Template:Generalized gamma probability density function: Difference between revisions

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===Generalized Gamma Probability Density Function===
===Generalized Gamma Probability Density Function===


The generalized gamma function is a three-parameter distribution. One version of the generalized gamma distribution uses the parameters , , and . The   for this form of the generalized gamma distribution is given by:
The generalized gamma function is a three-parameter distribution. One version of the generalized gamma distribution uses the parameters ''k'', <math>\beta<\math>, and <math>\theta<\math>. The ''pdf'' for this form of the generalized gamma distribution is given by:


::<math>f(t)=\frac{\beta }{\Gamma (k)\cdot \theta }{{\left( \frac{t}{\theta } \right)}^{k\beta -1}}{{e}^{-{{\left( \frac{t}{\theta } \right)}^{\beta }}}}</math>


where   is a scale parameter,   and   are shape parameters and   is the gamma function of , which is defined by:
where <math>\theta >0</math> is a scale parameter, <math>\beta >0</math> and <math>k>0</math> are shape parameters and <math>\Gamma (x)</math> is the gamma function of ''x'', which is defined by:





Revision as of 19:03, 14 February 2012

Generalized Gamma Probability Density Function

The generalized gamma function is a three-parameter distribution. One version of the generalized gamma distribution uses the parameters k, [math]\displaystyle{ \beta\lt \math\gt , and \lt math\gt \theta\lt \math\gt . The ''pdf'' for this form of the generalized gamma distribution is given by: ::\lt math\gt f(t)=\frac{\beta }{\Gamma (k)\cdot \theta }{{\left( \frac{t}{\theta } \right)}^{k\beta -1}}{{e}^{-{{\left( \frac{t}{\theta } \right)}^{\beta }}}} }[/math]

where [math]\displaystyle{ \theta \gt 0 }[/math] is a scale parameter, [math]\displaystyle{ \beta \gt 0 }[/math] and [math]\displaystyle{ k\gt 0 }[/math] are shape parameters and [math]\displaystyle{ \Gamma (x) }[/math] is the gamma function of x, which is defined by:


With this version of the distribution, however, convergence problems arise that severely limit its usefulness. Even with data sets containing 200 or more data points, the MLE methods may fail to converge. Further adding to the confusion is the fact that distributions with widely different values of , , and may appear almost identical [21]. In order to overcome these difficulties, Weibull++ uses a reparameterization with parameters , , and [21] where:


where and While this makes the distribution converge much more easily in computations, it does not facilitate manual manipulation of the equation. By allowing to become negative, the of the reparameterized distribution is given by: