We consider the class of three-dimensional finite-range, or similar, p
otentials lambda W(r), depending on a strength constant lambda. We stu
dy the behaviour of the eigenvalue E as a function of lambda - lambda(
c), where lambda(c) is the critical value at the transition from 0 -->
1 bound state. For the l = 0 case, we find E proportional to (lambda
- lambda(c))(2), whereas the relationship is linear for l greater than
or equal to 1. Treating l as a continuous parameter in the radial Sch
rodinger equation, we give the evolution of the power law between l =
0 and l = 1. Besides spherically symmetric scalar potentials, we also
discuss the case of a repulsive scalar potential combined with a spin-
orbit component of the Thomas form.