Bending Members (Beams) under Pure Bending (Couples)          

 

Typical bending members are straight and long with a pure bending couple, M .  The figure

below shows various cross-sectional possibilities all of which are symmetrical about the y-axis.

            

 

In a Nut Shell:  Normal Stress in a Bending Member (Beam)  (Bending Stress)

 

Under the assumption that plane sections before bending remain plane afterwards it can be

shown that the curvature of the beam (1/ρ) is directly proportional to the couple (bending

moment) and inversely proportional to the flexural rigidity (EI) of the beam where E is the

modulus of elasticity and  Izz  is the moment of inertia of the entire cross-sectional area about

the centroidal (neutral) axis.

 

        Curvature  =  1/ρ  =  M / EIzz

 

 

In addition the strain at a distance, y, above the centroidal (neutral) axis is

           

 

                          εx  =   - y/ρ 

 

So                   εx  =   - My/EIzz  =  - My/EI 

 

 

For linear elastic response                σx  =  E εx                (Hooke’s Law)                

                            

and substituting the expression for  εx  the “bending stress”  becomes     σx  =   - My/I 

 

If   c   is the maximum distance to the “outer” fiber of the beam, then the maximum

bending stress is

                                                         σm =  Mc / I

 

Common units for stress are  psi,  ksi,    MPa, N/mm2  (English/Metric)

 

Click here for a discussion of strategy in the analysis of bending stresses in beams.

 

 

    Click here for examples.

 


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