estimating the resistance of aging service-proven bridges
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Original Research Paper
Estimating the resistance of aging service-provenbridges with a Gamma process-baseddeterioration model
Cao Wang a,b,*, Kairui Feng b, Long Zhang c, Aming Zou b
a School of Civil Engineering, The University of Sydney, Sydney, NSW 2006, Australiab Department of Civil Engineering, Tsinghua University, Beijing 100084, Chinac CCCC Highway Consultants CO., Ltd., Beijing 100088, China
h i g h l i g h t s
� A method is proposed to update the resistance of aging bridges using a Gamma process-based deterioration model.
� The difference between the updated distributions of bridge resistance is discussed with different deterioration models.
� A “fully correlated” deterioration process overestimates the bridge resistance compared with a Gamma process-based model.
a r t i c l e i n f o
Article history:
Received 15 July 2018
Received in revised form
5 November 2018
Accepted 10 November 2018
Available online 12 December 2018
Keywords:
Existing aging bridges
Historical load information
Resistance updating
Gamma deterioration process
Bridge safety
* Corresponding author. School of Civil EnE-mail address: [email protected]
Peer review under responsibility of Periodichttps://doi.org/10.1016/j.jtte.2018.11.0012095-7564/© 2018 Periodical Offices of Chanaccess article under the CC BY-NC-ND licen
a b s t r a c t
The environmental or anthropogenic factors, to which the in-service bridges are subjected,
are responsible for the reduction of bridge performance, and finally lead to great service
risk for bridges and increase the probability of substantial economic losses. Probability-
based estimate of bridge resistance is an essential indicator for the bridge condition
evaluation and for optimization of bridge maintenance/repair decisions. It places an
emphasis on the proper probabilistic models of structural properties and assessment
methods. Making full use of historical service load information may improve the accuracy
of bridge performance assessment with reduced epistemic uncertainty for existing aging
bridges. In to-date analyses to update the bridge resistance with past service information,
the models of resistance deterioration have been assumed as either deterministic or fully
correlated, which may differ significantly from the realistic case. With this regard, this
paper proposes a novel method for updating the resistance of service-proven bridges with
a realistic deterioration model. The Gamma stochastic process has been suggested in the
literature to describe the probabilistic behavior of structural time-dependent resistance
and thus is adopted in this paper. An illustrative bridge is presented to demonstrate the
applicability of the proposed method. Parametric examples are conducted to investigate
the role of resistance deterioration model in the updated estimate of bridge resistance with
historical service information.
© 2018 Periodical Offices of Chang'an University. Publishing services by Elsevier B.V. on
behalf of Owner. This is an open access article under the CC BY-NC-ND license (http://
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gineering, The University(C. Wang).
al Offices of Chang'an Un
g'an University. Publishinse (http://creativecommo
of Sydney, Sydney, NSW 2006, Australia. Tel.: þ61 424003086.
iversity.
g services by Elsevier B.V. on behalf of Owner. This is an openns.org/licenses/by-nc-nd/4.0/).
J. Traffic Transp. Eng. (Engl. Ed.) 2019; 6 (1): 76e84 77
1. Introduction
The performance of in-service bridges is of great concern to
the asset owners and civil engineers in this era with a rapid
growth in public awareness of infrastructure safety.While the
serviceability goal of new-built bridges has been well accom-
plished in existing codes and standards, the operating or
environmental conditions that the in-service bridges are
exposed to may cause substantial deterioration to structural
strength and/or stiffness below the criteria as assumed for
design, impairing the bridge reliability considerably during a
subsequent service period (Ellingwood, 2005; Li and Elliing-
wood, 2007; Melchers and Beck, 2017; Vu and Stewart, 2000).
To manage the safety of a bridge (or a bridge group within a
traffic network), risk-based performance indicators are
essentially necessary to account for the uncertainties associ-
ated with bridge resistance and applied loads (Kumar and
Gardoni, 2011; Lin et al., 2015; Nowak et al., 2010; Pang and Li,
2016; Saydam et al., 2013). Probability-based assessment of
bridge resistance is a widely-used tool providing quantitative
measure of structural reliability (or probability of failure), both
immediate and long-term, subjected to future extreme events,
which is further the basis for the optimization of mainte-
nance/repair decisions regarding the bridges (Wang et al.,
2016, 2017).
