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Control Engineering Lecture #2 Lecture #2 9 th Sep,2009 9 th Sep,2009.

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Presentation on theme: "Control Engineering Lecture #2 Lecture #2 9 th Sep,2009 9 th Sep,2009."— Presentation transcript:

1 Control Engineering Lecture #2 Lecture #2 9 th Sep,2009 9 th Sep,2009

2 Models of Physical Systems  Two types of methods used in system modeling:  (i) Experimental method  (ii) Mathematical method  Design of engineering systems by trying and error versus design by using mathematical models.  Mathematical model gives the mathematical relationships relating the output of a system to its input.

3 Models of Electrical Circuits  Resistance circuit: v(t) = i(t) R  Inductance circuit: 

4 Models of Electrical Circuits  Capacitance circuit:

5 Models of Electrical Circuits  Kirchhoff’ s voltage law: The algebraic sum of voltages around any closed loop in an electrical circuit is zero. The algebraic sum of voltages around any closed loop in an electrical circuit is zero.  Kirchhoff’ s current law: The algebraic sum of currents into any junction in an electrical circuit is zero. The algebraic sum of currents into any junction in an electrical circuit is zero.

6 Models of Electrical Circuits  Example:

7 Transfer Function  Suppose we have a constant-coefficient linear differential equation with input f(t) and output x(t).  After Laplace transform we have X(s)=G(s)F(s)  We call G(s) the transfer function.

8 An Example An Example  Linear differential equation  The Laplace transform is:

9 An Example An Example  Differential equation:

10 Characteristic Equation Characteristic Equation

11 Block Diagram and Signal Flow Graphs  Block diagram:  Signal flow graph is used to denote graphically the transfer function relationship:

12  System interconnections  Series interconnection Y(s)=H(s)U(s) where H(s)=H 1 (s)H 2 (s). Y(s)=H(s)U(s) where H(s)=H 1 (s)H 2 (s).  Parallel interconnection Y(s)=H(s)U(s) where H(s)=H 1 (s)+H 2 (s). Y(s)=H(s)U(s) where H(s)=H 1 (s)+H 2 (s).

13  Feedback interconnection

14 An Example An Example

15  Parallel interconnection:

16 Another example :

17 Mason’s Gain Formula  Motivation: How to obtain the equivalent Transfer Function? Ans: Mason’s formula

18 Mason’s Gain Formula Mason’s Gain Formula  This gives a procedure that allows us to find the transfer function, by inspection of either a block diagram or a signal flow graph.  Source Node: signals flow away from the node.  Sink node: signals flow only toward the node.  Path: continuous connection of branches from one node to another with all arrows in the same direction.  Forward path: is a path that connects a source to a sink in which no node is encountered more than once.

19  Loop: a closed path in which no node is encountered more than once. Source node cannot be part of a loop.  Path gain: product of the transfer functions of all branches that form the path.  Loop gain: products of the transfer functions of all branches that form the loop.  Nontouching: two loops are non-touching if these loops have no nodes in common.

20 An Example An Example  Loop 1 (-G 2 H 1 ) and loop 2 (-G 4 H 2 ) are not touching.  Two forward paths:

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23 More Examples:

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25 Another Example:


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