Statistical evaluation of low cycle durability for corrosion and heat-resistant steels welded joints materials at room and elevated temperature.
Daunys, M. ; Stulpinaite, A.
1. Introduction
Many structural components contain the zones of geometrical
parameters change, shoulders, keyways, oil holes, welded joints and
termed notches. When such elements are loaded, local stress and strain
concentrations are generated in such zones of geometrical parameters
change [1, 2]. Plastic strain in these areas appears in small material
volumes. During cyclic loading the cyclic plastic deformation in the
area of stress and strain concentrations can severely reduce the
durability of the construction. Plastic strains in these areas are
limited by adjacent elastic strained zones, therefore the conditions of
loading with limited strains in these areas are very similar.
The low cycle loading experiments are very complicated and
expensive, particular at elevated temperature because of temperature
control and stress strain curves recording. That is why the attempts to
obtain characteristics of low cycle loading from monotonous tension
curves, hardness or other parameters, but without cyclic loading are
made. Heat treatment is widely used in nuclear power equipment and other
engineering components. Under low cycle loading tempered or normalized
steels cyclically stabilized or hardened, therefore high strength steels
are cyclically softened [3].
It is very important to analyze the reliability of structures under
low cycling loading. The probabilistic methods of reliability
determination of corrosion and heat-resistant steels are analyzed in
this work. Durability calculation is based on the statistical method by
the use mechanical characteristics and low cyclic loading parameters.
The parameters of low cycle loading fatigue curves according
plastic strain [m.sub.p] and [C.sub.p] and elastic strain [m.sub.e] and
[C.sub.e] for corrosion and heat-resistant steels at room and elevated
temperatures were determined under tension compression and at symmetric (R = -1) strain limited conditions. In works [4, 5] detailed statistical
analysis showed that parameters of Coffin curves the best correlate with
modified plasticity ([[sigma].sub.u]/[[sigma].sub.y])Z , i.e. the
parameter depending on ultimate tensile and yield strengths and
reduction of the area at fracture, at room and elevated temperatures.
The relationship between the parameters of fatigue curves and mechanical
characteristics was conformed according to normal distribution. Only the
results of experiments of Kaunas University of Technology laboratory
were analyzed. In this work the results of the investigation of 55
corrosion and heat-resistant steels, 36 their weld metals at room
(20[degrees]C) and 46 corrosion steels at elevated
(250[degrees]C550[degrees]C) temperatures were selected from materials
investigated in the laboratories of Kaunas University of Technology and
other countries (Slovakia, Russia, Hungary).
2. Mechanical characteristics and low cycle fatigue curves
parameters
The low cycle fatigue characteristics of materials are significant
for estimating the reliability and durability of construction elements
during exploitation [6]. The parameters of low cycle loading with
limited strain are understood as the durability or low cycle fatigue
curves, which are composed in coordinates lg [epsilon] - lg N and lgS-
lg N according the number of cycles till crack Nc or fracture N f
appears. The durability of the material under loading with limited
strain is expressed by Coffin's equation
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII.] (1)
where [delta] is the range of plastic strain or the width of
plastic hysteresis loop; N is the number of cycles up to crack formation
or fracture; [m.sub.p] and [C.sub.p] are characteristics of the
material, which are proposed by Coffin: [m.sub.p] = 0.5 and [C.sub.p] =
0.5ln (1/(1-Z)), where Z is reduction of the area at fracture, while
S.S. Manson [8] proposed the expression [C.sub.p] = [(ln/1-Z).sup.0.6].
The hysteresis loop describes cyclic behavior of the material and
its resistance to fatigue. Under loading with limited strain, the cyclic
hardened, softened or stable materials are damaged of fatigue, because
at this loading there is no quasistatic damage. The shape of hysteresis
loop vary during the low cycle loading with limited strain for hardened
and softened materials, therefore it is proposed to calculate equivalent
plastic strain by expression [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE
IN ASCII.], 8k where kc is the number of semicycles up to crack, or to
the applied width of plastic hysteresis loop for durability kJ2 [3].
In work [3] it was proposed to change plastic deformation [delta]
in Eq. (1) by [epsilon], because the range of total strain s remains
constant at cyclic loading with limited strain therefore the durability
is proposed to be evaluated by the equation
[epsilon][N.sup.m] = C (2)
This equation, when [epsilon] >(3.0-3.5)[e.sub.pr], is correct
for the majority of materials, then, [m.sub.p] > m, [C.sub.p] > C
[3], and when s < (3.0 -3.5)[e.sub.pr] the durability greatly
increases, therefore low cycle fatigue curves are defined in this work
by the equation
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII.] (3)
where [epsilon] is total elastic plastic strain; [m.sub.e],
[C.sub.e], [m.sub.p], [C.sub.p] are parameters of low cycle fatigue
curves according toelastic and plastic strains accordingly.
