Advanced Methods of Structural Analysis

(Jacob Rumans) #1

11.8 Analysis of Statically Indeterminate Trusses 413


Vector displacements


ZED

2 6 6 6 6 6 6 6 6
Z 1
Z 2
Z 3
Z 4
Z 5

3 7 7 7 7 7 7 7 7

DK^1 PED

d
EA

2 6 6 6 6 6 6 6 6
2:2071
8:6594
0:2071
6:8665
1:7929

3 7 7 7 7 7 7 7 7

The negative sign forZ 1 indicates that the jointAaccordingZ-Pdiagram has a
negative displacement, i.e., downwards.
Vector of internal forces


ESD

2 6 6 6 6 6 6 6 6 6 6
S 1
S 2
S 3
S 4
S 5
S 6

3 7 7 7 7 7 7 7 7 7 7

DkAQ

TE
ZD

2 6 6 6 6 6 6 6 6 6 6
0:2071
2:2071
2:5360
3:1217
1:7929
1:7929

3 7 7 7 7 7 7 7 7 7 7

The negative sign forS 4 accordingS-ediagram means that the diagonal member 4
is compressed. The units for all internal forces are kN.
Control:ASDPE. In our case


AESD

2 6 6 6 6 6 4
0  10 0:707 0 0
0000:70710
1000:70700
00 0:707 0  10
0 0 0:707 0 0 1

3 7 7 7 7 7 5



2 6 6 6 6 6 6 6 6 6 6
0:2071
2:2071
2:5360
3:1217
1:7929
1:7929

3 7 7 7 7 7 7 7 7 7 7

D

2 6 6 6 6 6 6 6 6
0
 4
 2
0
0

3 7 7 7 7 7 7 7 7

For calculation of reaction of supports, we need to consider equilibrium condi-
tions for rolled and pinned supports. For example, the free-body diagram for pinned
supportDand corresponding equilibriumequations are shown in Fig.11.28e.


X
XD 0 !XDDS 1 C0:707S 3 D2:0kN;
X
YD 0 !YDDS 2 C0:707S 3 D4:0kN:

Of course, for thisexternallystatically determinate structure all reactions may be
determined considering the structure in whole. However, for calculation of reactions
we used typical approach as for any statically indeterminate structure.

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