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Mathematical and Physical Properties of Reliability Models in View of their Application to Modern Power System Components

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Innovations in Power Systems Reliability

Part of the book series: Springer Series in Reliability Engineering ((RELIABILITY))

Abstract

This chapter has a twofold purpose. The first is to present an up-to-date review of the basic theoretical and practical aspects of the main reliability models, and of some models that are rarely adopted in literature, although being useful in the authors’ opinion; some very new models, or new ways to justify their adequacy, are also presented. The above aspects are illustrated from a general, methodological, viewpoint, but with an outlook to their application to power system component characterization, aiming at contributing to a rational model selection. Such selection should be based upon a full insight into the basic consequences of assuming—sometimes with insufficient information—a given model. The second purpose of this chapter, closely related to the first, is to highlight the rationale behind a proper and accurate selection of a reliability model for the above devices, namely a selection which is based on phenomenological and physical models of aging, i.e., on the probabilistic laws governing the process of stress and degradation acting on the device. This “technological” approach, which is also denoted in the recent literature as an “indirect reliability assessment” (IRA), might be in practice the only feasible in the presence of a limited amount of data, as typically occurs in the field of modern power system. Although the present contribution does not address, for reasons of brevity, the topic of model or parameter statistical estimation, which is well covered in reliability literature, we believe that the development of the IRA is perfectly coherent—from a “philosophical” point of view—with the recent success and fast-growing adoption of the Bayesian estimation methodology in reliability. This success is proved by the ever-increasing number of papers devoted to such methodology, in particular, in the field of electric and electronic engineering. Indeed, the Bayesian approach makes use of prior information, which in such kind of analyses is provided by technological information available to the engineer, and—as well known—proves to be very efficient in the presence of data scarcity. Loosely speaking, IRA is a way of using prior information not (only) for random parameter assessment, but for a rational “model assessment”. In the framework of the investigation of innovations in reliability analyses regarding modern power systems, the present chapter takes its stimulus from the observation that the modern, deregulated, electrical energy market, striving toward higher system availability at lower costs, requires an accurate reliability estimation of electrical components. As witnessed by many papers appearing on the subject in literature, this is becoming an increasingly important, as well as difficult, task. Indeed, utilities have to face on one hand the progressive aging of many power system devices and on the other hand the high-reliability of such devices, for which only a small number of lifetime values are observed. This chapter gives theoretical and practical aids for the proper selection of reliability models for power system components. First, the most adopted reliability models in the literature about electrical components are synthetically reviewed from the viewpoint of the classical “direct reliability assessment”, i.e., a reliability assessment via statistical fitting directly from in-service failure data of components. The properties of these models, as well as their practical consequences, are discussed and it is shown that direct fitting of failure data may result poor or uncertain due to the limited number of data. Thus, practical aids for reliability assessment can be given by the knowledge of the degradation mechanisms responsible for component aging and failure. Such aging and life models, when inserted in a probabilistic framework, lead to “physical reliability models” that are employed for the above-mentioned IRA: in this respect, a key role is played by “Stress-Strength” models, whose properties are discussed in detail in the chapter. While the above part is essentially methodological and might be of interest even for non-electrical devices (e.g., Stress-Strength models were originally derived in mechanical engineering), a wide range of models can be deduced in the framework of IRA, that are useful for describing the reliability of electrical components such as switchgears, insulators, cables, capacitors, transformers and rotating electrical machines. Then, since insulation is the weakest part of most electrical devices—particularly in medium voltage and high voltage systems—phenomenological and physical models are developed over the years for the estimation of insulation aging and life is illustrated in this framework. Actually, in this kind of application the prior knowledge could be very fruitfully exploited within a “Stress-Strength” model, since Stress and Strength are clearly identifiable (mostly being applied voltage and dielectric Strength, respectively) and often measurable. By means of this approach, new derivations of the log-logistic distribution and of the “Inverse power model”, widely adopted for insulation applications, are shown among the others. Finally, the chapter shows by means of numerical and graphical examples that seemingly similar reliability models can possess very different lifetime percentiles, hazard rates and conditional (or “Residual”) reliability function values (and, thus, mean residual lives). This is a very practical consequence of the model selection which is generally neglected, but should be carefully accounted for, since it involves completely different maintenance actions and costs.

Abbreviations and list of symbols: The singular and plural of names are always spelled the same. “Log” always denotes natural logarithm. Random variables are denoted by uppercase letters.

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Notes

  1. 1.

    The references at the end of the chapter are listed alphabetically, due to the length of the Bibliography, for an easier search by the reader. They are referred to in the chapter by their number.

  2. 2.

    A significant citation from C.S. Pierce comes to mind: “Probability is the only branch of mathematics in which good mathematicians frequently get results which are entirely wrong”.

  3. 3.

    Here, the term “prior” means, loosely, something not closely related to observed data, but coming from pieces of information “outside the data”, in analogy with Bayesian estimation terminology.

  4. 4.