3. Statistic evaluation of low cycle fatigue parameters
The corrosion and heat-resistant steels and their weld metals [4,
5] investigated in this work were divided according temperature into 2
groups: 1) at room temperature; 2) at elevated temperature. Dependences
of the parameters of low cycle fatigue curve [m.sub.p] , [C.sub.p]
according plastic strain and [m.sub.e] , [C.sub.e] according elastic
strain on modified plasticity ([[sigma].sub.u]/[[sigma].sub.y])Z for
steels at room temperature and 95% confidence interval ranges (dotted
line) to theoretic line are given in Fig. 1. Fig. 2 represent the
results of parameters [m.sub.p] , [C.sub.p] dependences on modified
plasticity for steels at elevated temperature.
[FIGURE 1 OMITTED]
Figs. 1 and 2 show that the 95% confidence interval ranges (dotted
line) to theoretic line are narrower at room temperature comparing with
the results at elevated temperature.
Rectangular diagrams of parameters [m.sub.p] for steels and their
weld metals (Fig. 3) show that the scatter interval of the results is
not wide (within limits [x.sub.min] / [x.sub.maxx]). In these diagrams
the median values [x.sub.me] for the investigated n number of materials
are also represented, which divides the scatter of the results into two
equal parts. Defined area (within quartiles limits [x.sub.0.25] /
[x.sub.0.75]) describes the 50% scatter of the middle values.
Statistical characteristics of low cycle fatigue curve parameters
[m.sub.p], [C.sub.p], [m.sub.e], [C.sub.e] according to elastic and
plastic strain at room (20[degrees]C) and elevated (250[degrees]C -
550[degrees]C) temperatures are given in Table 1. Mean values of the
parameters are similar to median values; the implication is that here
are no strongly outstanding materials. The mean values of scatter
results of parameters [m.sub.p] and [C.sub.p] according elastic and
plastic strain for corrosion and heat-resistant steels at room
temperature are greater comparing with the results at elevated
temperature, however parameters [m.sub.e] and [C.sub.e] are smaller at
room temperature than at elevated temperature.
[FIGURE 2 OMITTED]
[FIGURE 3 OMITTED]
Parameter [m.sub.p] of low cycle fatigue curves for analyzed steels
and their weld metals at room and elevated temperatures has left
skewness compared with normal distribution, while parameter [m.sub.e]
for those steels at elevated temperature has right skewness. Kurtosis coefficient shows that the results of parameters [m.sub.p] and [m.sub.e]
for corrosion and heat-resistant steels and weld metals at room and
elevated temperatures are spread wider interval comparing with normal
distribution.
Correlation analysis is statistical relation strength between
analyzed variables, which is expressed by correlation coefficient.
Pearson correlation coefficient measures the linear relation strength.
Correlation analysis is not used to determine nonlinear correlations.
When linear model is not adequate, it is necessary to use nonlinear
model.
In previous works the accomplished statistical analysis conformed
that the parameters of Coffin curves the best correlate with modified
plasticity ([[sigma].sub.u]/[[sigma].sub.y]) z at room and elevated
temperatures. The results in Table 2 confirm that the parameters of low
cycle fatigue curves me, [C.sub.e], [m.sub.p] , [C.sub.p] for steels,
their weld metals and modified plasticity
([[sigma].sub.u]/[[sigma].sub.y]) z at room and elevated temperatures
are correlated. Pearson correlation coefficient has the minimum value |-
0.402 for corrosion and heat-resistant steels coefficient [C.sub.p] at
elevated temperature and the maximum value |0.747| for those steels
coefficient [C.sub.e] at room temperature.
Analytical dependences of Coffin parameters on modified plasticity
for analyzed steels and weld metals at room and elevated temperatures
are given in Table 3. The dependences of [m.sub.p] , [C.sub.p] ,
[m.sub.e], [C.sub.e] are used for forecasting the preliminary durability
of a material by Eq. (3).
