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8.
Assessing Product Reliability
8.1. Introduction 8.1.6. What are the basic lifetime distribution models used for non-repairable populations?
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| A model based on cycles of stress causing degradation or crack growth | In 1969, Birnbaum and Saunders
described a life distribution model that could be derived from a physical
fatigue process where crack growth causes failure. Since one of the best
ways to choose a life distribution model
is to derive it from a physical/statistical argument that is consistent
with the failure mechanism, the Birnbaum-Saunders Fatigue Life Distribution
is worth considering.
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| Formulas and shapes for the Fatigue Life model | The PDF, CDF, mean and variance for the Birnbaum-Saunders
Distribution are shown below. The parameters are:
PDF shapes for the model vary from highly skewed and long tailed (small gamma values) to nearly symmetric and short tailed as gamma increases. This is shown in the figure below.
Corresponding failure rate curves are shown in the next figure.
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| If crack growth in each stress cycle is a random amount independent of past cycles of growth, the Fatigue Life mode model may apply. | Derivation
and Use of the Birnbaum-Saunders Model:
Consider a material that continually undergoes cycles of stress loads. During each cycle, a dominant crack grows towards a critical length that will cause failure. Under repeated application of n cycles of loads, the total extension of the dominant crack can be written as ![]() and we assume the Yj are independent and identically
distributed non-negative random variables with mean µ and variance
Since there are many cycles, each lasting a very short time, we can replace the discrete number of cycles N needed to reach failure by the continuous time tf needed to reach failure. The cdf F(t) of tf is given by
denotes the
standard normal cdf. Writing the model with parameters
and is an alternative
way of writing the Birnbaum-Saunders distribution that is often used
( ,
as compared to the way the formulas were parameterized earlier in this
section).
Note:
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| This kind of physical degradation is consistent with Miner's Rule. | The Birnbaum-Saunders assumption, while physically restrictive, is consistent with a deterministic model from materials physics known as Miner's Rule (Miner's Rule implies that the damage that occurs after n cycles, at a stress level that produces a fatigue life of N cycles, is proportional to n/N). So, when the physics of failure suggests Miner's Rule applies, the Birnbaum-Saunders model is a reasonable choice for a life distribution model. | ||
| Dataplot commands for the Fatigue Life model | Dataplot
Functions for the Birnbaum-Saunders Model
The PDF for a Birnbaum-Saunders (Fatigue Life) distribution with parameters
µ, LET PDF = FLPDF(t,The CDF is LET CDF = FLCDF(t,To generate 100 random numbers, when µ = 5000,
= 2, for example, type the following Dataplot commands:
LET GAMMA = 2Finally, we can do a Fatigue Life Probability Plot of the 100 data points in DATA by LET GAMMA = 2and the points on the resulting plot (shown below) line up roughly on a straight line, as expected for data correctly modeled by the Birnbaum-Saunders distribution.
Notes
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