Many existing analytical or predictive approaches lead to
overly conservative estimate of bridge resistance, e.g., Faber
et al. (2000), Saraf and Nowak (1998), Wipf et al. (2003),
implying the necessity of realistic analytical methods for
bridge condition assessment. Although the historical service
load is one of themajor contributors to the reduction of bridge
performance, it is still evident of the bridge resistance (load-
bearing capacity) from the viewpoint of statistics (Ellingwood,
1996; Hall, 1988; Hall and Tsai, 1989; Stewart, 1997). For
instance, for an existing bridge with a service period of T
years, the lower tail of the probabilistic distribution of current
resistance, R(T), is progressively truncated due to the fact that
R(T) is higher than any of the historically imposed loads. In
fact, the successful historical traffic load can be regarded as a
proof load test with uncertainty for an existing service-proven
bridge. In recent years, much effort has been made regarding
the safety issues of existing bridges in many engineering
practices; for instance, the weight-in-motion (WIM) systems
(Vardanega et al., 2016) have been installed on key roads. The
routine condition inspections and evaluations are carried out
to collect traffic flow data and bridge condition information.
Such observed data can be taken full use of in advancing
analysis methods to improve the estimate of bridge
resistance with reduced epistemic uncertainty.
Significant researches have been published in the past
decades regarding the updating of structural performance of
existing aging structures using historical load information.
The work by Hall (1988) was among the first to update the
resistance of existing bridges using historical service
information, which is based on the concept of Bayesian
theorem. The subsequent work by Faber et al. (2000) and
Schweckendiek (2010) also adopted this methodology to
update the reliability of service-proven structures. However,
Hall (1988) ignored the deterioration of bridge resistance
with time, and thus concluded that the updated resistance
after surviving for T years is even higher than the initial
resistance. Such conclusion becomes untenable once the
resistance deterioration is taken into consideration.
Recognizing this, Stewart et al. (Stewart and Val, 1999;
Stewart, 2001) investigated the combined effect of both prior
service loads and resistance deterioration on the reliability
of existing bridges, where the Monte Carlo simulation based
procedure was employed. In order to improve the analysis
efficiency and seek deep insights into the problem, Li et al.
(Li et al., 2015a; Li and Wang, 2015) developed explicit
methods to update the bridge resistance and reliability
estimates with historical service load. However, in the to-
date analysis methods, the models of structural resistance
deterioration have been assumed as either deterministic or
fully-correlated. These models imply that the overall
trajectory of the degradation within a reference period of
interest is determined once the deterioration type and the
deterioration scenario at a specific time are provided. In fact,
the resistance deterioration is unavoidably associated with
uncertainties and it is a non-increasing stochastic process
by nature with the exclusion of rehabilitation or other types
of strengthening. Thus, in the probability-based bridge
performance assessment, a reasonable resistance
deterioration model plays a vital role. It is expected to
ensure that both the temporal autocorrelation and the
variability in the degradation process are properly taken into
account. The Gamma process has been employed in many
researches to model the resistance degradation, e.g., Li et al.
(2015b), Dieulle et al. (2003), Saassouh et al. (2007), Wang
et al. (2015), and thus it is employed in this paper to describe
the probabilistic behavior of time-variant resistance.
The aim of this paper is to investigate the updated resis-
tance of aging service-proven bridges by modeling the resis-
tance deterioration as a Gamma process-based stochastic
process. This paper is organized as follows. After the intro-
duction part in Section 1, the Gamma deteriorationmodel and
the reliability analysis method are briefly introduced in
Section 2, followed by the proposed method for the updating
of bridge resistance in Section 3. Illustrative examples are
presented in Section 4 to demonstrate the applicability of
the proposed method and to investigate the role of
deterioration model in the updated estimate of structural
performance and finally conclusions are formulated in
Section 5.
2. Deterioration model and reliabilityanalysis
The degradation of structural resistance may be posed by
construction defects, severe operating or environmental
conditions or applied loads (Pipinato, 2016). For an aging
bridge, the time-variant resistance changes in time
according to Eq. (1), where R(t) is the resistance at time t; R0
is the initial resistance (a random variable) and D(t) denotes
the deterioration function (a stochastic process). In this
paper, R0 is assumed statistically independent of D(t).
