The name is absent



116


adjacent weak compartment we find

'l(awυ)2 , awW


.2 (∆x)2   4(∆x}2


a‰-l
faT - a-w


:NW
w


,2


2 (∆τ)2
'(aww)2


ɪ
aw

4(∆τ)2

aW Z


Nw — 1

LW


(∆rr)2   2(∆τ)2


‰-l

LW


= ‰,l√τ

Now we are ready to write the complete coupled strong-weak system. Letting

1 1 1

c =----jʊ- and cw = ———∑τ-

2Λαafr       w 2Raa%-
and defining the coordinate vectors

eNw ∈          and eNr ∈ Rλ∖

we can write the coupling matrices as

Zw = e.‰,3(⅛r⅛) ∈ R^,∙×^,-<m+1>

7   Cw ,,   („  erΓ ∖ c τpJVw(m+l)×Ns

ls — -^rXw,i\.eNiueNT) ∈ K '   '

and let Hs ∈ Rn≡×7v≈ be the Hines matrix for the strong part and Q be the quasi-active
matrix for the weak part. Then the coupled strong-weak “Hines” matrix is



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