NapkinCalc

Beams & Columns — Bending & Buckling

Columns — buckling, the sneaky failure

continues from lesson 3 — values defined earlier in the course stay live here

ELI5: a slender column doesn't crush — it suddenly bows out sideways at a load far below its crushing strength. Euler's formula gives that critical load P_cr = π²·E·I / L² (for pinned ends). It depends on stiffness and length squared, not on strength at all.

dcol:=30mmd_{col} := 30 mm = 30 mm a round column
Icol=πdcol464I_{col} = \frac{\pi \cdot d_{col}^{4}}{64} = 39761 mm^4 second moment for a circle
Lcol:=2mL_{col} := 2 m = 2 m column length
Pcrit:=π2EbeamIcol/Lcol2inkNP_{crit} := \pi ^2 * E_{beam} * I_{col} / L_{col}^2 in kN = 19.621 kN buckling load ≈ 19.6 kN
✓ pass Pcrit>0kNP_{crit} > 0 kN the load at which it bows out (longer column ⇒ much smaller P_crit)

Real-world hook: buckling is why a soda can crushes flat, why scaffolding is cross-braced, and why you can't hold up a load with a length of cooked spaghetti.

Where next: the track shifts from solids to energy — Thermodynamics governs engines, heat, and efficiency.