Fig. 1 e Sample degradation curves. (a) Gamma deterioration process. (b) Fully correlated process.
J. Traffic Transp. Eng. (Engl. Ed.) 2019; 6 (1): 76e8478
RðtÞ ¼ R0½1� DðtÞ� (1)
In order to reflect the stochastic characteristic of resistance
deterioration, the deterioration function, D(t), is modeled as a
Gamma process, denoted by G(t). Mathematically, if a random
variable,X, followsGammadistributionwith shape parameter
a> 0 and scale parameter b > 0, thenX is written asX ~ Ga (a, b)
and the probability density function (PDF) of X takes the form
of
fXðxÞ ¼ ðx=bÞa�1
bGðaÞ expð�x=bÞ x � 0 (2)
where Gð,Þ denotes the Gamma function, GðuÞ ¼ R∞0 su�1e�sds.
The mean value and variance of X are respectively ab and ab2.
Further, a stochastic process, {X(t), t > 0} is deemed as a
Gamma process if (1) Pr[X (0) ¼ 1] ¼ 1, where Pr($) denotes the
probability of the event in the bracket, and (2) X(t) has inde-
pendent increments and each increment follows Gamma
distribution with an identical scale parameter.
Now we consider the modeling of deterioration process,
G(t). At the end of t years, suppose that the time-variant mean
value and variance of G(t) are respectively m(t) and v(t). Obvi-
ously,m(t) and v(t) are not independent due to the shared scale
parameter of the Gamma process increments. If the shape
parameter and the scale parameter of the deterioration
function increment within time interval (t, t þ dt] are respec-
tively a(t) and b, where dt/0, then
8>>>>>><>>>>>>:
mðtÞ ¼ bZ t
0
aðtÞdt
vðtÞ ¼ b2
Z t
0
aðtÞdt ¼ bmðtÞ(3)
The function m(t) takes the form of
mðtÞ ¼ kta (4)
where k is a constant reflecting the deterioration rate, while a
is a parameter representing the deterioration shape, which
can be determined according to the dominant deterioration
mechanism of interest. For instance, a is 1, 2 and 0.5 corre-
sponding to deteriorations due to corrosion of reinforcement,
sulfate attack and diffusion-controlled aging respectively
(Mori and Ellingwood, 1993). The parameters defining the
stochastic degradation process, b, k and a can be calibrated
by regression analysis of observed data.
Since G(t) has independent increments, the auto-covari-
ance of G(t) at two different time instants, ti and tj (j > i), is
obtained as
Covar�GðtiÞ;G
�tj�� ¼ Var½GðtiÞ� (5)
where Var($) represents the variance of the variable in the
bracket. Further, the linear correlation coefficient of G (ti) and
G (tj), ri,j, is
ri;j ¼Var½GðtiÞ�ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
Var½GðtiÞ�Var�G�tj��q ¼
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffibmðtiÞbm�tj�
s¼
ffiffiffiffitaitaj
s(6)
Eq. (6) indicates that the correlation between G (ti) and G (tj)
increases when the time lag between ti and tj becomes larger
and vice versa. By noting the fact that ri,j is constantly equal
to 1 for the case of fully-correlated deterioration process, it
is seen from Eq. (6) that for the case of Gamma process-
based deterioration, the resistances of an aging bridge at
different times are positively but not fully correlated,
implying that a bridge with slight deterioration at the early
stage of the reference period may still degrade severely at
the latter stage although it has a greater possibility of “good
performance” within the whole service period.
In order to illustrate the behavior of the Gamma deterio-
ration process, Monte Carlo simulations are performed for
b ¼ 0.01, k ¼ 0.0075 and a ¼ 1, and samples of the resulting
degradation curves are presented in Fig. 1. In order to sample a
degradation process within time interval (0, T], we first
discretize this interval into j identical sections with the
maximum duration of the j sections being sufficiently small,
with which the sampling procedure for each simulation run
is as follows:
(1) For i ¼ 1, 2, /, j, sample the resistance deterioration
within the ith interval, di, which is a Gamma random
variable with shape and scale parameters being kata�1Tbj
and b respectively.
