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and the plasticity condition is violated. The statical method can now be used to
obtain a lower bound by reducing Q until M 3 = M p , whence
M 3
Q = 4.5 M p
L
M p = 3 M p
L
and so
3 M p / L < Q ult < 4.5 M p / L .
The true collapse load can be obtained by assuming a collapse mechanism
with plastic hinges at point 3 (the point of maximum moment for the previous
mechanism) and at points 1 and 4. For this mechanism
M 1 = M 3 =− M 4 = M p ,
and so, from the second of equations 5.72,
Q ult 3.6 M p / L .
If this result is substituted into the first of equations 5.72, then
M 2 = 0.6 M p < M p ,
and so the plasticity condition is also satisfied.Thus
Q ult = 3.6 M p / L .
5.11.2.3 Graphical solution
Acollapsemechanismcanbeanalysedgraphicallybyfirstplottingtheknownfree
moment diagram (for the applied loading on a statically determinate beam), and
then the reactant bending moment diagram (for the redundant reactions) which
corresponds to the collapse mechanism.
For the built-in beam (Figure 5.38a), the free moment diagram for a simply
supported beam is shown in Figure 5.38c. It is obtained by first calculating the
left-hand reaction as
R L = ( Q × 2 L / 3 + 2 Q × L / 3 )/ L = 4 Q / 3
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