Math 2.0

Mechanics of deformable solids Definition

Bending moment

Builds on Stress

Definition

Let a straight beam lie along the xx-axis, with cross-section AA in the (y,z)(y, z)-plane and centroid of AA on the axis. Let the beam bend in the (x,y)(x, y)-plane, and let σxx(x,y,z)\sigma_{xx}(x, y, z) be the normal stress on the cross-section at xx. The bending moment at xx is M(x)=∫Ay σxx(x,y,z) dy dz.M(x) = \int_A y \, \sigma_{xx}(x, y, z) \, dy \, dz. Let the beam be in equilibrium. Then M(x)M(x) equals the moment about xx of the external forces and couples on the part of the beam to one side of xx.

Remarks

Here yy points in the direction of the load, so that a moment that makes the beam sag, with tension on the side y>0y > 0, is positive. Example: a simply supported beam of length LL with a point load PP at mid-span has support reactions P/2P/2. For 0≤x≤L/20 \le x \le L/2 the forces to the left of xx are only the reaction P/2P/2 at 00, with lever arm xx, so M(x)=Px/2M(x) = Px/2. The largest value is M(L/2)=PL/4M(L/2) = PL/4.

Non-example: the integral ∫Aσxx dy dz\int_A \sigma_{xx} \, dy \, dz is the axial force, not the bending moment; it is 00 in pure bending, while MM is not.

In the Euler–Bernoulli theory the stress is σxx=−Eyw′′\sigma_{xx} = -E y w'', where ww is the deflection in the direction of yy, so M=−EIw′′M = -E I w'', where II is the second moment of area. Texts differ in the sign conventions for MM.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Bending_moment
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Changed3 November 2026

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