VGAM (version 0.8-2)

expexp: Exponentiated Exponential Distribution

Description

Estimates the two parameters of the exponentiated exponential distribution by maximum likelihood estimation.

Usage

expexp(lshape = "loge", lscale = "loge", eshape = list(), escale = list(),
       ishape = 1.1, iscale = NULL, tolerance = 1.0e-6, zero = NULL)

Arguments

lshape, lscale

Parameter link functions for the $\alpha$ and $\lambda$ parameters. See Links for more choices. The defaults ensure both parameters are positive.

eshape, escale

List. Extra argument for each of the links. See earg in Links for general information.

ishape

Initial value for the $\alpha$ parameter. If convergence fails try setting a different value for this argument.

iscale

Initial value for the $\lambda$ parameter. By default, an initial value is chosen internally using ishape.

tolerance

Numeric. Small positive value for testing whether values are close enough to 1 and 2.

zero

An integer-valued vector specifying which linear/additive predictors are modelled as intercepts only. The default is none of them. If used, choose one value from the set {1,2}.

Value

• An object of class "vglmff" (see vglmff-class). The object is used by modelling functions such as vglm and vgam.

Warning

Practical experience shows that reasonably good initial values really helps. In particular, try setting different values for the ishape argument if numerical problems are encountered or failure to convergence occurs. Even if convergence occurs try perturbing the initial value to make sure the global solution is obtained and not a local solution. The algorithm may fail if the estimate of the shape parameter is too close to unity.

Details

The exponentiated exponential distribution is an alternative to the Weibull and the gamma distributions. The formula for the density is $$f(y;\alpha,\lambda) = \alpha \lambda (1-\exp(-\lambda y))^{\alpha-1} \exp(-\lambda y)$$ where $y>0$, $\alpha>0$ and $\lambda>0$. The mean of $Y$ is $(\psi(\alpha+1)-\psi(1))/\lambda$ (returned as the fitted values) where $\psi$ is the digamma function. The variance of $Y$ is $(\psi'(1)-\psi'(\alpha+1))/\lambda^2$ where $\psi'$ is the trigamma function.

This distribution has been called the two-parameter generalized exponential distribution by Gupta and Kundu (2006). A special case of the exponentiated exponential distribution: $\alpha=1$ is the exponential distribution.

References

Gupta, R. D. and Kundu, D. (2001) Exponentiated exponential family: an alternative to gamma and Weibull distributions, Biometrical Journal, 43, 117--130.

Gupta, R. D. and Kundu, D. (2006) On the comparison of Fisher information of the Weibull and GE distributions, Journal of Statistical Planning and Inference, 136, 3130--3144.

See Also

expexp1, gamma2.ab, weibull, CommonVGAMffArguments.

Examples

# A special case: exponential data
y = rexp(n <- 1000)
fit = vglm(y ~ 1, fam = expexp, trace = TRUE, maxit = 99)
coef(fit, matrix=TRUE)
Coef(fit)


# Ball bearings data (number of million revolutions before failure)
bbearings = c(17.88, 28.92, 33.00, 41.52, 42.12, 45.60,
48.80, 51.84, 51.96, 54.12, 55.56, 67.80, 68.64, 68.64,
68.88, 84.12, 93.12, 98.64, 105.12, 105.84, 127.92,
128.04, 173.40)
fit = vglm(bbearings ~ 1, fam = expexp(iscale = 0.05, ish = 5),
           trace = TRUE, maxit = 300)
coef(fit, matrix = TRUE)
Coef(fit)   # Authors get c(shape=5.2589, scale=0.0314)
logLik(fit) # Authors get -112.9763


# Failure times of the airconditioning system of an airplane
acplane = c(23, 261, 87, 7, 120, 14, 62, 47,
225, 71, 246, 21, 42, 20, 5, 12, 120, 11, 3, 14,
71, 11, 14, 11, 16, 90, 1, 16, 52, 95)
fit = vglm(acplane ~ 1, fam = expexp(ishape = 0.8, isc = 0.15),
           trace = TRUE, maxit = 99)
coef(fit, matrix = TRUE)
Coef(fit)   # Authors get c(shape=0.8130, scale=0.0145)
logLik(fit) # Authors get log-lik -152.264