The vibration of structures is governed by a set of second-order ordinary d
ifferential equations in which the (N x N) coefficient matrices are real. T
hese equations often produce both complex roots and complex modes. In the e
stablished method for computing the roots, the eigenvalue problem is solved
for a certain (2N x 2N) matrix whose form is such that it contains an (N x
N) submatrix of zeros as one of the two diagonal (N x N) blocks. This very
special form has substantial significance in the modes and roots that emer
ge. For systems having no real roots, a part of this significance has alrea
dy been identified by the authors in the form of a relationship between the
real and imaginary parts of complex modes. This article extends this signi
ficance to the point where the equation normally used in computing the comp
lete set of characteristic roots and vectors is transformed to another very
compact form. One of the attractions of this new form is that all of the n
umbers involved are real-although some or all of the roots and vectors may
be complex. The new form has several potential applications, including prov
iding new methods for examining the sensitivity of solutions to perturbatio
ns, achieving realizations of second-order systems from partial knowledge o
f the roots and modes, and forming the basis for a new solution method for
obtaining the characteristic roots and vectors of self-adjoint second-order
systems.