The name is absent

tethered to the wall. If we consider a flat wall and that the chains are uniformly dis-
tributed over the surface of the wall, then the problem reduces to a one dimensional
problem with the relevant dimension along the normal to the wall. The external field
exerted by the wall on the tethered segment T’ is

∞ otherwise

And for the other segments

(6.9)

0 otherwise

Then the density of segment T’ is

Pi(O) = ехр(^рм) exp[A(0) - ∕⅛]∕ι,₁(0)∕₂,ι(0),

and for the other segments

(6.ιi)

where,

ʃi,i(^) — T

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