Twist — where it appears
Named by 4 essays across 4 fields — each of them below, with the objects they name alongside it.
The load that moves with the twist
A beam about to buckle sideways is beginning to rotate, and everything attached to it rotates with it. A load hung from the top flange swings out over the side and drives the rotation on; the same load hung underneath swings back and stops it. Two identical beams, two different capacities, and the only difference is a height.
The torque that has nowhere to go
A curved beam on two supports splits its torsion between them, and the two halves cancel at mid-span. A curved cantilever has one end, so every increment of torque accumulates toward it — and the largest action at the root of a curved balcony is one that a straight beam does not have at all.
The eccentricity a purlin cannot avoid
A channel's shear centre is outside the material, so a load applied anywhere on the section misses it. The distance is fixed by the proportions rather than by the detailing, it is 38 mm on an ordinary purlin, and the torque it produces is not an error anybody made.
The secondary beam that twists what it holds
A secondary beam framing into a twisting primary at mid-span is the best restraint a primary can have — concentrated exactly where the twist is. It is also a load: its reaction arrives on the primary's web, off the shear centre, as a torque at exactly the same place. Which wins is decided by the connection, and the threshold is low: a fin plate stiffer than about 33 kN·m per radian, a seventieth of what still counts as a pin, makes the secondary hold far more than it twists. The bolts' free play is another matter, because the torque acts from the first millimetre and the restraint only once the play is taken up.
Named alongside it
The objects these essays reach for when they reach for this one.
Shear centreTorsionTorsional constantWarpingFree bodyRestraintServiceabilityBearingBending momentBracingCantileverCladding