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Next: 17/1/2003 by Chachra Up: 14/01/2003 by Ajit Shegaonkar Previous: Analyse Rocket Altitude Control

Analyse the following system

A Capacitor(C) and Inductor(L) are connected in series across a battery which provides variable supply voltage ($ e_r$) which varies with the current as given by the following equation. The Capacitor and Inductor are respectively rated at $ \frac{1}{2} $ farad and 1 Henry. Analyse the system for its stability and response. Supply voltage ($ e_r$):-

\begin{displaymath}\begin{array}{ccccccc}
 e_r &=& -3\dot q && && \vert{\dot q}\...
...\dot q > 1 \\  
 &=& 3\dot q + 6 && && \dot q < -1
 \end{array}\end{displaymath} (1.6)

The system can be mathematically expressed as :-

$\displaystyle L{\ddot q} + e_r + \frac{q}{C} = 0$ (1.7)

For the state space representation, state space variables are:-

\begin{displaymath}\begin{array}{ccccccc}
 x_1 &=& q \\  
 x_2 &=& \dot q 
 \end{array}\end{displaymath} (1.8)

For $ \vert\dot q\vert \leq 1$ i.e. $ \vert x_2\vert \leq 1$, we have,

$\displaystyle \dot x_1$ $\displaystyle = x_2$ (1.9)
$\displaystyle \dot x_2$ $\displaystyle = -2x_1 + 3x_2$ (1.10)

and the state space representation is :-

$\displaystyle \begin{pmatrix}
 \dot x_1 \\  \dot x_2
 \end{pmatrix}
 =
 \begin{...
...matrix}
 x_1 \\  x_2
 \end{pmatrix}
 +
 \begin{pmatrix}
 0 \\  0
 \end{pmatrix}$ (1.11)

the equillibrium point is (0,0), the eigenvalues are $ 1 , 2$ and hence the equillibrium point is an unstable node. For $ \dot q > 1$ i.e. $ x_2 > 1$, we have,

$\displaystyle \dot x_1$ $\displaystyle = x_2$ (1.12)
$\displaystyle \dot x_2$ $\displaystyle = -2x_1 - 3x_2 + 6$ (1.13)

and the state space representation is :-

$\displaystyle \begin{pmatrix}
 \dot x_1 \\  \dot x_2
 \end{pmatrix}
 =
 \begin{...
...matrix}
 x_1 \\  x_2
 \end{pmatrix}
 +
 \begin{pmatrix}
 0 \\  6
 \end{pmatrix}$ (1.14)

the equillibrium point is (3,0), the eigenvalues are $ -1 , -2$ and hence the equillibrium point is a stable node. But this equillibrium point does not lie in the range over which the function is defined, hence the equillibrium point is a virtual equillibrium point and the trajectories will never converge to this stable node. For $ \dot q < -1$ i.e. $ x_2 < -1$, we have,

$\displaystyle \dot x_1$ $\displaystyle = x_2$ (1.15)
$\displaystyle \dot x_2$ $\displaystyle = -2x_1 - 3x_2 - 6$ (1.16)

and the state space representation is :-

$\displaystyle \begin{pmatrix}
 \dot x_1 \\  \dot x_2
 \end{pmatrix}
 =
 \begin{...
...atrix}
 x_1 \\  x_2
 \end{pmatrix}
 +
 \begin{pmatrix}
 0 \\  -6
 \end{pmatrix}$ (1.17)

the equillibrium point is (-3,0), the eigenvalues are $ -1 , -2$ and hence the equillibrium point is a stable node. But this equillibrium point does not lie in the range over which the function is defined, hence the equillibrium point is a virtual equillibrium point and the trajectories will never converge to this stable node. The solution trajectory (phase portrait) is given below : Trajectory2
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Next: 17/1/2003 by Chachra Up: 14/01/2003 by Ajit Shegaonkar Previous: Analyse Rocket Altitude Control
Vishal Mahulkar (98D10043) 2003-02-14