The spin-one Ising ferromagnet on a simple cubic lattice is treated in
the mean-spherical approximation (MSA) for an exchange potential J(r)
parametrized by a Kac-Baker inverse-range parameter gamma, The mean-f
ield result is recovered when gamma --> 0; in this limit the result is
exact. For gamma not equal 0, a detailed analysis is given of the pha
se separation associated with the tricritical point that occurs. The a
nalysis is made through the relation that gives the internal energy vi
a [J(r)]. it shows that the MSA result satisfactorily captures the imp
ortant thermodynamic features of the tricritical point as long as gamm
a is not too large. The case of Coulombic J(r) is also considered; her
e J(r) is antiferromagnetic, An argument is given in support of the ex
pectation that on the simple cubic and body-centered cubic lattices th
e Coulombic J(r) will give rise to a tricritical point at which a lamb
da-line of Neel points meets a paramagnetic-antiferromagnetic coexiste
nce boundary.