Consider the problem of the bending of a beam usually
studied in the first course on
Mechanics of Deforms. This is generally based on the following
assumptions:
- i)
- The beam is initially straight.
- ii)
- The cross-section is uniform.
- iii)
- The beam is made of a homogeneous and isotropic material which
obeys Hooke's law.
- iv)
- Plane sections remain plane.
- v)
- The beam is subjected to a pure bending moment applied at the
ends.
Under these assumptions, one can derive the formula
|
(1.3.1) |
in which is the longitudinal bending stress, the
distance from the neutral axis which passes through the centroid of the
cross-section and I the moment of inertia of the cross-section about the
neutral axis. The derivation of (1.3.1) makes no reference to other
components of stress acting at a point. Of course, if the beam were initially
curved or were one interested in finding the transverse
shear stress at a point, one would
start essentially from scratch.