SUPPORT THE WORK

GetWiki

Weibull distribution

ARTICLE SUBJECTS
aesthetics  →
being  →
complexity  →
database  →
enterprise  →
ethics  →
fiction  →
history  →
internet  →
knowledge  →
language  →
licensing  →
linux  →
logic  →
method  →
news  →
perception  →
philosophy  →
policy  →
purpose  →
religion  →
science  →
sociology  →
software  →
truth  →
unix  →
wiki  →
ARTICLE TYPES
essay  →
feed  →
help  →
system  →
wiki  →
ARTICLE ORIGINS
critical  →
discussion  →
forked  →
imported  →
original  →
Weibull distribution
[ temporary import ]
please note:
- the content below is remote from Wikipedia
- it has been imported raw for GetWiki
{{Short description|Continuous probability distribution}}







factoids
  • A value of k
< 1, indicates that the failure rate decreases over time (like in case of the Lindy effect, which however corresponds to Pareto distributionsJOURNAL, Eliazar, Iddo, November 2017, Lindy’s Law, Physica A: Statistical Mechanics and Its Applications, 486, 797–805, 2017PhyA..486..797E, 10.1016/j.physa.2017.05.077, 125349686, rather than Weibull distributions). This happens if there is significant “infant mortality”, or defective items failing early and the failure rate decreasing over time as the defective items are weeded out of the population. In the context of the diffusion of innovations, this means negative word of mouth: the hazard function is a monotonically decreasing function of the proportion of adopters;
  • A value of k = 1, indicates that the failure rate is constant over time. This might suggest random external events are causing mortality, or failure. The Weibull distribution reduces to an exponential distribution;
  • A value of k > 1, indicates that the failure rate increases with time. This happens if there is an “aging” process, or parts that are more likely to fail as time goes on. In the context of the diffusion of innovations, this means positive word of mouth: the hazard function is a monotonically increasing function of the proportion of adopters. The function is first convex, then concave with an inflection point at (e^{1/k} - 1)/e^{1/k},, k > 1,.
In the field of materials science, the shape parameter k of a distribution of strengths is known as the Weibull modulus. In the context of diffusion of innovations, the Weibull distribution is a “pure” imitation/rejection model.

Alternative parameterizations

First alternative

Applications in medical statistics and econometrics often adopt a different parameterization.BOOK, Collett, David, Modelling survival data in medical research, Boca Raton, Chapman and Hall / CRC, 3rd, 2015, 978-1439856789, BOOK, Cameron, A. C., Trivedi, P. K., Microeconometrics : methods and applications, 2005, 978-0-521-84805-3, 584, The shape parameter k is the same as above, while the scale parameter is b = lambda^{-k}. In this case, for x ≥ 0, the probability density function is
f(x;k,b) = bkx^{k-1}e^{-bx^k},
the cumulative distribution function is
F(x;k,b) = 1 - e^{-bx^k},
the hazard function is
h(x;k,b) = bkx^{k-1},
and the mean is
b^{-1/k}Gamma(1+1/k).

Second alternative

A second alternative parameterization can also be found.BOOK, Kalbfleisch, J. D., The statistical analysis of failure time data, Prentice, R. L., J. Wiley, 2002, 978-0-471-36357-6, 2nd, Hoboken, N.J., 50124320, WEB, Therneau, T., 2020, R package version 3.1., A Package for Survival Analysis in R.,CRAN.R-project.org/package=survival, The shape parameter k is the same as in the standard case, while the scale parameter λ is replaced with a rate parameter β = 1/λ. Then, for x ≥ 0, the probability density function is
f(x;k,beta) = beta k({beta x})^{k-1} e^{-(beta x)^k}
the cumulative distribution function is
F(x;k,beta) = 1 - e^{-(beta x)^k},
and the hazard function is
h(x;k,beta) = beta k({beta x})^{k-1}.
In all three parameterizations, the hazard is decreasing for k < 1, increasing for k > 1 and constant for k = 1, in which case the Weibull distribution reduces to an exponential distribution.

