Chapter 4 Optimum Design Concepts
4.153_______________________________________________________________________________
For the three-bar truss problem of Exercise 4.150, consider the case of KKT conditions with g2 as
the only active constraint. Solve the conditions for optimum solution and determine the range for
the load angle θ for which the solution is valid.
Solution
Ref. to Exercise 4.150, the KKT conditions for the case
( )
2 2 1 34
g 0 0 and 0s u uu= = = = =
,
are
( )
2
1 2 12
22 2 2 0
v
Lx u P x x
∂∂= + − + =
(1)
( )
2
2 2 12
12 2 0
v
Lx u P x x
∂∂ =+ − + =
(2)
( )
2 1 2 2 12
g 2 2 20,000 0, 0, , 0
v
P x x u xx= +− =≥ ≥
(3)
From (1), u2 =
; From (2),
( )
2
21 2
22
v
ux x P= +
. These two equations are
inconsistent, so there is no solution in this case.
4.154_______________________________________________________________________________
For the three-bar truss problem of Exercise 4.150, consider the case of KKT conditions with g1
and g4 as active constraints. Solve the conditions for optimum solution and determine the range for
the load angle θ for which the solution is valid.
Solution
Referring to Exercise 4.150, we write the KKT conditions for this case,
( )
1 4 14 2 3
g g 0 0 and 0,ss uu= = = = = =
as
( )
2
2
1 1 1 12
22 2 2 2 0
uv
Lx u P x P x x
∂∂= + − − + =
(1)
( )
2
2 1 124
1 20
v
Lx u P x x u
∂∂ =+ − + − =
(2)
( ) ( )
( )
1 1 12
g 1 2 2 20,000 0
uv
Px Px x
= ++ − =
(3)
4 2 12 1
g 0; , 0, 0x uu x== ≥≥
(4)
( )
( )
22
1 1 1 14
2 2 2 0; 1 0
uv v
u P P x uPx u
+ −− = − − =
( )
( )
( )
1
1 2 20,000 0
uv
PPx+−=
From the last equation, we get
( )
( )
2000,20
1vu PPx +=
.
Substituting
into the previous two equations and solving for
and
, we obtain
( )
( )
8
1
2 10 ,
uv
u PP=+×
( ) ( )
vuvu
PPPPu +−= 3
4
.
Now
requires that
which is equivalent to tan
, or
18.43°.