Without adequate guiding rules and a good number
of typical examples, the conjugate beam method may likely appear as in accessible or esoteric
to many beginners. On the other hand, most beginners are pleasantly surprised to learn that there
are only two major steps in this method. The first step is to set up an additional beam, called
conjugate beam, besides the actual beam. The second step is to determine the “ shearing forces ”
and “bending moments ” in the conjugate beam using mainly concepts and skills in statics. In
the process, these two steps are most effectively guided by the set of ten rules synthesized by
Jong.
These rules are natural and logical extensions of the method using moment-area theorems.
Rule 1: The conjugate beam and the actual beam are of the same length.
Rule 2: The loading on the conjugate beam is simply the distributed elastic weight ,
which is given by the bending moment M in the actual beam divided by the flexural
rigidity EI of the actual beam. (The elastic weight , M/EI, points upward if the bending moment is
positive — to cause the top fiber in compression — in beam convention.)
For each existing support condition of the actual beam, there is a corresponding suppor
condition for the conjugate beam. The correspondence is given by rules 3 through 7 listed i
Table 1, where a simple support is either a roller support or a hinge support, since a beam i
usually not subjected to axial loads.
Ta b l e 1 Corresponding support conditi on for the conjugate beam
Existing support condition of the actual beam Corresponding support condition for the conjugate beam
Rule 3: Fixed end .................................................................Free end
Rule 4: Free end .................................................................... Fixed end
Rule 5: Simple support at the end .............................Simple support at the end
Rule 6: Simple support not at the end........................ Unsupported hinge
Rule 7: Unsupported hinge ....................................... Simple support
The slope and deflection of the actual beam are obtaine d by employing the following rules:
Rule 8: The conjugate beam (hence its free body) is in static equilibrium.
Rule 9: The slope of (the centerline of ) the actual beam at any cross section is given by
the “shearing force” at that cross section of the conjugate beam. (This slope is positive, or
counterclockwise, if the “shearing force” is positive — tending to rotate the beam element clockwise — in
beam convention.)
Rule 10: The deflection of (the centerline of ) the actual beam at any point is given by the
“ bending moment” at that point of the conjugate beam. (This deflection is upward if the
“bending moment” is positive — tending to cause the top fiber in compression — in beam convention. )
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