2949775113

2949775113



727

(3.18)


By setting z = [F(y)]1/0 in (3.18), we find that

On substituting the above expression of J(x) in (3.17), we get

<Tj~0Cs-l


E[Xl (r, n, m, k)X3 p(s,n,m, A;)] =


(r — l)!(s — r — l)!(m + l)s-2


EE


p|r(i -p) '--+2±ł=^a=i-I&.

(3.19)


Again by setting t = [F(x)]x^Q in (3.19), we get

E[Xt(r,n,m,k)Xj 0(s,n,m,k)]


(m + l)s


EE(-»'


c«{fc+(n-r)(m+l)}+P+q-{(i+j)/g}l

a(m+l)    J

p!«! r(j -p)r(f +1 - 9) r    ]

p f q{fc+(n—s)(m+l)}+p+l —(j/0) 1

(3.20)


ttlfc+fn-rKTO+Dł+p+l-Cj/ffll a(m+l)    I

and hence the result given in (3.16).

Special cases

iii) Putting m = 0, k = 1 in (3.20), the explicit formula for the ratio moments of order statistics of the type II exponentiated log-logistic distribution can be obtained as

P!9!r(i-P)r(i + i-5) .r[a(n -r + l)+p + q- {(» + j)/i8}]r[q(n -s + l)+p+l- (j/P)\


; + l

r[a(n+ 1) +p + q- {(i+j)//9}]r[a(n-r + l)+p + 1 - (j/P)] iv) Putting m — —1 in (3.16), the explicit expression for the ratio moments of upper record values for the type II exponentiated log-logistic distribution can be obtained as

r(i)rU + l)

UU v'q- r(p -p)r(j + 1 -5)


Making use of (1.6), we can derive recurrence relations for ratio moments of gos from

(1.2).



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