AAWSAP DIRD, An Introduction to the Statistical Drake Equation, March 2010
DOW-UAP-D127 · page 15 of 55
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UNCLASSIFIED/ /FOR OFFIEiIAk Wlii QPU,¥ Table 1. Summary of the Properties of the Lognormal Distribution That Applies to the Random Variable N = Number of ET Communicating Civilizations in the Galaxy Random variable N = number of communicating ET civilizations in galaxy Probability distribution Loqnormal Probability density function (1n(11h,J' 1 1 -~ (n ;::-: 0) n 27!<:T JN (n)= - · & e a' Mean value - (N )= eµe 2 Variance a1 = e2µ ea' (ea' - I) a' a N = eµ e 2 .Jea2 - 1 Standard deviation All the moments, i.e. k-th moment 2 a' k ·2 (N k)= ekµ e _ _ ~I - a-2 Mode (= abscissa of the log normal peak) n nnde = npeak - e e a' f ( ) Value of the Mode Peak 1 -p 2 N n lTl)dc = & ·e ·e 2,r (l Median (= fifty-fifty probability value for rred ian =m =e" N) Skewness K ( , ) e-6pe-3a' _ 3_ = ea + 2 (K4)¾ ., lne3a2 + 3e2a' +6ea' +61 k' K ,, ., ., "} Kurtosis _ 4_ = e4a- + 2 e3a- + 3 e-u- - 6 (K2)2 Expression of 1-1 in terms of the lower (a;) µ = ± (Y;) =± b;[in(b;) - 1]- a;[in(a;)-1] and upper (b;) limits of the Drake i=I i= I b; - a; uniform input random variables 0 ; Expression of <:T 2 in terms of the lower (a;) 7 7 a;b;[ln (b; )- in(a;)f a 2 =La~ = L l and upper (b;) limits of the Drake (b;-a} i= I i=I uniform input random variables 0 ; 7. An Example Explaining the Statistical Drake Equation To understand how things work in practice for the statistical Drake equation, please consider the following table 2. It is made up of three columns: • The first column on the left lists the seven input sheer numbers that also become • The mean values (middle column). • Finally the last column on the right lists the seven input standard deviations. UNCLASSIFIED/1re1t OFFl@IAL WSE 9Nk¥ 15