144 CHAPTER 5 Energy Methods
Fig.5.21
Statically indeterminate truss of Example 5.9.
in which (^) ADandvCare, respectively, the change in length of the diagonal AD and the vertical
displacement of C due to the actual loads acting on the released truss, whilea 11 ,a 12 , and so on are
flexibilitycoefficients,whichwehavepreviouslydefined.Thecalculationsaresimilartothosecarried
outinExample5.8andareshowninTable5.7.Fromthattable,
(^) AD=
∑n
j= 1
F0,jF1,j(X 1 )Lj
AE
=
−27.1
AE
(i.e.,ADincreasesinlength)
vC=
∑n
j= 1
F0,jF1,j(R 2 )Lj
AE
=
−48.11
AE
(i.e.,Cdisplaceddownwards)
a 11 =
∑n
j= 1
F1,^2 j(X 1 )Lj
AE