Control Systems
Modeling a system
Series RC circuit
Let \(I(t)\) = output (current), \(v(t)\) = input (applied voltage).
Time-domain equation (series resistor \(R\) and capacitor \(C\)):
Assuming zero initial conditions, take Laplace transform (differentiate both sides of the time-domain equation for simplification):
Transfer function from input voltage to current:
Two-node/two-branch network
KVL in Laplace transform domain
Solve using Cramer's rule. Let the coefficient matrix be \(A(s)\) and \(\Delta(s)=\det A(s)\).
Transfer function is given by
Here, \(\det A_1(s)\) is determinant of matrix formed by replacing first column of \(A\) with \(\begin{pmatrix}V(s)\\0\end{pmatrix}\), \(\det A_2(s)\) is determinant of matrix formed by replacing second column of \(A\) with \(\begin{pmatrix}V(s)\\0\end{pmatrix}\).
Mechanical damper system
Damper equation:
Newton’s law for \(m_2\) gives:
Newton's law for \(m_1\) gives:
The equations can be written in a matrix form:
Laplace transform form of the equation is:
Using Cramer’s rule, we can find:
Equivalent electric circuit for mechanical damper system
In the damper system, we have these components:
To convert it into an equivalent electrical circuit, we use the following relations for electrical component
Force–current analogy
Resistor
Inductor
Capacitor
Let \(\frac{dx}{dt} = v\). Two equations \(\Rightarrow\) Two nodes.
Force–voltage analogy
Resistor
Inductor
Capacitor
Let \(\frac{dx}{dt} = i\). Two equations \(\Rightarrow\) Two loops.
Scanned notes
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Author
Anurag Gupta is an M.S. graduate in Electrical and Computer Engineering from Cornell University. He also holds an M.Tech degree in Systems and Control Engineering and a B.Tech degree in Electrical Engineering from the Indian Institute of Technology, Bombay.
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