Properties

Density function

The form of the density function of the Weibull distribution changes drastically with the value of k. For 0 < k < 1, the density function tends to ∞ as x approaches zero from above and is strictly decreasing. For k = 1, the density function tends to 1/λ as x approaches zero from above and is strictly decreasing. For k > 1, the density function tends to zero as x approaches zero from above, increases until its mode and decreases after it. The density function has infinite negative slope at x = 0 if 0 < k < 1, infinite positive slope at x = 0 if 1 < k < 2 and null slope at x = 0 if k > 2. For k = 1 the density has a finite negative slope at x = 0. For k = 2 the density has a finite positive slope at x = 0. As k goes to infinity, the Weibull distribution converges to a Dirac delta distribution centered at x = λ. Moreover, the skewness and coefficient of variation depend only on the shape parameter. A generalization of the Weibull distribution is the hyperbolastic distribution of type III.

Cumulative distribution function

The cumulative distribution function for the Weibull distribution is
F(x;k,lambda) = 1 - e^{-(x/lambda)^k},
for x ≥ 0, and F(x; k; λ) = 0 for x < 0.If x = λ then F(x; k; λ) = 1 âˆ’ e−1 ≈ 0.632 for all values of k. Vice versa: at F(x; k; λ) = 0.632 the value of x â‰ˆ Î».The quantile (inverse cumulative distribution) function for the Weibull distribution is
Q(p;k,lambda) = lambda(-ln(1-p))^{1/k}
for 0 ≤ p < 1.The failure rate h (or hazard function) is given by
h(x;k,lambda) = {k over lambda} left({x over lambda}right)^{k-1}.
The Mean time between failures MTBF is
text{MTBF}(k,lambda) = lambdaGamma(1+1/k).

Moments

The moment generating function of the logarithm of a Weibull distributed random variable is given by{{harvnb|Johnson|Kotz|Balakrishnan|1994}}
operatorname Eleft[e^{tlog X}right] = lambda^tGammaleft(frac{k}+1right)
where {{math|Γ}} is the gamma function. Similarly, the characteristic function of log X is given by
operatorname Eleft[e^{itlog X}right] = lambda^{it}Gammaleft(frac{it}{k}+1right).
In particular, the nth raw moment of X is given by
m_n = lambda^n Gammaleft(1+frac{n}{k}right).
The mean and variance of a Weibull random variable can be expressed as
operatorname{E}(X) = lambda Gammaleft(1+frac{1}{k}right),
and
operatorname{var}(X) = lambda^2left[Gammaleft(1+frac{2}{k}right) - left(Gammaleft(1+frac{1}{k}right)right)^2right],.
The skewness is given by
gamma_1=frac{2Gamma_1^3-3Gamma_1Gamma_2+ Gamma_3 }{[Gamma_2-Gamma_1^2]^{3/2}}
where Gamma_i=Gamma(1+i/k), which may also be written as
gamma_1=frac{Gammaleft(1+frac{3}{k}right)lambda^3-3musigma^2-mu^3}{sigma^3}
where the mean is denoted by {{math|μ}} and the standard deviation is denoted by {{math|σ}}.The excess kurtosis is given by
gamma_2=frac{-6Gamma_1^4+12Gamma_1^2Gamma_2-3Gamma_2^2-4Gamma_1 Gamma_3 +Gamma_4}{[Gamma_2-Gamma_1^2]^2}
where Gamma_i=Gamma(1+i/k). The kurtosis excess may also be written as:
gamma_2=frac{lambda^4Gamma(1+frac{4}{k})-4gamma_1sigma^3mu-6mu^2sigma^2-mu^4}{sigma^4}-3.

