Titel_SS06

(Brent) #1
In case of non-stationary Normal processes it can be shown, see e.g. Madsen et al. (1986), that
the MOR may be determined as:

(()) X ()(( ) ( ))
XX X

t

 


E --


 


(^) ,







 (8.13)


where

() () ()


()


X
X

t tt
t

 E 





 


.


In the foregoing only the simplest cases have been considered, i.e. the case of scalar valued
stochastic processes where the failure domain is given as a simple one-sided boundary to the
sample space of the process. However, the presented theory may easily be generalised to
vector valued stochastic processes and also to random fields. In the specialist literature, see
e.g. Bryla et al. (1991), Faber et al. (1989) and Faber (1989) more general situations are
considered and efficient approximate solutions are given.

8.3 Approximations to the Time Variant Reliability Problem
The exact assessment of the time variant reliability problem, i.e. the first passage problem, is
hardly possible for the types of stochastic processes which are relevant for civil engineering
purposes and it is therefore necessary to approach the problem by means of approximations
and or simplifications of the considered problem.
One of the most commonly adapted approximations is to assess the probability of failure
conditional on events which may be assumed to follow a Poisson process. This could e.g. be
relevant when assessing the probability of failure in regard to earthquakes, floods, ship
impacts, explosions, fires and other rare events. In this case the reliability problem may be
assessed using the Poisson spike process model in which case the first passage problem is
readily solved using Equation (8.5).
For phenomena occurring continuously in time such as stresses in a steel structure subject to
wave loading the Poisson spike model is no longer appropriate as no particular event can be
said to be more critical than others. Failure could e.g. occur as a result of a combination of
fatigue crack growth and extreme stresses and whether the structure will fail due to instable
crack growth or plastic rupture depends on the crack geometry and the stresses at any given
time. Also in this case help may be found from the results derived from Poisson processes. It
can be shown that under certain regularity conditions, which are usually fulfilled then the
failure events will occur as realisations of a simple Poisson process in which case the result of
Equation (8.5) may readily be applied.

Non-ergodic Components and Random Sequences
Without going into details it is, however, emphasised that care should be taken when applying
the results in Equation (8.5) as the characteristics of the considered problem could lead to a
gross misuse of these. This is for engineering purposes typically the case when in addition to
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