For the comparison of the results of experimental and calculated
durability by Eq. (3), which are distributed according to normal low,
there were determined such scatter limits: fourfold, ninefold,
sixteenfold. The scatter between experimental and calculated durability
results for steels and their weld metals (according analytical
dependences given in Table 3) at room and elevated temperatures is
presented in Table 4. Scatter of the results between experimental
[N.sup.exp.sub.f] and calculated [N.sup.cal.sub.f] durability for steels
at elevated (250[degrees]C - 550[degrees]C) temperature is 19% greater
than the scatter of the results at room (20[degrees]C) temperature. The
scatter of comparison results of experimental and calculated durability
for steels and their weld metals are similar at room temperature. The
comparison between their durability at room temperature is shown in Fig.
4. When [N.sup.cal.sub.f]f >10000 the relation [N.sup.cal.sub.f]
/[N.sup.exp.sub.f] is greater than 10, it means that in Table 3 proposed
analytical dependences are correct to use when [N.sup.cal.sub.f]l
<10000.
[FIGURE 4 OMITTED]
4. Conclusions
1. The mean value of parameter [m.sub.p] for corrosion
and heat-resistant steels and their weld metals at room at elevated
temperatures is greater than Coffin's suggested constant m = 0.5 .
The obtained mean value at room temperature for steels [m.sub.p]=0.791,
for weld metals [m.sub.p] = 0.608, at elevated temperature for steels
[m.sub.p] = 0.735.
2. The parameters of low cycle fatigue curves me, [C.sub.e],
[m.sub.p] , [C.sub.p] for steels and their weld metals are correlated
with modified plasticity ([[sigma].sub.u]/[[sigma].sub.y])z by linear
regression at room and elevated temperatures.
3. The scatter of the results between experimental
[N.sup.exp.sub.f] and calculated [N.sup.cal.sub.f] durability for steels
at elevated temperature is 19% greater than the scatter of the results
at room temperature. The scatter of the results between experimental and
calculated durability for steels and their weld metals are similar at
room temperature.
4. Analytical dependences of low cycle fatigue curve parameters on
modified plasticity for corrosion and heat-resistant steels and their
weld metals are enough correct to figure out the durability at room and
elevated temperatures. The scatter of the results is 2-3 times greater
than for one material experimental durability at low cycle loading.
5. Dependencies proposed in this work may be used for preliminary
durability evaluation of corrosion and heat-resistant steels and their
weld metals at low cycle loading.
Received October 11, 2008
Accepted February 11, 2009
References
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M., Stonkus, R. Strength of differently cooled cast iron subjected to
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p.18-22.
[2.] Daunys, M., Bazaras, Z., Timofeev, B.T. Low cycle fatigue of
materials in nuclear industry. -Mechanika. -Kaunas: Technologija, 2008,
Nr.5(73), p.12-17.
[3.] Daunys, M. Cycle Strength and Durability of Structures.
-Kaunas: Technologija, 2005. -286p. (in Lithuanian).
[4.] Sniuolis, R. Dependence of Low Cycle Fatigue Parameters on
Mechanical Characteristics of Structural Materials. Doctoral
dissertation.-Kaunas: 1999, -117p. (in Lithuanian).
[5.] Catalog of Data for Structural Materials of Mechanical and Low
Cycle Loading Characteristics. -Moscow. 1990.-400p. (in Russian).
[6.] Mishnaevsky, L.L. Methods of theory of complex system in
modeling of fracture: a brief review. -Engng. Fract. Mech., 1997, 56
(1), p.47-56.
[7.] Makhutov, N.A. Deformation Criterions and Strength Counting
for Construction Elements. -Moscow: Mashinostroenie, 1981.-272p. (in
Russian).
[8.] Manson, S.S. Fatigue: a complex subject - some simple
approximations. -Experimental Mechanics, 1965, v.5, No7, p.193-276.
