Fatigue Crack Paths 2003
Fundamental system of equations
EJmQs.
EA fl — l— G i A fl + l + r+p = 0
ds r
r ds r
G A fl + l + ¢ E@ — +Xq = 0
ds r
r ds r
[ E l d ¢ ) — G A [ d v + u + o ) + m = 0
ds
a's
r
Displacements vector
\ Exte,rnal forces vector
6 l P
on
i
Indefinite equilibrium equations
d 1 _ i L 0
i — l 0
p
is rd
N
8
ds r
u
q I —- —I 0 T
y I I i 1
v
r
ds
r ds
m
d M
Z
d (p
0
1
— i
0
i
ds
ds
T Internal forces vector
Constitutive relations
Strain vector
l
/N S: T
N EA 0 0 e T = 0 GA y X
Y
i;
‘
8 X
I < i ‘ s II y
M 0
El
/
\
Figure 2. Arch problem in the form of Tonti Diagram.
XIIIIIXI/IZ
=0
(1)
together with two differential equations: the first involving tangential displacement and
curvature, the second involving radial displacement and curvature. Then, the general
solution of such system can be expressed as follows [5]:
u: —C2+C4r & — Lcos£+ C1—C3r & — Lsin£+C4Assin£+CA
s 3 s cos——C5rs— C6r
2 A r
2 A r 2
r
I’
(2)
C31 ,
s C41
s
.
s
s
v=C1cos—+C2s1n——
s cos——C5r2
s 81H — +
r
r
r
2
r 2
. s (p : C3r2s1n;— C4r2cos;+ C5s+ C6 s
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