The Weibull and Gumbel (Extreme Value)

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The Weibull and Gumbel (Extreme Value) Distributions 1 STA312 Spring 2019 1 See last slide for copyright information. 1 / 14

Transcript of The Weibull and Gumbel (Extreme Value)

Page 1: The Weibull and Gumbel (Extreme Value)

The Weibull and Gumbel (Extreme Value)Distributions1

STA312 Spring 2019

1See last slide for copyright information.1 / 14

Page 2: The Weibull and Gumbel (Extreme Value)

The Weibull Distribution

f (t|α, λ) ={αλ(λt)α−1 exp{−(λt)α} for t ≥ 0

0 for t < 0,

where α > 0 and λ > 0.

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Weibull with α = 1/2 and λ = 1

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Density

Weibull Density with alpha = 0.5 and lambda = 1

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Weibull with α = 1 and λ = 1Standard exponential

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Weibull Density with alpha = 1 and lambda = 1

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Weibull with α = 1.5 and λ = 1

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Weibull Density with alpha = 1.5 and lambda = 1

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Weibull with α = 5 and λ = 1

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Weibull Density with alpha = 5 and lambda = 1

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Weibull with α = 5 and λ = 1/2

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Weibull Density with alpha = 5 and lambda = 0.5

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The Weibull Distribution

f(t|α, λ) =

{αλ(λt)α−1 exp{−(λt)α} for t ≥ 00 for t < 0

,

where α > 0 and λ > 0.

E(T k) =Γ(1 + k

α)

λk

Median =[log(2)]1/α

λS(t) = exp{−(λt)α}h(t) = αλαtα−1

If α = 1, Weibull reduces to exponential and h(t) = λ.

If α > 1, the hazard function is increasing.

If α < 1, the hazard function is decreasing.

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Page 9: The Weibull and Gumbel (Extreme Value)

The Gumbel DistributionAlso called the extreme value distribution

f (y|µ, σ) = 1

σexp

{(y − µσ

)− e(

y−µσ )

}where σ > 0.

This is a location-scale family of distributions.

µ is the location and σ is the scale.

Write Y ∼ G(µ, σ).

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Page 10: The Weibull and Gumbel (Extreme Value)

Log of standard exponential is Gumbel(0,1)µ = 0 and σ = 1

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Density

Standard Gumbel Density

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Properties of the G(0, 1) Distributionf(y) = exp {y − ey} for all real y.

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Density

Standard Gumbel Density Let Z ∼ G(0, 1).

MGF is Mz(t) = Γ(t+ 1).

E(Z) = Γ′(1) = −0.5772157 . . . = −γ,where γ is Euler’s constant.

V ar(Z) = π2

6 .

Median is log(log(2)) = −0.3665129 . . .

Mode is zero.

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General Y ∼ G(µ, σ)f(y|µ, σ) = 1

σexp

{(y−µσ

)− e(

y−µσ )}

Let Z ∼ G(0, 1) and Y = σZ + µ. Then Y ∼ G(µ, σ).

E(Y ) = σE(Z) + µ = σµ− γ.

V ar(Y ) = σ2V ar(Z) = σ2 π2

6 .

Median is σ log log(2) + µ.

Mode is µ.

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Log of Weibull is Gumbel

Let T ∼ Weibull(α, λ), and Y = log(T ).

In addition, re-parameterize, meaning express the parameters in adifferent, equivalent way.

Let σ = 1α and µ = − log λ.

Or equivalently, substitute 1σ for α and e−µ for λ.

The result is Y ∼ G(µ, σ).

So if you believe the distribution of a set of failure time data couldbe Weibull (a popular choice), you can log-transform the data andapply a Gumbel model.

The Gumbel distribution may be preferable because theparameters µ and σ are easy to interpret.

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Copyright Information

This slide show was prepared by Jerry Brunner, Department ofStatistics, University of Toronto. It is licensed under a CreativeCommons Attribution - ShareAlike 3.0 Unported License. Use any partof it as you like and share the result freely. The LATEX source code isavailable from the course website:http://www.utstat.toronto.edu/∼brunner/oldclass/312s19

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