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Implications of change management in public administration

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Revista T<strong>in</strong>erilor Economişti (The Young Economists Journal)<br />

the optimal trajectories <strong>of</strong> our system are the geodesics <strong>in</strong> the framework <strong>of</strong> sub-<br />

Riemannian geometry [3], [5], [6].<br />

2. Control aff<strong>in</strong>e systems<br />

Let us consider the drift less control aff<strong>in</strong>e system (called also distributional<br />

n<br />

system) <strong>in</strong> the space R on the form<br />

with<br />

X<br />

i<br />

,<br />

.<br />

X ( t)<br />

<br />

m<br />

<br />

i1<br />

i<br />

u ( t)<br />

X<br />

i<br />

( x(<br />

t))<br />

i 1,...,<br />

m vector fields <strong>in</strong> R n and the controls u u , u ,..., u ) take<br />

(1)<br />

(<br />

1 2 m<br />

n<br />

values <strong>in</strong> an open subset R . The vector fields X<br />

i<br />

generate a nonholonomic<br />

n<br />

(non<strong>in</strong>tegrable) distribution D R such that the rank <strong>of</strong> D is not necessarily constant.<br />

n<br />

Let x0<br />

and x<br />

1<br />

be two po<strong>in</strong>ts <strong>of</strong> R . An optimal control problem consists <strong>of</strong><br />

f<strong>in</strong>d<strong>in</strong>g those trajectories <strong>of</strong> the distributional system which connect x0<br />

and x<br />

1<br />

, while<br />

m<strong>in</strong>imiz<strong>in</strong>g the cost<br />

m<strong>in</strong><br />

u F ( x(<br />

t),<br />

u(<br />

t))<br />

dt , (2)<br />

(.) I<br />

where F is a positive homogeneous cost on D .<br />

The controlled paths are obta<strong>in</strong>ed by <strong>in</strong>tegrat<strong>in</strong>g the system (1). If D is assumed to be<br />

bracket generat<strong>in</strong>g (i.e. the vector fields <strong>of</strong> D and iterated Lie brackets span the entire<br />

n<br />

R ), by a well-known theorem <strong>of</strong> Chow the system (1) is controllable, that is for any<br />

two po<strong>in</strong>ts x<br />

0<br />

and x<br />

1 there exists an optimal curve which connects these po<strong>in</strong>ts.<br />

1 2<br />

We consider the Lagrangian function <strong>of</strong> the form L F and it results that is<br />

2<br />

2-homogeneous positive function. Necessary conditions for a trajectory to be an<br />

extreme are given by Pontryag<strong>in</strong> Maximum Pr<strong>in</strong>ciple. The Hamiltonian reads as<br />

H(<br />

x,<br />

p,<br />

u)<br />

p,<br />

X L(<br />

x,<br />

u)<br />

, (3)<br />

where p is the momentum variable on the dual space. The maximization conditions with<br />

respect to the control variables u, namely<br />

H( x(<br />

t),<br />

p(<br />

t),<br />

u(<br />

t))<br />

max H(<br />

x(<br />

t),<br />

p(<br />

t),<br />

v)<br />

leads to the equations<br />

H<br />

( x,<br />

p,<br />

u)<br />

0 , (4)<br />

u<br />

and the extreme trajectories satisfy the Hamilton‟s equations<br />

.<br />

H<br />

.<br />

H<br />

x , p .<br />

(5)<br />

p<br />

x<br />

If the equations (4) permit us to f<strong>in</strong>d <strong>in</strong> a unique way u as a smooth function <strong>of</strong> x and p,<br />

then we can write the Hamiltonian system (5) without any dependence on the control.<br />

This nice situation happens always for distributional systems with quadratic cost<br />

.<br />

v<br />

108

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