Stellar discs of highly flattened giant galaxies, including that of the Mil
ky Way, are studied by linear theory to determine the stability of such dis
cs against small-amplitude gravity perturbations. In order to understand th
e physics of the problem better, the simplest theoretical model is applied.
That is, the local disc is studied by employing the method of particle orb
it theory. In this purely Lagrangian method, an approximate solution of the
Newtonian equations of the motion of stars is obtained using a general tec
hnique based upon the perturbation method. In the second order of Lindblad'
s epicyclic theory, expressions are found for the unperturbed motions of st
ars in a stationary system with an axially symmetric mass distribution. The
n, expressions are found for the perturbed motions of stars when the small
non-axisymmetric gravity perturbation is additionally taken into account. T
he perturbed terms are obtained as second-order oscillations. To describe t
he ordered behaviour of a medium near its quasi-equilibrium state, these eq
uations for the trajectories of stars are used to obtain the dispersion rel
ation that connects the frequency of excited collective oscillations with t
he wavenumber throughout the disc, including resonant regions. Using the di
spersion relation, a new class of gradient microinstabilities of a non-unif
ormly rotating disc inherent in an inhomogeneous system is discussed. The L
andau mechanism of excitation of spiral density waves works at the corotati
on resonance between stars and hydrodynamically (Jeans) stable perturbation
s (e.g. those produced by a bar-like structure, a spontaneous perturbation
and/or a companion galaxy). A physical aetiology of the gradient microinsta
bilities of collisionless stellar discs is explained. Such instabilities ca
n develop only if the inhomogeneous and non-uniformly rotating disc of star
s is Jeans-stable. Certain astronomical implications of the theory for actu
al galaxies are explored as well. In particular, the development of these i
nstabilities of a stellar disc can result directly in the formation of diff
erent observable structural features, e.g, spiral arms and collisionless dy
namical relaxation of the system on the Hubble time-scale.