Moment generating function

A variety of expressions are available for the moment generating function of X itself. As a power series, since the raw moments are already known, one has
operatorname Eleft[e^{tX}right] = sum_{n=0}^infty frac{t^nlambda^n}{n!} Gammaleft(1+frac{n}{k}right).
Alternatively, one can attempt to deal directly with the integral
operatorname Eleft[e^{tX}right] = int_0^infty e^{tx} frac k lambda left(frac{x}{lambda}right)^{k-1}e^{-(x/lambda)^k},dx.
If the parameter k is assumed to be a rational number, expressed as k = p/q where p and q are integers, then this integral can be evaluated analytically.See {{harv|Cheng|Tellambura|Beaulieu|2004}} for the case when k is an integer, and {{harv|Sagias|Karagiannidis|2005}} for the rational case. With t replaced by −t, one finds
operatorname Eleft[e^{-tX}right] = frac1{ lambda^k, t^k} , frac{ p^k , sqrt{q/p}} {(sqrt{2 pi})^{q+p-2}} , G_{p,q}^{,q,p} !left( left. begin{matrix} frac{1-k}{p}, frac{2-k}{p}, dots, frac{p-k}{p} frac{0}{q}, frac{1}{q}, dots, frac{q-1}{q} end{matrix} ; right| , frac {p^p} {left( q , lambda^k , t^k right)^q} right)
where G is the Meijer G-function.The characteristic function has also been obtained by {{harvtxt|Muraleedharan|Rao|Kurup|Nair|2007}}. The characteristic function and moment generating function of 3-parameter Weibull distribution have also been derived by {{harvtxt|Muraleedharan|Soares|2014}} by a direct approach.

Minima

Let X_1, X_2, ldots, X_n be independent and identically distributed Weibull random variables with scale parameter lambda and shape parameter k. If the minimum of these n random variables is Z = min(X_1, X_2, ldots, X_n), then the cumulative probability distribution of Z given by
F(z) = 1 - e^{-n(z/lambda)^k}.
That is, Z will also be Weibull distributed with scale parameter n^{-1/k} lambda and with shape parameter k.

Reparametrization tricks

Fix some alpha > 0. Let (pi_1, ..., pi_n) be nonnegative, and not all zero, and let g_1,... , g_n be independent samples of text{Weibull}(1, alpha^{-1}), thenJOURNAL, Balog, Matej, Tripuraneni, Nilesh, Ghahramani, Zoubin, Weller, Adrian, 2017-07-17, Lost Relatives of the Gumbel Trick,proceedings.mlr.press/v70/balog17a.html, International Conference on Machine Learning, en, PMLR, 371–379,
  • argmin_i (g_i pi_i^{-alpha}) sim text{Categorical}left(frac{pi_j}{sum_i pi_i}right)_j
  • min_i (g_i pi_i^{-alpha}) simtext{Weibull}left( left(sum_i pi_i right)^{-alpha}, alpha^{-1}right).

Shannon entropy

The information entropy is given by
H(lambda,k) = gammaleft(1 - frac{1}{k}right) + lnleft(frac{lambda}{k}right) + 1where gamma is the Euler–Mascheroni constant. The Weibull distribution is the maximum entropy distribution for a non-negative real random variate with a fixed expected value of x’k equal to λ’k and a fixed expected value of ln(x’k) equal to ln(λ’k) âˆ’ gamma.

Kullback–Leibler divergence

The Kullback–Leibler divergence between two Weibulll distributions is given byARXIV, 1310.3713, cs.IT, Christian, Bauckhage, Computing the Kullback-Leibler Divergence between two Weibull Distributions, 2013,
D_text{KL}( mathrm{Weib}_1 parallel mathrm{Weib}_2) = log frac{k_1}{lambda_1^{k_1}} - log frac{k_2}{lambda_2^{k_2}} + (k_1 - k_2) left[ log lambda_1 - frac{gamma}{k_1} right] + left(frac{lambda_1}{lambda_2}right)^{k_2} Gamma left(frac{k_2}{k_1} + 1 right) - 1

