Abstract
The analytic properties of the effective dielectric constant of a class of three-phase composite materials are studied. Specifically, we investigate the effective dielectric constant of a periodic array of coated cylinders, as a function of the core dielectric constant (
ϵ
c
) and the shell dielectric constant (
ϵ
s
), while keeping the matrix dielectric constant (
ϵ
b
) fixed. We show that when
ϵ
s
= –
ϵ
c
, the composite has exactly the same effective dielectric constant as a periodic array of solid cylinders with dielectric constant
ϵ
c
and radius equal to the outer radius of the original coated cylinder. We also show that when
ϵ
s
= – 1, the composite has exactly the same effective dielectric constant as a periodic array of solid cylinders with dielectric constant
ϵ
c
, and radius exceeding the shell radius. We explore the location of poles and zeros of the three-phase effective dielectric constant in the (
ϵ
s
,
ϵ
c
) plane. The lines
ϵ
s
= – 1 and
ϵ
s
+
ϵ
c
= 0 are loci of essential singularities. We also comment on the behaviour of the effective dielectric constant in the neighbourhood of the two special points (
ϵ
s
,
ϵ
c
) = (0,0) and (
ϵ
s
,
ϵ
c
) = ( - 1 , + 1 ).
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5. J .Phys. C 12 4947-4960.
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