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Bernal S D_2010.pdf - University of Plymouth

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3.3. DEFINITION AND MATHEMATICAl^ FORMULATION<br />

= i;i,l)'(0.27,0.73)^(0.27,0.73)<br />

K{W) - ^n^g,"!) • nw(g) • rcw[m)<br />

n{w = 0) = {P{w ^ OIJ? = 0,m = 0) • iZv^iR - 0) • nw{m - 0)) +...<br />

+ (^(^--01^- l,ffl = 0)-;riv(j?- I}-;rvv(m-0)) + ...<br />

+ {P{w = 0[^' = 0.;/i = I) • ^TivC^ - 0). TTivlm - 1)) + ...<br />

+ {P{w = Q\g= \.m= \)-nw{g= \)-nw(m= \))<br />

-(0.9 0.8 0.5)+ (0.2-0.2-0.5)+ (0.3 0.8-0.5)+ (0.9'0.2-0.5)-0.51<br />

n{w - 1) = (0.1 0.8 • 0.5) + (0.8 • 0.2 • 0.5) + (0.7 • 0.8 • 0.5) + (0.9 • 0.2 • 0.5) - 0.49<br />

;r(>v)-(0.51,0.49)<br />

Bel{w) - a-X{w)-n{w)<br />

-a(0.27,0.73)-(0.51,0.49)-ct-(0.138,0.358)<br />

^(0.278,0.722)<br />

In this case, the evidence in Surfing yields a value <strong>of</strong> k{w) that suggests there is a high prob­<br />

ability <strong>of</strong> Waves (0.73). The top-down prior information i:{w) is practically a flat distribution<br />

(0.51,0.49), i.e. doesn't add any inforniaiion. ihu.s the resulting Ixilief suggests there is u high<br />

probability <strong>of</strong> Waves (0.722). This is shown graphically in the top diagram <strong>of</strong> Figure 3.6.<br />

The next step is to generate the outgoing messages from node IV to its child and parent nodes.<br />

The key property here is that the outgoing messages take into account all evidence except that<br />

which originated from the destination node. For example, the message from W to G. An'(^),<br />

doesn't take into account the prior information conveyed through the incoming message Ttwig).<br />

Given Equations (3.30) and (3.31). the resulting expressions are<br />

97

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