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Geometry beats material — page 5

Essays 97 to 100 of 100 on this thread, in the same order.
18 kN/m18 kN/mN = 9.3 kN/m1190 Pa121 mm of water60 mtotal uplift 3365 kNworst membrane force when the snow melts Structural form

Held up by the air inside

A membrane has no bending stiffness at all, so the only thing that can hold it in tension is a pressure difference. The pressure needed to hold up a roof is smaller than the pressure a closed door makes — and the same pressure arrives at the foundation as hundreds of tonnes of uplift.

a12.12 kNb12.12 kNc5.02 kNd6.86 kNe6.86 kNf9.61 kNgoverning: mode c · 5.02 kN per shear plane Connections

The smallest of six failures

Everything else in this collection that fails does so in one way at a time. A dowel through timber does not — the wood can crush while the steel stays straight, or one plastic hinge can form in it, or two — and the capacity is the smallest of the six, which is the kinematic theorem of plasticity applied to a joint rather than to a frame.

n = 20.138n = 30.367n = 40.689n = 51.102critical pressure in N/mm² · lowest is n = 2 Stability

The pressure that needs no direction

Every buckling problem in this collection has had a load with a direction — a column pushed along its axis, a plate along its edge, an arch by what is on it. A buried pipe has none. The pressure is the same everywhere, it stays normal to the wall as the wall moves, and it does work on any change of shape that reduces the area inside.

10^-410^-210^2123456strain rate (per second)strength ÷ its static valuea testing machinean earthquakea vehicle impacta blastconcrete in tensionsteel, yieldsteel, ultimatethe modulus Materials

The steel that is stronger in a millisecond

Every strength quoted anywhere in this collection was measured at about a ten-thousandth of a strain per second, because that is what a testing machine does, and nothing on a drawing says so. Load the same steel a million times faster and its yield stress rises by a third.

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