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4.2.2 Temporal control perturbation

Let us see what happens if we introduce a small change in the terminal time $ t^*$ of the optimal trajectory, i.e., let the optimal control act on a little longer or a little shorter time interval. We formalize this as follows: for an arbitrary $ \tau\in\mathbb{R}$ and a small $ \varepsilon >0$ , we consider the perturbed control

$\displaystyle u_\tau(t):=u^*(\min\{t,t^*\}), \qquad t\in[t_0,t^*+\varepsilon \tau]
$

which is illustrated by the thick curves in Figure 4.3 (for the two cases depending on the sign of $ \tau$ ).

Figure: A temporal perturbation
\includegraphics{figures/temporal.eps}

We are interested in the value of the resulting perturbed trajectory $ y$ at the new terminal time $ t^*+\varepsilon \tau$ . For $ \tau>0$ , the first-order Taylor expansion of $ y$ around $ t=t^*$ gives

\begin{displaymath}\begin{split}y(t^*+\varepsilon \tau)&=y^*(t^*)+ \dot y(t^*)\v...
...:y^*(t^*)+\varepsilon \delta(\tau)+o(\varepsilon ). \end{split}\end{displaymath} (4.9)

For $ \tau<0$ , we have $ y(t^*+\varepsilon \tau)=y^*(t^*+\varepsilon \tau)$ and the first-order Taylor expansion of $ y^*$ around $ t=t^*$ gives the same result. The vector $ \varepsilon \delta(\tau)$ describes the infinitesimal (first-order in $ \varepsilon $ ) perturbation of the terminal point. By definition, $ \delta(\tau)$ depends linearly on $ \tau$ . As we vary $ \tau$ over $ \mathbb{R}$ , keeping $ \varepsilon $ fixed, the points $ y^*(t^*)+\varepsilon \delta(\tau)$ form a line through $ y^*(t^*)$ . We denote this line by $ \vec\rho$ ; see Figure 4.4. Every point on $ \vec\rho$ corresponds to a control $ u_\tau$ for some $ \tau$ . On the other hand, the approximation of $ y(t^*+\varepsilon \tau)$ by $ y^*(t^*)+\varepsilon \delta(\tau)$ is valid only in the limit as $ \varepsilon \to 0$ . So, $ \delta(\tau)$ tells us the direction--but not the magnitude--of the terminal point deviation caused by an infinitesimal change in the terminal time. The arrow over $ \rho$ is meant to indicate that points on the line correspond to perturbation directions. Note that we are describing deviations of the terminal point in the $ (x^0,x)$ -space only, ignoring the differences in the terminal times; accordingly, the time axis is not included in the figures.

Figure: The effect of a temporal control perturbation
\includegraphics{figures/rho.eps}


next up previous contents index
Next: 4.2.3 Spatial control perturbation Up: 4.2 Proof of the Previous: 4.2.1 From Lagrange to   Contents   Index
Daniel 2010-12-20