I-section
The material far from the middle does nearly all the work
A strip of steel contributes to bending stiffness in proportion to the square of its distance from the centre. Move the same steel outward and the section gets stiffer for nothing.
The same steel in a different shape, and a factor of forty
Four sections of identical area, identical weight and identical cost. The stiffest is dozens of times the stiffest of the flattest, and the only thing that changed was the arrangement.
The shear nobody draws
A stack of loose planks slides at its ends when it is loaded. Glue them and the sliding stops — and whatever the glue is now carrying is a stress that no bending calculation contains.
The point that is not in the section
A channel loaded down its web twists. To stop it, the load must be applied through a point outside the steel entirely — in the air beside the section, where nothing can be attached.
Named alongside it
The objects these essays reach for when they reach for this one.
Neutral axisSecond moment of areaShear flowTorsionCentroidDelaminationEccentricityFirst moment of areaHollow sectionLocal bucklingOpen sectionParallel axis theorem