Sc. Sinha et R. Pandiyan, ANALYSIS OF QUASI-LINEAR DYNAMICAL-SYSTEMS WITH PERIODIC COEFFICIENTSVIA LIAPUNOV-FLOQUET TRANSFORMATION, International journal of non-linear mechanics, 29(5), 1994, pp. 687-702
In this paper, a new analysis technique in the study of general quasil
inear systems with periodically varying parameters is presented. The m
ethod is based on the fact that all quasilinear periodic systems can b
e replaced by similar systems whose linear parts are time-invariant, v
ia the well-known Liapunov-Floquet (L-F) transformation. A general tec
hnique for the computation of the L-F transformation matrices is outli
ned. In this technique, the state vector and the periodic matrix of th
e linear system equations are expanded in terms of the shifted Chebysh
ev polynomials over the principal period. Such an expansion reduces th
e original problem to a set of linear algebraic equations from which t
he state transition matrix can be constructed over the period as an ex
plicit function of time. Application of Floquet theory and use of symb
olic software yields the L-F transformation matrix in a form suitable
for algebraic manipulations. Once the transformation has been applied,
the solution of the resulting system is obtained through an applicati
on of the time-dependent normal form theory. The method is suitable fo
r both numerical and symbolic computations and in some cases approxima
te closed form solutions can be obtained. Two simple examples of quasi
linear periodic systems-namely, a commutative system with quadratic no
nlinearity and a Mathieu equation with cubic non-linearity-are used to
demonstrate the effectiveness of the method. For verification, result
s obtained from the proposed technique are compared with the numerical
solutions computed using a standard Runge-Kutta type algorithm. It is
shown that the present technique is applicable to systems where the p
eriodic matrix does not contain a small parameter, which is not the ca
se with averaging and perturbation procedures. It can also be used eve
n for those systems for which the generating solutions do not exist in
the classical sense.