12 1 Kinematical Analysis of Structures
b
c
1
2
d
1
2
a 23
5
6710
1
4 8 9
Fig. 1.13 Different ways of truss formation. For cases (a), (b), and (c) degrees of freedomWD 0 ,
for case (d)WD 1. Only case (a) may be adopted as engineering structure
Degrees of freedomWfor these cases according to formula (1.2) equal to zeros.
Indeed:
Case aWJD10; SD17; S 0 D3; so WD 2 10 17 3 D0;
Case bWJD10; SD17; S 0 D3; so WD 2 10 17 3 D0;
Case cWJD10; SD16; S 0 D4; so WD 2 10 16 4 D0:
The degrees of freedom for trusses may be calculated also by the Chebushev for-
mula. The truss in Fig.1.13a contains 17 bars, which are considered as the rigid
discs, and 3 support constraints. The number of theequivalent simple hingesH
can be calculated as follows: only two hinges are simple (joints 1 and 9) and
all other hinges are multiple. The each multiple hinge at joints 2, 3, 5, 7, 10 are
equivalent to two simple hinges; the each multiple hinge 4, 6, 8 are equivalent
to four simple hinges. Thus, the total number of equivalent simple hinges is
HD 2 1 C 5 2 C 3 4 D 24. The Chebushev formula leads to the fol-
lowing resultWD3D2HS 0 D 3 17 2 24 3 D 0. The same results
may be obtained for Cases (b) and (c).
Even ifWD 0 for systems in Fig.1.13a–c, only system (a) may be used as en-
gineering structure. System (b) has a rigid disc (shown as solid) and geometrically
changeable right part. System (c) consists of two rigid discs, which are connected
bytwomembers 1 and 2 (while for generation of geometrically unchangeable struc-
tures two rigid discs must be connected bythreenonconcurrent members), and
therefore it is geometrically changeable system.
3.W<0. The system has redundant constraints. However, existence of redun-
dant constraints still does not mean that the structure can resist load, because the
structure can be generated incorrectly. The system in Fig.1.13d contains one re-
dundant constraint; indeed, the degrees of freedom isW D 2 10 17 4 D 1.