(2) Set G
�iTj
�¼Pi
k¼1dk i ¼ 1; 2;/; j.
For the purpose of comparison, the samples of fully
correlated deterioration process are also simulated and pre-
sented in Fig. 1. The fully correlated process means that a
structure with “good” performance at the early stage (i.e.,
J. Traffic Transp. Eng. (Engl. Ed.) 2019; 6 (1): 76e84 79
minor degradation) is predetermined to behave well within
the whole service period. However, it is not realistic in many
cases, in which the significant deterioration may still occur
at the latter stage. The variability and temporal
autocorrelation can be better reflected by the Gamma
process-based deterioration model.
Within the considered time interval (0, T], significant load
events that essentially affect structural safety occur randomly
in time with random intensities. Supposing that the duration
of each load event is sufficiently small so that the loads only
occupy a small fraction of the whole service life, and there is
no dynamic response, we can use a sequence of randomly
occurring pulses with random intensities to model the load
events, say, S1, S2, /, Sn at times t1, t2, /, tn, as illustrated in
Fig. 2. In this paper, the load events are assumed independent
of each other. The reliability over this reference period, L(T), is
defined as
LðTÞ ¼ PrfRðt1Þ>S1∩Rðt2Þ> S2∩/∩RðtnÞ>Sng (7)
Let Gi denote the resistance deterioration within time in-
terval (ti-1, ti], i.e., G(ti) e G(ti-1), and then
LðTÞ ¼ Pr
(∩n
i¼1
"R0
1�
Xi
k¼1
Gk
!>Si
#)(8)
Note that the number of load events, N, is also a random
variable, and thus Eq. (8) is indeed a conditional probability
given N ¼ n. Employing the Poisson process to model the
occurrence of loads, then
PrðN ¼ nÞ ¼ ðlTÞn expð�lTÞn!
n ¼ 0;1; 2;/ (9)
where l is the mean occurrence rate of the loads.
3. Resistance of service-proven structures
If an existing bridge is subjected to a proof load test, then the
PDF of the bridge resistance is simply truncated at this known
load effect (Fujino and Lind, 1977). Treating the service loads
as proof loads with uncertainties, the bridge resistance and
reliability for subsequent service years can be updated with
the historical load information. In the pioneering study by
Hall (1988), assuming that no resistance deterioration occurs
Fig. 2 e Stochastic processes of resistance deterioration
and loads.
during the past time interval (0, T], the updated PDF of
current bridge resistance, f 'RðrÞ, is obtained as
f 'RðrÞ ¼fRðrÞFSðrÞZ ∞
0
fRðrÞFSðrÞdr(10)
where FS($) is cumulative density function (CDF) of the
maximum load effect experienced up to time T, and fR ($) is the
PDF of prior estimate of bridge resistance. It is noticed that the
initial and current resistances are not distinguished in Eq. (10)
since the resistance deterioration is ignored.
Now consider the case where the bridge resistance de-
grades with time during the past service period. If the PDFs of
the initial resistance R0 and the deterioration function G(T) are
known as fR0 ðrÞ and fGðrÞ respectively, prior to the load infor-
mation, the probabilistic distribution of current
resistance, R(T), can be determined according to Eq. (11)
under the assumption of independent R0 and G(T) (Li and
Wang, 2015).
fRðTÞðrÞ ¼Z∞0
fR0ðtÞfG
1� r
t
1tdt (11)
Taking into account the past service information, the
updated PDF of R(T), f 'RðTÞðrÞ, is determined by
f 'RðTÞðrÞ ¼ limdr/0
1dr
Pr½ðr � RðTÞ< rþ drÞjA�
¼ limdr/0
1dr
Pr½ðr � RðTÞ< rþ drÞ∩A�PrðAÞ (12)
where A represents a successful performance (survival) of the
bridge within time period (0, T]. Modeling the resistance
degradation as a Gamma process, the denominator of Eq. (12),
Pr(A), is estimated according to Eq. (8) as
PrðAÞ ¼ Pr
(∩N
i¼1
"R0
1�
Xi
k¼1
Gk
!> Si
#)(13)
while the numerator of Eq. (12) is
Pr½ðr � RðTÞ< rþ drÞ∩A� ¼ Pr
(∩
Nþ1
i¼1
"R0
1�
Xi
k¼1
Gk
!>Sð1Þ
i
#)
� Pr
(∩
Nþ1
i¼1
"R0
1�
Xi
k¼1
Gk
!>Sð2Þ
i
#)(14)
where Sð1Þi ¼ Sð2Þ
i ¼ Si for i ¼ 1, 2, /, N; Sð1ÞNþ1 ¼ r; Sð2Þ
Nþ1 ¼ rþ dr,
and GNþ1 is the resistance deterioration within time interval
(tN, T], i.e., G(T) e G (tN).
