59Exponential Rate Parameters
n = 20
β = 0.05
t
1 −
β ≈ 1.729
Tt
S
n
1.29 1.729
1.08
20
1.708
1
1
0
+≈+≈≥
λ
≈
−β
.
Therefore, we reject H
0
. Also, we have
20 * 1.29 25.8γ≈ =
and
Gn
n
xe dx1(25.8|20, 0.75)1
()
0.5287
n
nx
0
0
1
25.8
0
∫
−=λ= =−
λ
Γ
−−λ
.
Therefore, we would reject H
0
using the “exact” gamma critical value. Note
that for β = 0.05, with n = 20, the critical value, γ
c
, is 17.67. That is,
Gn
n
xe dx(17.67|20, 0.75)
()
0.05
n
nx
0
0
1
17.67
0
∫
=λ==
λ
Γ
−−λ
.
Figure4.1 shows the power curve using the exact gamma critical value of
17.67 for this example.
Condence interval formulation:
Tt
S
1
+
−β
is a 100(1 − β) percent upper condence limit on 1/λ. For the example,
Tt
S
1.29 1.729
1.08
1.708
1
+≈
−β
is a 95 percent upper condence limit on 1/λ, the mean time to event.
Computational considerations:
Care should be taken when using built-in functions for computing
probabilities or quantiles from gamma distributions. In some cases, the
“scale” parameter may be expressed as a rate, for example, the expected
number of occurrences per unit time, and in some cases, the scale parameter
may be expressed as a mean time between events (R, JMP). In some cases,