Using a mathematical approach, this paper seeks an efficient solution to th
e problem of beams bending under singular loading conditions and having var
ious jump discontinuities. For two instances, the boundary-value problem th
at describes beam bending cannot be written in the space of classical funct
ions. In the first instance, the beam is under singular loading conditions,
such as point forces and moments, and in the second instance, the dependen
t variable(s) and its derivatives have jump discontinuities. In the most ge
neral case, we consider both instances. First, we study singular loading co
nditions and present a theorem by which the equivalent distributed force of
a general class of singular loading conditions can be found. As a conseque
nce of obtaining the equivalent distributed force of a distributed moment,
we find a mathematical explanation for the corner condition in classical pl
ate theory. While plate theory is not the focus of this paper, this explana
tion is interesting. Then beams with various jump discontinuities are consi
dered. When beams have jump discontinuities the form of the governing diffe
rential equations changes. We find the governing differential equations in
the space of generalized functions. It is shown that for Euler-Bernoulli be
ams with jump discontinuities the operator of the differential equation rem
ains unchanged, only the force term changes so that delta function and its
distributional derivatives appear within it. But for Timoshenko beams with
jump discontinuities, in addition to changes in the force terms, the operat
or of one of the governing differential equations changes. We then propose
a new method for solving these equations. This method which we term the aux
iliary beam method, is to solve the governing differential equations not in
the space of generalized functions but rather to solve them by means of so
lving equivalent boundary-value problems in the space of classical function
s. The auxiliary beam method reduces the number of differential equations a
nd at the same time obviates the need to solve these differential equations
in the space of generalized functions which can be more difficult. (C) 200
0 Elsevier Science Ltd. All rights reserved.