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=
{F} =
=
1
2
3
0
1 1 0
1 2 1
0 1 1
u
u
u
AE
AE
109
F1x = 18000 lb
P(x) = 18000 –
(10 x) x
P(x) = 18000 – 5 x2
u(x) =
dx
u(0) = 0 = C
Analytical comparison with FEM
Element stress
Exact
(x)
3.55
Analytical solution
x = displacement
Applying the boundary conditions
(x = 0) = 0 = C
Finite element solutions
(i) One element
(2) Two elements
f1x =
112
Computer solutions
One element
NUMBER OF ELEMENTS (NELE) = 1
NUMBER OF NODES (KNODE) = 2
NUMBER OF NONZERO UPPER CO-DIAGONALS (MUD) = 5
DISPLACEMENTS X Y Z
NODE NUMBER 1 0.0000E+00 0.0000E+00 0.0000E+00
NODE NUMBER 2 0.9000E–02 0.0000E+00 0.0000E+00
STRESSES IN ELEMENTS (IN CURRENT UNITS)
FORCE (1, K) FORCE (2, K) FORCE (3, K)
0.000000E+00 0.000000E+00 0.000000E+00
ELEMENTS
K MODE (I, K) K(K) A(K)
NUMBER OF NONZERO UPPER CO-DIAGONALS (MUD) = 5
DISPLACEMENTS X Y Z
STRESSES IN ELEMENT (IN CURRENT UNITS)
ELEMENT NUMBER STRESS
1 = 0.67500E+04
Four elements
NUMBER OF ELEMENTS (NELE) = 4
NUMBER OF MODES (KNODE) = 5
NODE POINTS
K IFIX XC(K) YC(K) ZC(K)
1 1 1 1 0.000000E+00 0.000000E+00 0.000000E+00
FORCE (1, K) FORCE (2, K) FORCE (3, K)
0.000000E+00 0.000000E+00 0.000000E+00
4.500000E+03 0.000000E+00 0.000000E+00
ELEMENTS
114
NODE NUMBER 3 0.6750E–02 0.0000E+00 0.0000E+00
STRESSES IN ELEMENTS (IN CURRENT UNITS)
ELEMENT NUMBER STRESS
Analytical comparison with FEM
Analytical comparison with FEM
3.56
[k(1)] =
[k(2)] =
Global equations
1
6
2
3
0
1 1 0
(2)(30 10 ) 1 1 1 1
30 0 1 1 0
u
u
Solving Equation (2)
2 106 (2 u2) = 3000
Element stresses
(1) = [C {d} =
[– C – S C S]
3.57 Bar hanging under own weight
Two element solution
Wx =
V(x) =
Ax = P(x)
118
3.58
f1x u1 + f2x u2 =
(100 + 5 x)
(b)
2 1 1
( ) ( ) x
u x u u x
L
f1x u1 + f2x u2 =
f1x = – (16) 5 +
= 26.67 kN
= 106.67 kN total force
3.59
Exact solution
P(x) = 18000 – 300 x