Parameter estimation

Ordinary least square using Weibull plot

(File:Weibull qq.svg|thumb|right|Weibull plot)The fit of a Weibull distribution to data can be visually assessed using a Weibull plot.WEB,www.itl.nist.gov/div898/handbook/eda/section3/weibplot.htm, 1.3.3.30. Weibull Plot, www.itl.nist.gov, The Weibull plot is a plot of the empirical cumulative distribution function widehat F(x) of data on special axes in a type of Q–Q plot. The axes are ln(-ln(1-widehat F(x))) versus ln(x). The reason for this change of variables is the cumulative distribution function can be linearized:
begin{align}
F(x) &= 1-e^{-(x/lambda)^k}[4pt]-ln(1-F(x)) &= (x/lambda)^k[4pt]underbrace{ln(-ln(1-F(x)))}_{textrm{’y’}} &= underbrace{kln x}_{textrm{’mx’}} - underbrace{kln lambda}_{textrm{’c’}}end{align}which can be seen to be in the standard form of a straight line. Therefore, if the data came from a Weibull distribution then a straight line is expected on a Weibull plot.There are various approaches to obtaining the empirical distribution function from data: one method is to obtain the vertical coordinate for each point using widehat F = frac{i-0.3}{n+0.4} where i is the rank of the data point and n is the number of data points.Wayne Nelson (2004) Applied Life Data Analysis. Wiley-Blackwell {{ISBN|0-471-64462-5}}Linear regression can also be used to numerically assess goodness of fit and estimate the parameters of the Weibull distribution. The gradient informs one directly about the shape parameter k and the scale parameter lambda can also be inferred.

Method of moments

The coefficient of variation of Weibull distribution depends only on the shape parameter:JOURNAL,www.stat.cmu.edu/technometrics/59-69/VOL-07-04/v0704579.pdf, Maximum Likelihood Estimation in the Weibull Distribution Based on Complete and on Censored Samples, A. Clifford, Cohen, Technometrics, 4, 7, Nov 1965, 579-588,
CV^2 = frac{sigma^2}{mu^2}
= frac{Gammaleft(1+frac{2}{k}right) - left(Gammaleft(1+frac{1}{k}right)right)^2}{left(Gammaleft(1+frac{1}{k}right)right)^2}.
Equating the sample quantities s^2/bar{x}^2 to sigma^2/mu^2, the moment estimate of the shape parameter k can be read off either from a look up table or a graph of CV^2 versus k. A more accurate estimate of hat{k} can be found using a root finding algorithm to solve
frac{Gammaleft(1+frac{2}{k}right) - left(Gammaleft(1+frac{1}{k}right)right)^2}{left(Gammaleft(1+frac{1}{k}right)right)^2} = frac{s^2}{bar{x}^2}.
The moment estimate of the scale parameter can then be found using the first moment equation as
hat{lambda} = frac{bar{x}}{Gammaleft(1 + frac{1}{hat{k}}right)}.

Maximum likelihood

The maximum likelihood estimator for the lambda parameter given k is
widehat lambda = left(frac{1}{n} sum_{i=1}^n x_i^k right)^frac{1}{k}
The maximum likelihood estimator for k is the solution for k of the following equationBOOK
, Sornette, D.
, 2004
, Critical Phenomena in Natural Science: Chaos, Fractals, Self-organization, and Disorder, .


0 = frac{sum_{i=1}^n x_i^k ln x_i }{sum_{i=1}^n x_i^k }
- frac{1}{k} - frac{1}{n} sum_{i=1}^n ln x_i
This equation defines widehat k only implicitly, one must generally solve for k by numerical means.When x_1 > x_2 > cdots > x_N are the N largest observed samples from a dataset of more than N samples, then the maximum likelihood estimator for the lambda parameter given k is
widehat lambda^k = frac{1}{N} sum_{i=1}^N (x_i^k - x_N^k)
Also given that condition, the maximum likelihood estimator for k is{{citation needed|date=December 2017}}
0 = frac{sum_{i=1}^N (x_i^k ln x_i - x_N^k ln x_N)}
{sum_{i=1}^N (x_i^k - x_N^k)}
- frac{1}{N} sum_{i=1}^N ln x_i
Again, this being an implicit function, one must generally solve for k by numerical means.

