## Berichte der Arbeitsgruppe Technomathematik (AGTM Report)

78

Several topological necessary conditions of smooth stabilization in the large have been obtained. In particular, if a smooth single-input nonlinear system is smoothly stabilizable in the large at some point of a connected component of equilibria set, then the connected component is to be an unknoted, unbounded curve.

71

80

68

Elements of the differential topology are used to prove necessary conditions for stabilizability in large by a smooth feedback. Criteria for the smooth feedback stabilizing a smooth nonlinear system locally to have the smooth piecewise smooth extension, which stabilizes the system over a given compact set, have been obtained.

76

75

In this paper noises and disturbances are treated as distributions of some general class. The problem of sensitivity minimization is considered. A design procedure for the construction of Luenberger observers which estimate the state of a system with a given rate of accuracy has been proposed. The design procedure is applied to identify the first derivatives of an oscillating signal. The constraints on a noise and on a sampling which are necessary to estimate the derivatives to a given accuracy have been obtained.

79

Given a proper antistable rational transfer function g, a balanced realization of g is contructed as a matrix representation of the abstract shift realization introduced in Fuhrmann [1976]. The required basis is constructed as a union of sets of polynomials orthogonal with respect to weights given by the square of the absolute values of minimal degree Schmidt vectors of the corresponding Hankel operators. This extends results of Fuhrmann [1991], obtained in the generic case.

74

On the Mróz Model
(1992)

86

We consider two transmission boundary-value problems for the time-harmonic Maxwell equations without displacement currents. For the first problem we use the continuity of the tangential parts of the electric and magnetic fields across material discontinuities as transmission conditions. In the second case the continuity of the tangential components of the electric field E is replaced by the continuity of the normal component of the magnetization B=müH. For this problem existence of solutions is already shown in [6]. If the domains under consideration are not simply connected the solution is not unique. In this paper, we improve the regularity results obtained in [6] and then prove existence and uniqueness theorems for the first problem by extracting its solution out of the set of all solutions of the second problem. Thus we establish a connection between the solutions corresponding to the different transmission boundary conditions.