The name is absent

and

∕₂j(r) = y ‰ι(r') expμ¼ι(r') - βV^r^,)]Δ^⁺¹∖r, r')dr',   (4.28)

∕₂,_m(r) = 1,                                                             (4.29)

where ∕ι,∙(r) = ----—_i~τ---<τ>— and ∕₂,(r) = ----¹——z-∏—. Finally, the

^{ljv j} exp(∕3∑tι¹Wp⅛>(Γ)        ^2jv >     exp(∕3∑-_j+1μ_i)X<f>(r)

Euler-Lagrange eqn. 4.2 can be written as

lnp_j∙(r) - ∑>_j∙(r) - ln∕ι,√r)∕_2j(r) = βμM - βV_j^ext(r),          (4.30)

where μj∏(= ∑2j=i∕^zj) is the bulk chemical potential of the chain. Rearranging
eqn. 4.30 gives

p_j∙(r) = exp(∕3μ⅛f) exp[P_j∙(r) - /3V∕^rf(r)]∕_{1 j}(r)∕₂,√r).          (4.31)

The equilibrium grand free energy is given by
where n(f(ɑɔ) is the total number of associating sites on segment a.

Picard-type iteration method is used to solve the set of eqs. 4.31 for the density
profile of the segments. For the systems considered in this work, the inhomogeneity is
only in one dimension (z). For the density profile, a grid is set up in the z dimension

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