It can be stated as follows: If a set of self-equilibrating loads
are applied on a body over an area of characteristic dimension
d, the internal stresses resulting from these loads are
only significant over a portion of the body of approximate
characteristic dimension d. Note that this principle is
rather vague, as it deals with 'approximate' characteristic
dimensions. It allows qualitative rather that quantitative
conclusions to be drawn. An important application of
Saint-Venant's principle deal with end effects in bars and
beams.