M. Daunys *, A. Stulpinaite **
* Kaunas University of Technology, Kqstucio str. 27, 44312 Kaunas,
Lithuania, E-mail: Mykolas.Daunys@ktu.lt ** Kaunas University of
Technology, Kqstucio str. 27, 44312 Kaunas, Lithuania, E-mail:
agnes@erdves.lt
Table 1
Statistical characteristics of low cycling curves parameters
[m.sub.e], [C.sub.e], [m.sub.p], [C.sub.p] at room and elevated
temperatures
Corrosion and heat-resistant
Parameters steels at room temperature
[m.sub.p] [C.sub.p] [m.sub.e] [C.sub.e]
Number of materials 42 42 42 40
Mean value 0.791 189 0.152 2.40
Median value 0.811 212 0.137 1.81
Minimum value 0.39 4.44 0.06 0.65
Maximum value 1.12 555 0.30 6.49
Kurtosis coefficient -0.06 0.56 -0.46 0.71
Skewness coefficient -0.63 0.39 0.78 1.25
Corrosion and heat-resistant
Parameters steels at elevated temperature
[m.sub.p] [C.sub.p] [m.sub.e] [C.sub.e]
Number of materials 36 36 34 29
Mean value 0.735 154 0.200 2.58
Median value 0.798 193 0.197 2.35
Minimum value 0.36 6.05 0.11 0.83
Maximum value 1.10 347.8 0.34 5.08
Kurtosis coefficient -0.94 -1.10 -0.73 0.30
Skewness coefficient -0.38 -0.36 0.52 0.71
Weld metals of corrosion and
Parameters heat-resistant steels at room temperature
[m.sub.p] [C.sub.p] [m.sub.e] [C.sub.e]
Number of materials 25 24 23 22
Mean value 0.608 93.1 0.171 2.3
Median value 0.665 52.7 0.157 1.6
Minimum value 0.24 2.88 0.05 0.5
Maximum value 0.97 348 0.36 6.9
Kurtosis coefficient -0.50 1.16 -0.42 0.7
Skewness coefficient -0.19 1.38 0.47 1.3
Table 2
Correlation analysis of parameters [m.sub.e], [C.sub.e],
[m.sub.p], [C.sub.p] and modified plasticity ([[sigma].sub.u]/
[[sigma].sub.y]) * Z at room and elevated temperatures
Pearson correlation coefficient
Material [m.sub.p] [C.sub.p] [m.sub.e] [C.sub.e]
At room temperature
Corrosion and heat- -0.660 -0.461 0.610 0.747
resistant steels
Corrosion and heat- 0.559 0.707 0.545 0.466
resistant steels
weld metals
At elevated temperature
Corrosion and heat- -0.567 -0.402 0.501 0.436
resistant steels
Table 3
Analytical dependences of low cycle curves parameters on modified
plasticity (aujay) Z at room and elevated temperatures
At room temperature At elevated temperature
Corrosion and heat-resistant steels
[m.sub.p] = 1.00 - 0.149 [m.sub.p] = 1.08 - 0.189
([[sigma].sub.u]/[[sigma].sub.y])Z ([[sigma].sub.u]/[[sigma].sub.y])Z
[C.sub.p] = 294 - 73.8 [C.sub.p] = 266 - 60.7
([[sigma].sub.u]/[[sigma].sub.y])Z ([[sigma].sub.u]/[[sigma].sub.y])Z
[m.sub.e] = 0.073 + 0.059 [m.sub.e] = 0.105 + 0.052
([[sigma].sub.u]/[[sigma].sub.y])Z ([[sigma].sub.u]/[[sigma].sub.y])Z
[C.sub.e] = 0.260 + 1.61 [C.sub.e] = 1.44 + 0.645
([[sigma].sub.u]/[[sigma].sub.y])Z ([[sigma].sub.u]/[[sigma].sub.y])Z
Weld metals of corrosion and heat-resistant
steels at room te[m.sub.p]erature
[m.sub.p] = 0.363 + 0.244 ([[sigma].sub.u]/[[sigma].sub.y])Z
[C.sub.p] =-79.7 + 181 ([[sigma].sub.u]/[[sigma].sub.y])Z
[m.sub.e] = 0.057 + 0.114 ([[sigma].sub.u]/[[sigma].sub.y])Z
[C.sub.e] = 0.147 + 2.26 ([[sigma].sub.u]/[[sigma].sub.y])Z
Table 4
Comparison of experimental [N.sup.exp.sub.f] and calculated
[N.sup.cal.sub.f] durability for corrosion and heat-resistant steels
and their weld metals at room and elevated temperatures
Number of specimens, when scatter of
results between experimental and
calculated durability is
Total
number of fourfold ninefold
Material specimens number % number %
At room temperature
Corrosion and 449 142 32 212 47
heat-resistant
steels
Weld metals of 228 88 31 145 50
corrosion
and heat-resistant
steels
At elevated temperature
Corrosion and 362 58 16 100 28
heat-resistant
steels
Number of specimens, when scatter of
results between experimental and
calculated durability is
Total
number of sixteenfold
Material specimens number %
At room temperature
Corrosion and 449 260 58
heat-resistant
steels
Weld metals of 228 173 60
corrosion
and heat-resistant
steels
At elevated temperature
Corrosion and 362 139 39
heat-resistant
steels