6.4Matrix Analysis of Pin-jointed Frameworks 179
Hence,
uj−ui=λ(uj−ui)+μ(vj−vi)
SubstitutinginEq.(6.31)andrewritinginmatrixform,wehave
Sij=
AE
L
[
λμ
ij
]{
uj−ui
vj−vi
}
(6.32)
Example 6.1
Determine the horizontal and vertical components of the deflection of node 2 and the forces in the
members of the pin-jointed framework that is shown in Fig. 6.4. The productAEis constant for all
members.
We see in this problem that nodes 1 and 3 are pinned to a fixed foundation and are therefore not
displaced.Hence,withtheglobalcoordinatesystemshown,
u 1 =v 1 =u 3 =v 3 = 0
Theexternalforcesareappliedatnode2suchthatFx,2=0,Fy,2=−W;thenodalforcesat1and3are
thenunknownreactions.
Thefirststepinthesolutionistoassemblethestiffnessmatrixforthecompleteframeworkbywriting
down the member stiffness matrices referred to the global coordinate system using Eq. (6.30). The
Fig.6.4
Pin-jointed framework of Example 6.1.