Joint equilibrium — where it appears
Named by 2 essays across 2 fields — each of them below, with the objects they name alongside it.
The cut that needs a joint first
The method of sections works because a cut through three members leaves three unknowns and a point about which two of them have no moment. A K-braced tower has no such cut anywhere: every section severs two legs and two diagonals. One joint in the middle of a horizontal supplies the missing equation, and only in that order does each step have one unknown — after which the diagonals turn out to be carrying not the shear but the moment about the point where the legs would meet.
The panel that gravity leaves empty
A corner joint's panel carries the difference between a beam's flange couple and half a column's shear, and full gravity load is what makes that large. An interior joint has a beam on each side, and under full gravity their two couples cancel: the panel between them carries nothing at all, in the load case that sizes every member around it. It fills under the two loads that are not symmetric. A pattern load hands it one beam's moment, and sway hands it two beams' moments turning the same way. Together they put more shear through it than through any exterior joint, in a combination that governs no member.
Named alongside it
The objects these essays reach for when they reach for this one.
Bending momentDeterminacyEquilibriumFlange coupleFree bodyLattice towerLoad combinationMethod of sectionsMoment centrePanel zonePattern loadingPortal frame