A purely analytical solution would have existed if the es-
timates of the probabilities in Eqs. (13) and (14) can be solved
numerically. However, multiple-fold integral is involved in
Eqs. (13) and (14) so that it is difficult to find the numerical
solution in practice. Therefore, we adopt a simulation-based
approach herein to estimate the posterior PDF of current
resistance. The procedure for each simulation run is
illustrated in Fig. 3. Note that the service load information can
also be used to update the estimates of initial
resistance, thus the updated PDF of R0 is also obtained in the
simulation.
Fig. 4 e Girder section of Qingfang Bridge (unit: mm) (Li and
Wang, 2015).
J. Traffic Transp. Eng. (Engl. Ed.) 2019; 6 (1): 76e8480
4. Illustrative examples
4.1. Structural configuration
The Qingfang Bridge as illustrated in Li and Wang (2015) is
adopted in this paper to demonstrate the application of the
proposed updating method and to investigate the role of
deterioration model in the updated estimate of bridge
resistance. This bridge, with a service age of 22 years, is
located in a coastal city in China; as a result, its dominant
deterioration mechanism is chloride-induced corrosion of
the steel bar, which is regarded independent of the load
process. Since the bridge is a simply supported RC beam
bridge, we focus on the bending moment capacity
(resistance) of the girder, whose section is given in Fig. 4.
The probabilistic models of material properties and
geometric variables are listed in Table 1, from which the
mean value and standard deviation of the initial resistance
are determined respectively as 4022 and 479 kN$m based on
Monte Carlo simulation. A condition inspection at the end of
22 years revealed that the mean value of G(22) is 0.35. As
there is no evidence on the variability of the deterioration
function, we assume that the coefficient of variation (COV,
defined as the ratio of standard deviation to the mean value)
of G(22) equals 0.25. The total bridge load consists of the
dead load and the truck live load. The mean occurrence rate
of the live load is set equal to 1/year, and the load process is
assumed to be stationary for the purpose of simplicity.
4.2. Application of the proposed method
The updated distributions of initial resistance (R0) and current
resistance (R(22)) are obtained using 100,000 simulation runs
Fig. 3 e Flow chart to simulate the updated PDFs of R(T) and
R0.
and are plotted in Fig. 5, where the deterioration type is
assumed linear (i.e., a ¼ 1 in Eq. (4)). The influence of
historical service load on the estimates of bridge resistances
is obvious. For instance, the mean values of R0 and R(22)
increase from 4022 kN$m and 2614 kN$m to 4061 kN$m and
2676 kN$m respectively, while the COV of R0 and R(22)
decrease from 0.1191 and 0.1801 to 0.1149 and 0.1615
accordingly.
4.3. Updated bridge resistances with differentdeterioration models
In order to investigate the effect of deteriorationmodel choice
(i.e., the fully correlated and Gamma process-based models)
on the updated distribution of initial and current resistances
for bridges subjected to different service conditions, three
deterioration mechanisms (i.e., linear, parabolic and square-
root, c.f. Eq. (4)) and two load models as presented in Table 2
are considered in the parametric examples.
The updated PDFs of the bridge initial and current re-
sistances using the Gamma process-based deterioration
model are presented in Figs. 6 and 7, where the resistance
deterioration type is assumed linear, and the service load
models in Table 2 are considered. For all cases, the lower tail of
the resistance distribution is truncated as a result of the
Table 1 e Statistical descriptions of bridge resistance andloads.
