Plate bending — where it appears
Named by 5 essays across 2 fields — each of them below, with the objects they name alongside it.
The section that will not keep its shape
A box girder is closed, so torsion costs it almost nothing. What an eccentric load actually does to it is something a torsion calculation contains no term for — the rectangle becomes a parallelogram, in its own plane, along the whole length of the span.
The plate that is only as big as it is thick
A base plate's design is presented as a bearing calculation: an area, a bearing strength, and a check that the pressure fits. The area in that calculation is the plate, and the plate cannot deliver it — a 20 mm plate on a 500 square reaches 43 mm past the column and the corners carry nothing at all.
The compression that stays under the flange
Put a moment on a base plate and a pressure-block calculation pushes the compression out to the plate's edge, where the lever arm to the holding-down bolts is longest. A plate that is not rigid cannot put it there. The compression stays within a few tens of millimetres of the compressed flange, the lever arm shrinks, and the bolts carry twice what the pressure block said.
A quarter of the weld takes half the pull
A beam flange welded straight on to an unstiffened column flange is checked with an effective width of 191 mm out of 250. While the joint is elastic the plate's force does not use anything like that width: 47 per cent of it goes through the 65 mm over the web, and the flange has already yielded at 30 per cent of the force the rule allows. The rule's width is a plastic width, and the full-strength weld it insists on is what lets the joint get there.
The flange bent hardest where it curls least
A curved I-beam's flange curls towards its web and is bent across its own width at the root, by a stress that rises with the curling parameter λ. A portal knee's flange is cut from plate and usually tapers, and a taper changes λ along the curve. So the obvious guess is that the transverse stress peaks where λ is largest. For a flange that only narrows, or only thins, it does. Taper it both ways and the guess fails: λ is smallest at the narrow, thin end, and that is where the flange is bent hardest, because the same force is carried there on half the steel. The force the changing width hands to the web, meanwhile, is a few newtons a square millimetre.
Named alongside it
The objects these essays reach for when they reach for this one.
Base plateBearing stressColumnEccentricityEffective areaEffective widthFoundationStress concentrationT-stubBeam on elastic foundationBox girderCantilever