Confirm the narrow model conditions
Use only a straight prismatic doubly symmetric I beam with uniform bending moment. The moment-gradient factor is fixed at C1 = 1.
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Use this to examine the classical elastic lateral–torsional critical moment of an ideal, doubly symmetric I beam under uniform pure major-axis bending.
Use only a straight prismatic doubly symmetric I beam with uniform bending moment. The moment-gradient factor is fixed at C1 = 1.
Use the weak-axis second moment, Saint-Venant J and warping Iw in the displayed units. J is not the polar second moment of area.
Review how unbraced length changes the ideal bifurcation moment. Do not treat Mcr as an allowable working moment or a code design resistance.
E = 200,000 MPa; G = 77,000 MPa; weak-axis Iz = 8,000,000 mm⁴; J = 150,000 mm⁴; Iw = 1,000,000,000,000 mm⁶; L = 6 m.
The ideal elastic critical moment Mcr is approximately 170.640 kN·m for the stated model with C1 = 1. This is not a rated or permissible working moment.
Mcr is the elastic bifurcation value for the stated support and loading assumptions.
The unbraced length is the segment with no intermediate restraint; it need not be the complete fabricated member length.
Yielding, residual stress, initial imperfections, local buckling and load-height effects are excluded. A design-resistance calculation needs an appropriate design method beyond this result.
Substituting the polar second moment for Saint-Venant J, or applying this uniform-moment equation to an arbitrary crane girder with unspecified restraints and load height.
Mcr = (π / L) × √[E × Iz × G × J + π² × E² × Iz × Iw / L²]
Use N and mm consistently; divide N·mm by 1,000,000 for kN·m.
No. Mcr is not code resistance or an allowable moment. Imperfections, yielding, relevant factors and other failure modes need the appropriate separate design checks.
Not in this tool. It fixes C1 = 1 and ideal end fork supports with free warping. Other restraint and loading conditions need a different model.