Applications

The Weibull distribution is used{{Citation needed|date=June 2010}}File:FitWeibullDistr.tif|thumb|240px|Fitted cumulative Weibull distribution to maximum one-day rainfalls using CumFreq, see also distribution fittingdistribution fitting(File:DCA with four RDC.png|thumb|240px|Fitted curves for oil production time series data JOURNAL, Lee, Se Yoon, Bani, Mallick, Bayesian Hierarchical Modeling: Application Towards Production Results in the Eagle Ford Shale of South Texas, Sankhya B, 2021, 84, 1–43, 10.1007/s13571-020-00245-8, free, )
  • In survival analysis
  • In reliability engineering and failure analysis
  • In electrical engineering to represent overvoltage occurring in an electrical system
  • In industrial engineering to represent manufacturing and delivery times
  • In extreme value theory
  • In weather forecasting and the wind power industry to describe wind speed distributions, as the natural distribution often matches the Weibull shapeWEB,www.reuk.co.uk/Wind-Speed-Distribution-Weibull.htm, Wind Speed Distribution Weibull – REUK.co.uk, www.reuk.co.uk,
  • In communications systems engineering
    • In radar systems to model the dispersion of the received signals level produced by some types of clutters
    • To model fading channels in wireless communications, as the Weibull fading model seems to exhibit good fit to experimental fading channel measurements
  • In information retrieval to model dwell times on web pages.BOOK, Liu, Chao, White, Ryen W., Dumais, Susan, 2010-07-19, Understanding web browsing behaviors through Weibull analysis of dwell time, ACM, 379–386, 10.1145/1835449.1835513, 9781450301534, 12186028,
  • In general insurance to model the size of reinsurance claims, and the cumulative development of asbestosis losses
  • In forecasting technological change (also known as the Sharif-Islam model)JOURNAL, 10.1016/0040-1625(80)90026-8, The Weibull distribution as a general model for forecasting technological change, Technological Forecasting and Social Change, 18, 3, 247–56, 1980, Sharif, M.Nawaz, Islam, M.Nazrul,
  • In hydrology the Weibull distribution is applied to extreme events such as annual maximum one-day rainfalls and river discharges.
  • In decline curve analysis to model oil production rate curve of shale oil wells.
  • In describing the size of particles generated by grinding, milling and crushing operations, the 2-Parameter Weibull distribution is used, and in these applications it is sometimes known as the Rosin–Rammler distribution.Computational Optimization of Internal Combustion Engine page 49 In this context it predicts fewer fine particles than the log-normal distribution and it is generally most accurate for narrow particle size distributions.BOOK, Austin, L. G., Klimpel, R. R., Luckie, P. T., Process Engineering of Size Reduction, 1984, Guinn Printing Inc., Hoboken, NJ, 0-89520-421-5, The interpretation of the cumulative distribution function is that F(x; k, lambda) is the mass fraction of particles with diameter smaller than x, where lambda is the mean particle size and k is a measure of the spread of particle sizes.
  • In describing random point clouds (such as the positions of particles in an ideal gas): the probability to find the nearest-neighbor particle at a distance x from a given particle is given by a Weibull distribution with k=3 and rho=1/lambda^3 equal to the density of the particles.JOURNAL, Chandrashekar, S., Stochastic Problems in Physics and Astronomy, Reviews of Modern Physics, 15, 1, 1943, 86,
  • In calculating the rate of radiation-induced (Radiation hardeningDigital_damage:_SEE|single event effects) onboard spacecraft, a four-parameter Weibull distribution is used to fit experimentally measured device cross section probability data to a particle linear energy transfer spectrum.REPORT, November 15, 2008, ECSS-E-ST-10-12C – Methods for the calculation of radiation received and its effects, and a policy for design margins,ecss.nl/standard/ecss-e-st-10-12c-methods-for-the-calculation-of-radiation-received-and-its-effects-and-a-policy-for-design-margins/, European Cooperation for Space Standardization, The Weibull fit was originally used because of a belief that particle energy levels align to a statistical distribution, but this belief was later proven false{{cn|date=November 2023}} and the Weibull fit continues to be used because of its many adjustable parameters, rather than a demonstrated physical basis.REPORT, L. D. Edmonds, C. E. Barnes, L. Z. Scheick, May 2000, An Introduction to Space Radiation Effects on Microelectronics,parts.jpl.nasa.gov/pdf/JPL00-62.pdf, NASA Jet Propulsion Laboratory, California Institute of Technology, 8.3 Curve Fitting, 75–76,

