Ladder

Warping — the ladder

One essay so far against this idea. A ladder is the distinct arguments that stand against one idea, and this one has room to grow.
  1. +67.0 N/mm²−67.0 N/mm²+67.0 N/mm²−67.0 N/mm²I-section, ω = ±12169 mm² at a tiptop flangebottom flangeh = 295V_f = 1.69 kN each way · V_f × h = 0.500 kN·m = the torque at the built-in endM_f = 3.04 kN·m each way · M_f × h = 0.897 kN·m² = the bimomentflange plan, sideways movement ×20 against the length

    The section that cannot stay flat

    Twist an I-section and its cross-section dishes out of its own plane. Stop that happening at one end and the member finds a second way to resist — the flanges bend in opposite directions — and the stress resultant that describes it has units nothing else in statics has.

    rung 1 · sections

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