Items Variable Mean Standard deviation Distribution
Model x 1.05 0.11 Normal
Geometry b (mm) 2200 82 Normal
d (mm) 1350 44 Normal
AS (mm2) 8042 / Deterministic
Material fy (MPa) 375 38 Normal
f 'c (MPa) 28.5 6 Lognormal
Load* D (kN$m) 1.05Dn / Deterministic
L (kN$m) 0.46Ln 0.18Ln Extreme type I
Note: * Dn and Ln are the nominal dead load and live load respec-
tively, Dn ¼ 1113 kN$m, and Ln ¼ 1215 kN$m.
Fig. 5 e Prior and updated PDFs of bridge resistances. (a) R0. (b) R(22).
Table 2 e Summarization of live load models.
Load model Mean Standard deviation Distribution
Service load 1 (SL1) 0.46Ln 0.18Ln Extreme type I
Service load 2 (SL2) 0.60Ln 0.18Ln Extreme type I
J. Traffic Transp. Eng. (Engl. Ed.) 2019; 6 (1): 76e84 81
failure of some deficient bridges caused by the service loads,
and this truncation is enhanced by greater load intensity.
From the comparison of Figs. 6 and 7, it is seen that the
impact of load history on the updated distribution is more
significant for the current resistance. This is because the
service load is used to update both the initial resistance and
the deterioration process, and the combined effect is
reflected in the updated distribution of R(22). For the purpose
of comparison, the updated distributions of initial and
current resistances using the fully-correlated deterioration
Fig. 6 e Updated PDFs of R0 with different
Fig. 7 e Updated PDFs of R(22) with differen
model are also calculated and are presented in Figs. 6 and 7,
and the updated mean value and COV of R0 and R(22) are
listed in Tables 3 and 4. It is seen that the difference
between the updated distributions of R0 associated with
both deterioration models is negligible. This is because the
Gamma process and fully correlated deterioration processes
result in close estimates of reliability in the past service
period (Li et al., 2015b), and the truncation of the lower tail is
caused by the “failure” of the bridges. The influence of
deterioration model choice on the updated distribution is
more significant for R(22). The updated mean value of R(22)
associated with the fully correlated process is greater than
that associated with the Gamma deterioration model,
indicating that the estimate of current resistance may be
overestimated with the fully correlated deterioration model.
This observation can be explained by the fact of the
approximately identical probability of structural failure
deterioration models. (a) SL1. (b) SL2.
t deterioration models. (a) SL1. (b) SL2.
Table 3 e Updatedmean value and COV of R0 for differentservice loads.
Servicemodel
Statistics Prior Updated
Gammaprocess model
Fully-correlatedmodel
SL1 Mean (kN$m) 4022 4061 4050
COV 0.1191 0.1149 0.1160
SL2 Mean (kN$m) 4022 4085 4077
COV 0.1191 0.1124 0.1132
Table 4 e Updated mean value and COV of R(22) fordifferent service loads.
Servicemodel
Statistics Prior Updated
Gammaprocess model
Fully-correlatedmodel
SL1 Mean (kN$m) 2614 2676 2727
COV 0.1801 0.1615 0.1614
SL2 Mean (kN$m) 2614 2715 2763
COV 0.1801 0.1523 0.1536
J. Traffic Transp. Eng. (Engl. Ed.) 2019; 6 (1): 76e8482
probability (i.e., the probability that the sampled resistance is
not recorded). Compared with the Gamma process-based
deterioration, with which the bridges with low current
resistance may have a relatively high resistance at the early
stage during the service period, the fully correlated
deterioration model enables that the sampled bridges with
Fig. 8 e Updated PDFs of R0 with different deterioration model
Fig. 9 e Updated PDFs of R(22) with different deterioration mode
low current resistance have greater probability of failure
(smaller probability of record) because the performance of
these bridges during the overall service period is always
“weak” (i.e., with severe deterioration).