Related distributions

  • If W sim mathrm{Weibull}(lambda, k), then the variable G = log W is Gumbel (minimum) distributed with location parameter mu = log lambda and scale parameter beta = 1/k. That is, G sim mathrm{Gumbel}_{min}(log lambda, 1/k).
  • {{paragraph break}}A Weibull distribution is a generalized gamma distribution with both shape parameters equal to k.
  • {{paragraph break}}The translated Weibull distribution (or 3-parameter Weibull) contains an additional parameter. It has the probability density function f(x;k,lambda, theta)={k over lambda} left({x - theta over lambda}right)^{k-1} e^{-left({x-theta over lambda}right)^k}, {{paragraph break}}for x geq theta and f(x; k, lambda, theta) = 0 for x < theta, where k > 0 is the shape parameter, lambda > 0 is the scale parameter and theta is the location parameter of the distribution. theta value sets an initial failure-free time before the regular Weibull process begins. When theta = 0, this reduces to the 2-parameter distribution.
  • {{paragraph break}}The Weibull distribution can be characterized as the distribution of a random variable W such that the random variable X = left(frac{W}{lambda}right)^k {{paragraph break}}is the standard exponential distribution with intensity 1.
  • This implies that the Weibull distribution can also be characterized in terms of a uniform distribution: if U is uniformly distributed on (0,1), then the random variable W = lambda(-ln(U))^{1/k}, is Weibull distributed with parameters k and lambda. Note that -ln(U) here is equivalent to X just above. This leads to an easily implemented numerical scheme for simulating a Weibull distribution.
  • The Weibull distribution interpolates between the exponential distribution with intensity 1/lambda when k = 1 and a Rayleigh distribution of mode sigma = lambda/sqrt{2} when k = 2.
  • The Weibull distribution (usually sufficient in reliability engineering) is a special case of the three parameter exponentiated Weibull distribution where the additional exponent equals 1. The exponentiated Weibull distribution accommodates unimodal, bathtub shapedWEB,www.sys-ev.com/reliability01.htm, System evolution and reliability of systems, Sysev (Belgium), 2010-01-01, and monotone failure rates.
  • {{paragraph break}}The Weibull distribution is a special case of the generalized extreme value distribution. It was in this connection that the distribution was first identified by Maurice Fréchet in 1927.BOOK, Montgomery, Douglas, Introduction to statistical quality control, John Wiley, [S.l.], 9781118146811, 95, 2012-06-19, The closely related Fréchet distribution, named for this work, has the probability density function f_{rm{Frechet}}(x;k,lambda)=frac{k}{lambda} left(frac{x}{lambda}right)^{-1-k} e^{-(x/lambda)^{-k}} = f_{rm{Weibull}}(x;-k,lambda).
  • The distribution of a random variable that is defined as the minimum of several random variables, each having a different Weibull distribution, is a poly-Weibull distribution.
  • {{paragraph break}}The Weibull distribution was first applied by {{harvtxt|Rosin|Rammler|1933}} to describe particle size distributions. It is widely used in mineral processing to describe particle size distributions in comminution processes. In this context the cumulative distribution is given by f(x;P_{rm{80}},m) = begin{cases}
1-e^{lnleft(0.2right)left(frac{x}{P_{rm{80}}}right)^m} & xgeq0 ,

- content above as imported from Wikipedia
- "Weibull distribution" does not exist on GetWiki (yet)
- time: 1:06pm EDT - Wed, May 22 2024
[ this remote article is provided by Wikipedia ]
LATEST EDITS [ see all ]
GETWIKI 21 MAY 2024
GETWIKI 09 JUL 2019
Eastern Philosophy
History of Philosophy
GETWIKI 09 MAY 2016
GETWIKI 18 OCT 2015
M.R.M. Parrott
Biographies
GETWIKI 20 AUG 2014
CONNECT