Page 452 - A First Course In Stochastic Models
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B. USEFUL PROBABILITY DISTRIBUTIONS             447

                1/µ 1 (1/µ 2 ). The hyperexponential density always has a coefficient of variation
                of at least 1 and is unimodal with a maximum at t = 0. The failure rate func-
                tion of the hyperexponential distribution is decreasing. The H 2 density has three
                parameters and is therefore not uniquely determined by its first two moments. For
                a two-moment fit, the H 2 density with balanced means is often used; that is, the
                normalization p 1 /µ 1 = p 2 /µ 2 is used. The parameters of the H 2 density having
                balanced means and fitting the first two moments of a positive random variable X
                     2
                with c ≥ 1 are
                     X

                          
      2
                        1       c − 1                         2p 1         2p 2
                                 X
                   p 1 =   1 +   2      ,  p 2 = 1 − p 1 ,  µ 1 =  ,  µ 2 =    .
                        2       c + 1                        E(X)         E(X)
                                 X
                In the context of a Coxian-2 distribution we give below another normalization we
                believe to be a more natural one. A three-moment fit by an H 2 density is not
                always possible, but it is unique whenever it exists. An H 2 density can only be
                fitted to the first three moments m 1 , m 2 and m 3 of a positive random variable X
                                                       2
                                                     3
                     2
                with c > 1 when the requirement m 1 m 3 ≥ m is satisfied; see Whitt (1982). If
                     X                               2  2
                        3
                          2
                m 1 m 3 = m then the H 2 fit is the exponential density, otherwise the parameters
                        2  2
                of the three-moment fit are given by
                           1        2               µ 1 (1 − µ 2 m 1 )
                     µ 1,2 =  a 1 + a − 4a 2 ,  p 1 =           ,  p 2 = 1 − p 1 ,
                                    1
                           2                          µ 1 − µ 2
                                         2
                                                              1
                             2
                                      3
                where a 2 = (6m − 3m 2 )/( m − m 1 m 3 ) and a 1 = (1 + m 2 a 2 )/m 1 . The require-
                             1
                                         2
                                                              2
                                      2
                            3
                               2
                ment m 1 m 3 ≥ m holds for both a gamma distributed and a lognormal distributed
                            2  2
                                     2
                random variable X with c > 1.
                                     X
                Coxian-2 distribution
                The hyperexponential density requires that the weights p 1 and p 2 are non-negative.
                However, in order that p 1 µ 1 exp(−µ 1 t) + p 2 µ 2 exp(−µ 2 t) represents a probability
                density, it is not necessary to require that p 1 and p 2 are both non-negative. The
                class of H 2 distributions can be shown to be a subclass of the class of so-called
                Coxian-2 (C 2 ) distributions. A random variable X is said to be Coxian-2 distributed
                if X can be represented as

                                      X 1 + X 2  with probability b,
                                X =
                                      X 1      with probability 1 − b,
                where X 1 and X 2 are independent random variables having exponential distribu-
                tions with respective means 1/µ 1 and 1/µ 2 . In words, the lifetime X first goes
                through an exponential phase X 1 and then through a second exponential phase X 2
                with probability b or it goes out with probability 1 − b; see Figure B.2. It can be
                assumed without loss of generality that µ 1 ≥ µ 2 .
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