In order to investigate the effect of deterioration type on
the difference between the updated resistance distributions
associated with different deterioration models, Figs. 8 and 9
show the updated PDFs of initial and current resistances
assuming square root and parabolic deterioration models,
where the live load intensity is 0.6Ln for all cases. The updated
mean value and COV of R0 and R(22) are presented in Tables 5
and 6. It is seen that the difference between the updated dis-
tributions of R0 associated with both deterioration models is
as before slight, indicating that one may employ either dete-
rioration model to update the estimate of initial resistance
with negligible error. Comparing Figs. 7(b) and 9, it is seen that
the parabolic deterioration model leads to the greatest dif-
ference between the updated distribution of R(22) using the
two deterioration models, followed by those associated with
the linear and square root deterioration types. This is because
with the parabolic model, the resistance deterioration occurs
mainly at the latter stage of the service life, and as a result the
truncation of the lower tail caused by the structural failure
also occurs at the latter stage. Thus, the fully-correlated
deterioration model unavoidably overestimates the estimate
of current resistance, and this overestimation is enhanced
with the parabolic deterioration mechanism. As a result, it is
more important to choose a proper resistance deterioration
model to update the bridge resistance for the cases where the
dominant deterioration mechanism is parabolic, such as the
RC bridges subjected to sulfate attack.
s. (a) Square root deterioration. (b) Parabolic deterioration.
ls. (a) Square root deterioration. (b) Parabolic deterioration.
Table 5 e Updatedmean value and COV of R0 for differentdeterioration mechanisms.
Servicemodel
Statistics Prior Updated
Gammaprocess model
Fully-correlatedmodel
Square
root
Mean (kN$m) 4022 4108 4099
COV 0.1191 0.1112 0.1113
Parabolic Mean (kN$m) 4022 4068 4054
COV 0.1191 0.1144 0.1151
Table 6 e Updated mean value and COV of R(22) fordifferent deterioration mechanisms.
Servicemodel
Statistics Prior Updated
Gammaprocess model
Fully-correlatedmodel
Square
root
Mean (kN$m) 2614 2747 2766
COV 0.1801 0.1458 0.1465
Parabolic Mean (kN$m) 2614 2685 2789
COV 0.1801 0.1597 0.1604
J. Traffic Transp. Eng. (Engl. Ed.) 2019; 6 (1): 76e84 83
Finally, it is noted that the proposed updating method in
this paper is based on the assumption of independent resis-
tance deterioration and loading processes, implying that the
effect of shock deterioration caused by extreme loads on the
updated resistance remains unaddressed, which deserves
more effort before the updating method becomes a practical
tool for bridge performance assessment.
5. Conclusions
A method has been developed in this paper to update the
resistance of existing aging bridges with prior service loads
employing a realistic deterioration model. For the purpose of
illustration, the proposed method is applied to an actual RC
beam bridge as suggested by Li and Wang (2015), based
on which parametrically representative examples are
conducted to show the difference between the updated
estimates of bridge resistances using different deterioration
models (i.e., the fully correlated and Gamma process-based
models). It is found that the deterioration model choice has
negligible impact on the updated estimate of bridge initial
resistance regardless of the dominant deterioration
mechanism. However, the difference between the updated
distributions of current resistance is significant posed by the
choice of deterioration model; such difference associated
with the parabolic deterioration type is largest, followed by
the linear and square root deterioration models. Moreover,
the fully correlated deterioration process may considerably
overestimate the updated mean value of current resistance
compared with the Gamma process-based model, indicating
that the unexpected risk will be induced in the probability-
based maintenance decisions if one employs the fully
correlated deterioration process.
Conflict of interest
The authors do not have any conflict of interest with other
entities or researchers.
Acknowledgments
This research has been supported by the National Natural
Science Foundation of China (Grant Nos. 51578315, 51778337),
the National Key Research and Development Program of
China (Grant No. 2016YFC0701404), and the Faculty of Engi-
neering and IT PhD Research Scholarship (SC1911) from the
University of Sydney. These supports are gratefully acknowl-
edged. The authors would like to acknowledge the thoughtful
suggestions of three anonymous reviewers, which substan-
tially improved the present paper.
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Cao Wang received his M.E. degree in July2015 from the Department of Civil Engi-neering, Tsinghua University. Currently, heis pursuing a PhD degree in the School ofCivil Engineering, The University of Sydney,Australia. His research interests includestructural reliability analysis and naturalhazards assessment.