Authors:
Francesco Bullo,
Andrew D. Lewis,
Volume: 1, Page 1260 Paper number 4101
Abstract:
This work presents a review of a number of control results for mechanical
systems. The key technical advances derive from the homogeneity properties
of affine connections models for a large class of mechanical systems.
Recent results on nonlinear controllability and on series expansions
are presented in a unified fashion.
Authors:
John Baillieul,
Volume: 1, Page 1266 Paper number 4102
Abstract:
Recent research has shown that for the class of controlled Lagrangian
systems having fewer control inputs than configuration variables, one
may blur the distinction between directly controlled states and the
corresponding input variables in analyzing the response to oscillatory
forcing. Following this approach, stable responses are associated
with local minima of an energy-like quantity which we have called the
averaged potential. Construction of the averaged potential involves
first constructing a reduced Lagrangian to which a Hamiltonian is associated
by means of a restricted Legendre transformation. The Hamiltonian
is time varying, but by simple averaging one obtains a canonical averaged
Hamiltonian from which the averaged potential is immediately determined.
It is also possible to an averaging analysis of the full (unreduced)
system under high-frequency oscillatory forcing. Under suitable symmetry
conditions, the averaged effect of an oscillatory input may also be
studied in terms of a certain em averaged potential which in general
differs from the one obtained for the reduced system. In the present
paper we discuss the differences between these two approaches and the
resulting averaged potentials.
Authors:
Anthony M. Bloch,
Peter E. Crouch,
Darryl D. Holm,
Jerrold E. Marsden,
Volume: 1, Page 1273 Paper number 4103
Abstract:
In this paper we consider the Hamiltonian formulation of the equations
of incompressible ideal fluid flow from the point of view of optimal
control theory. The equations are compared to the finite symmetric
rigid body equations analyzed earlier by the authors. We discuss various
aspects of the Hamiltonian structure of the Euler equations and show
in particular that the optimal control approach leads to a standard
formulation of the Euler equations -- the so-called impulse equations
in their Lagrangian form.
Authors:
J. Alexander Fax,
Richard M. Murray,
Volume: 1, Page 1279 Paper number 4104
Abstract:
In this paper we investigate the optimal control of affine connection
control systems. The formalism of the affine connection can be used
to describe geometrically the dynamics of mechanical systems, including
those with nonholonomic constraints. In the standard variational approach
to such problems, one converts an n-dimensional second-order system
into a 2n-dimensional first-order system, and uses these equations
as constraints on the optimization. An alternative approach, which
we develop in this paper, is to include the system dynamics as second-order
constraints of the optimization, and optimize relative to variations
in the configuration space. Using the affine connection, its associated
tensors, and the notion of covariant differentiation, we show how variations
in the configuration space induce variations in the tangent space.
In this setting, we derive second-order equations have a geometric
formulation parallel to that of the system dynamics. They also specialize
to results found in the literature.
Authors:
Perinkulam S. Krishnaprasad,
Volume: 1, Page 1285 Paper number 4105
Abstract:
The problem of control of rings of satellites is of current interest
driven by applications in telecommunications and space science. The
problem of stability of a ring is the subject of this paper. We use
methods from geometric approaches to hamiltonian systems to treat this
problem.
Authors:
Dmitry V. Zenkov,
Anthony M. Bloch,
Naomi E. Leonard,
Jerrold E. Marsden,
Volume: 1, Page 1289 Paper number 4106
Abstract:
In this paper we show how a generalized matching technique for stabilization
may be applied to the Routhian associated with a low-dimensional nonholonomic
system. The theory is illustrated with a simple model--a unicycle with
rider.
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