The three-component penetrable-sphere model is used to study the adsor
ption of a third component, b, at the surface of two fluid phases, alp
ha which is rich in component a, and gamma which is rich in component
c. The system has a tricritical point at a reduced pressure of pi(tc)
= 15/4, in a mean-field approximation. At and below this pressure the
adsorption of b, GAMMA(b), first rises as the activity of b, Zeta(b),
increases and then falls rapidly as the tricritical or ordinary critic
al point of the alpha-gamma system is reached. Above pi(tc) the adsorp
tion diverges to an infinite value as Zeta(b) approaches Zeta(b)sat, t
he value at which component b saturates both the alpha and gamma phase
s, and so first forms a new bulk phase, beta, which wets the alpha-gam
ma interface. It is shown that Gamma(b) diverges as - 1n(Zeta(b)sat --
Zeta(b)), a divergence that had been derived previously by Widom on t
he basis of a phenomenologically constructed free energy.