Crack Paths 2009
C O L D - D R A W RIENSGI D U ASLTRESSES
= ∞ d ρ ), determined by
The longitudinal residual stress data for an unnotched bar (
Elices [13] through the neutron and X-ray diffraction technique, are shown by solid
symbols in Fig. 2a, where the radial coordinate r is normalized with respect to the bar
radius
0 R (i.e.
0 R/= r*) andrthe residual stress with respect to the residual stress value
). By interpolating such data through
at the bar centre (i.e. resI σ σ best fitting polynomial, a continuous cu v is obtained (Fig. 2a). ) 0 ( = σ * ) ( ) ( = resI
) ( rresI
Such an axisymmetrical stress distribution has been used to numerically assess the
residual stress distribution in a notched bar (
= 009.0 d ρ ). The dimensionless residual
stress profile, in correspondence to the reduced section S-S, is reported in Fig. 2b (in
such a case, the dimensionless radial coordinate is given by R/ * r= ). r
A generic axysimmetrical residual stress distribution given by
)(
) ( * ) 0 (
(1)
σ
r
=
σ
r
=
⋅
σ
r
) (
) (
) (
resI
resI
resI
can be approximated through a power series expansion as follows:
B r A
dr
r
r
≅
i )(
resI
( ) r
i n
i resI
i
i n
resi
i
i n
resi
⎜ ⎜ ⎝ ⎛
⎟ ⎟ ⎠ ⎞
i d 1 σ
) (
i
() r
σ
⋅ =
∑ ∑ = = ⋅ = 0
⋅
∑ =
*)(
(2)
) (
!
) (
0
)(
0
0 ) (
r =
where *r is given by Rr/ (R is equal to
0 R for unnotched bar and to R for notched
are expressed by the following equation:
bar), and the coefficients
)(resiB
(3)
σ
B
i Ri d
dr
dr
B
resi
resi
i
i
⎢⎣⎡
⎟ ⎟ ⎞
⎤
/ *
⎜ ⎜ ⎝ ⎛
σ
σ
B
R i d
r
=
⋅
[
]
=
*
=
!
) (
* ) 0 (
!1
i
resI
r
=
with
)( ) ( resI
) (
=
)(
)(
0
⎥
) (
i
r
r e s i r e s I
⎥ ⎦
⎠
) ( ) (
)(
0
01.82
3.2
(a)
(b)
0.0 0.2 0.4 0.6 0.8 1.0
ρd =
ρd = 0.009
2.4
0.4
1.6
0.0
0.8
-0.4
0.0
-0.8
-0.8
-1.6
0.0 0.2 0.4 0.6 0.8 1.0 D I M E N S I O N L E S S R A D I A L C O O R D I N A T E , r* -1.2
D I M E N S I O N L E S S
R A D I A L C O O R D I N A T E , r*
Figure. 2. Dimensionless residual stress distribution
against dimensionless radial
σ
*
resI
) (
coordinate r * : (a) unnotched round bar; (b) notched round bar.
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