span L L³ ∝ δ
0.3 mdouble L · 8× the sag2.4 m
Orientation h h⁻³ ∝ δ
Sag at centre
mm
code limit, L/360
Try

For a simply supported beam with a load at its centre, beam deflection theory gives δ = PL³/(48EI), where I = bh³/12 is the cross-section's second moment of area — substituting that in leaves δ = PL³/(4Ebh³), which is the form shown above so the h³ is visible directly rather than hidden inside I. The board is a standard "2×6" stud, actual dimensions 38×140 mm, in spruce–pine–fir framing lumber (E = 9.65 GPa, the No. 2 grade design value). Turning it on edge swaps which dimension is h and which is b, making it about 13.6× stiffer — not because the wood changed, but because the equation's cubed term did. The gauge's limit line is L/360, a deflection commonly used in building codes as a serviceability limit for many spans. Only elastic bending is modelled: at the sliders' extreme corner (longest span, heaviest load, flat) the formula predicts several centimetres of sag, but a real board that thin would almost certainly crack or fail outright long before bending that far — the equation doesn't know that, so treat results far past the limit line as "this shape is a bad idea," not a literal prediction.