    It should be clear, by the way, that the hrf must be positive, but not necessarily less than 1: it can even diverge, as happens for models possessing a pdf which vanishes at some finite point in time, as the Uniform model. It has little to do with a pdf, too: e.g., its integral over the whole interval (0, ∞) must be ∞, since R(∞) = 0, etc.

  5. 5.

    The notation R(t|s) is purely symbolic, being used for suggesting the conditional aspect of the RF, and should not be confused with the conditional probability P(A|B), the main difference being that (r, s) are deterministic numbers, while (A, B) are random events.

  6. 6.

    This latter would probably be a better name: here we use the term “conditional” instead of residual since it is more adopted in literature.

  7. 7.

    When discussing aging and hrf and CRF properties, in the authoritative [10] it is observed that “certain materials increase in strength as they are work-hardened” (p. 55). This may be true, but it is unlikely that it holds for very long time intervals: wear-out should ultimately prevail for any device, corresponding to a CRF R(t|s) decreasing with s, for s large enough. Anyway, it is possible that in practice the device is maintained or retired before wearing-out, so that the ultimate, decreasing part of the CRF is not observed.

  8. 8.

    The extension of the following reasoning to three-state or multi-state models is straightforward (e.g., a three-state model occurs in power distribution studies when also “extremely adverse” weather conditions, or similar, are considered [156].

  9. 9.

    Mistaking (18) for (17) is in practice equivalent to mistaking—as to the computation of the expectation of a function ϕ of a RV X– the expectation E[ϕ(X)] with ϕ(E[X]), which is a trivial error, if ϕ is not a linear function.

  10. 10.

    The term “life” is used throughout the present Sect. 4 for indicating the generic percentile of the distribution of times-to-failure of an insulation, according to a very common practice in electrical insulation literature since the very early times till now (see, e.g., [58, 65, 118, 127, 144]).

Abbreviations

ALT:

Accelerated life test

a.s.:

Almost surely

BS:

Birnbaum–Saunders (distribution)

cdf:

Cumulative distribution function

CLT:

Central limit theorem

CV:

Coefficient of variation

CRF:

Conditional reliability function

DHR:

Decreasing hazard rate

DRA:

Direct reliability assessment

D[Y]:

Standard deviation of the RV Y

E[Y]:

Expectation of the RV Y

EV:

Extreme value (distribution)

F(x):

Generic cdf

f(x):

Generic pdf

f(x), F(x):

pdf and cdf of stress

g(y), G(y):

pdf and cdf of strength

G(r, ϕ):

Gamma distribution with parameters (r, ϕ)

H( ):

Cumulative hrf

hrf:

Hazard rate function

HRM:

Hyperbolic reliability model

HV:

High voltage

IDHR:

First increasing, then decreasing hazard rate

IG:

Inverse Gaussian (distribution)

IHR:

Increasing hazard rate

IID:

Independent and identically distributed (random variables)

IPM:

Inverse power model

IRA:

Indirect reliability assessment

IW:

Inverse Weibull (distribution)

LL:

Log-logistic (distribution)

LN:

Lognormal (distribution)

LT:

Lifetime

MRL:

Mean residual life

MV:

Medium voltage

N(α, β):

Normal (Gaussian) random variable with mean α and standard deviation β

pdf:

Probability density function

r(s):

Mean residual life function at age s

RF:

Reliability function

R(t):

Reliability function at mission time t

R(t|s):

Conditional reliability function at mission time t, after age s

RV:

Random variable

SD, σ :

Standard deviation

s-independent:

Statistically independent

SP:

Stochastic process

SS:

Stress-strength

Var, σ2 :

Variance

W(t):

Wear process at time t acting on a device

W(a, b):

Weibull model with RF: R(x) = exp(−ax b)

W′(α, β):

Alternative form of Weibull model, with RF: R(x) = exp[−(x/α)β]

δ(·):

Dirac delta function

X, X(t):

Stress (RV or SP)

Y, Y(t):

Strength (RV or SP)

Γ( ):

Euler–Gamma function

Γ(,):

Incomplete gamma function

μ:

Mean value (expectation)

Φ(z):

Standard normal cdf

φ(z):

Standard normal pdf

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Acknowledgments

The authors wish to express their thankful acknowledgments to some friends and colleagues of the University of Naples “Federico II”, for their very useful advices and significant contributions to the improvement of the present chapter. In particular, we express our thanks to Profs. Ernesto Conte, Pasquale Erto, Biagio Palumbo. We are also grateful to Profs. Erto and Palumbo and Dr. Giuliana Pallotta for bringing to our attention the main preliminary results of their last paper, while it was still in progress [75]. We also thank Dr. Claudia Battistelli for her help in revising the manuscript.

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Chiodo, E., Mazzanti, G. (2011). Mathematical and Physical Properties of Reliability Models in View of their Application to Modern Power System Components. In: Anders, G., Vaccaro, A. (eds) Innovations in Power Systems Reliability. Springer Series in Reliability Engineering. Springer, London. https://doi.org/10.1007/978-0-85729-088-5_3

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