This paper presents the classical flexural buckling solution to an ideal prismatic column with an intermediate lateral elastic restraint and subjected to a concentrated axial load at the top end only. The end conditions are ideal ~clamped, hinged, and free!. The discussor finds this paper useful, particularly for testing a matrix solution proposed by the writer that appears much more general and simpler to program. Consider the stepped column that connects points A and B ~Fig. 1!. This consists of two column segments, AC and CB, with semirigid connections at ends A and B and at the intermediate joint C. It is assumed that ~1! both column segments, AC and CB, are made of homogeneous linear elastic materials with mechanical and geometric properties Et It At ht and Eb Ib Ab hb ~where E5elastic modulus; I5moment of inertia; A5cross-sectional area; and h5span). The subindices t and b indicate the top and bottom column segments, respectively; ~2! the centroidal axis of each segment is a straight line with their centroidal axes lineup; ~3! the column is subject simultaneously to axial loading Pa and transverse load Va at point A, to concentrated loads Pc and Vc , and bending moment M c at the intermediate joint C; and ~4! the lateral sways of the column are partially inhibited by linear springs Sa and Sc located at A and C, respectively, and by an external rotational spring of magnitude SQ at joint C. The rotational fixity factors at ends A and B and the intermediate joint C ~of column segment AC! are assumed to be ra , rb , and rc , respectively. Further details of this model are given by Aristizabal-Ochoa ~1997b!. A general solution to the second-order analysis and buckling load of the column in Fig. 1 is as follows: