Contents Telektronikk - Telenor
Contents Telektronikk - Telenor
Contents Telektronikk - Telenor
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Frame 2<br />
Useful time distributions<br />
Negative exponential distribution (ned)<br />
The most interesting time distribution is the exponential distribution<br />
F(t) = 1 – e –λt ; G(t) = e –λt ; f(t) = λe –λt (16)<br />
with the Laplace transform of f(t)<br />
L{s} = f*(s) = λ/(λ + s) (17)<br />
and the nth derivative<br />
(−1) n L (n) {s} =<br />
(18)<br />
A particular property of the exponential distribution is that the<br />
coefficient of variation c = σ/µ = 1 and the form factor<br />
ε = v/µ 2 + 1 = 2. This is used to distinguish between steep<br />
(c < 1) and flat (c > 1) distributions. It has a positive skewness<br />
s = 2.<br />
Hyperexponential distribution<br />
The hyperexponential distribution is obtained by drawing at<br />
random, with probabilities p 1 , p 2 , p 3 , ... , p k , from different<br />
exponential distribution with parameters λ 1 , λ 2 , λ 3 , ... , λ k<br />
For a true distribution we must have<br />
k<br />
∑ pi = 1<br />
i=1<br />
The n th moment similarly becomes (as the Laplace transform<br />
of a sum is the sum of the Laplace transforms)<br />
Hyperexponential distributions are always flat distributions<br />
(c > 1).<br />
Erlang-k distribution<br />
(19)<br />
(20)<br />
(21)<br />
If k exponentially distributed phases follow in sequence, the<br />
sum distribution is found by convolution of all phases. If all<br />
phases have the same parameter (equal means) we obtain the<br />
special Erlang-k distribution (which is the discrete case of the<br />
Γ-distribution),<br />
f (t) =<br />
λ (λt)k −1<br />
(k −1)! e−λt<br />
n!⋅λ<br />
(λ + s) n+1 ;⇒ M n!<br />
n =<br />
λ n<br />
k<br />
F(t) = 1− ∑ pi ⋅e<br />
i=1<br />
−λ i t ; f (t) = piλ ie −λ<br />
k<br />
∑ i<br />
i=1<br />
t<br />
k<br />
k<br />
n<br />
Mn = ∑ pi ⋅ Mni = n!⋅ ∑ pi / λi i=1<br />
i=1<br />
(22)<br />
Since the Laplace transform of a convolution is the product of<br />
the Laplace transforms of the phases, we have for the special<br />
Erlang-k distribution<br />
k<br />
⎛ λ ⎞<br />
L{s} = ⎜ ⎟<br />
⎝ λ + s ⎠<br />
(23)<br />
and the nth moment is found by<br />
(-1) n ⋅ L (n) {s} = k ⋅ (k + 1) ... (k + n - 1) ⋅ λk /(λ + s) k+n<br />
⇒ Mn = k ⋅ (k + 1) ... (k + n - 1)/λn (24)<br />
The mean value is µ = k/λ. A normalised mean of µ = 1/λ is<br />
obtained by the replacement λ ⇒ kλ or t ⇒ kt in the distribution<br />
and the ensuing expressions. If k → ∞ for the normalised<br />
distribution, all central moments approach zero, and the<br />
Erlang-k distribution approaches the deterministic distribution<br />
with µ = 1/λ.<br />
For an Erlang-k distribution it applies in general that<br />
k<br />
µ = M1 = ∑µ<br />
i<br />
i=1<br />
k<br />
mn = ∑ mni for n = 2or3<br />
i=1<br />
k<br />
mn ≠ ∑ mni for n = 4,5,...<br />
i=1<br />
For the general Erlang-k distribution the phases may have different<br />
parameters (different means). The expressions are not<br />
quite so simple, whereas the character of the distribution is<br />
similar. The particular usefulness of the Erlangian distributions<br />
in a traffic scenario is due to the fact that many traffic<br />
processes contain a sequence of independent phases.<br />
β-distribution<br />
The β-distribution is a two-parameter distribution with a variable<br />
range between 0 and 1, 0 ≤ x ≤ 1. Thus, it is useful for<br />
description of a population with some criterion within this<br />
range, for example average load per destination, urgency of a<br />
call demand on a 0 – 1 scale, etc. The distribution density<br />
function is<br />
f (x) =<br />
Γ(α + β )<br />
Γ(α )⋅Γ(β ) xα −1 ⋅ 1− x<br />
( ) β −1 ;α,β > 0<br />
The n th moment is given by<br />
n−1 (α + i)<br />
Mn = ∏<br />
i=0 (α + β + i)<br />
Typical of the above distributions is<br />
Special Erlang-k: c = 1/√k < 1 (steep, serial)<br />
Exponential (ned): c = 1<br />
Hyperexponential: c > 1 (flat, parallel)<br />
β-distribution: c > 1 for α < 1 and β > α(α + 1)/(1 – α)<br />
c < 1 otherwise<br />
(25)<br />
(26)<br />
11