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Control System Engineering
Kuntumal Sagar M.
B.TECH (E.E)
UID-U41000000484
Email: skuntmal@yahoo.com
TOPIC
Signal Flow Graphs
Outline
• Introduction to Signal Flow Graphs
– Definitions
– Terminologies
– Example
• Mason’s Gain Formula
– Example
Introduction
3
• A signal-flow graph consists of a network in which nodes
are connected by directed branches.
• It depicts the flow of signals from one point of a system
to another and gives the relationships among the signals.
Fundamentals of Signal Flow Graphs
• Consider a simple equation below and draw its signal flow graph:
• The signal flow graph of the equation is shown below;
• Every variable in a signal flow graph is designed by a Node.
• Every transmission function in a signal flow graph is designed by a
Branch.
• Branches are always unidirectional.
• The arrow in the branch denotes the direction of the signal flow.
axy 
x ya
Terminologies
• An input node or source contain only the outgoing branches. i.e., X1
• An output node or sink contain only the incoming branches. i.e., X4
• A path is a continuous, unidirectional succession of branches along which no
node is passed more than ones. i.e.,
• A forward path is a path from the input node to the output node. i.e.,
X1 to X2 to X3 to X4 , and X1 to X2 to X4 , are forward paths.
• A feedback path or feedback loop is a path which originates and terminates on
the same node. i.e.; X2 to X3 and back to X2 is a feedback path.
X1 to X2 to X3 to X4 X1 to X2 to X4 X2 to X3 to X4
Terminologies
• A self-loop is a feedback loop consisting of a single branch. i.e.; A33 is a self
loop.
• The gain of a branch is the transmission function of that branch.
• The path gain is the product of branch gains encountered in traversing a path.
i.e. the gain of forwards path X1 to X2 to X3 to X4 is A21A32A43
• The loop gain is the product of the branch gains of the loop. i.e., the loop gain
of the feedback loop from X2 to X3 and back to X2 is A32A23.
• Two loops, paths, or loop and a path are said to be non-touching if they have
no nodes in common.
Mason’s Rule (Mason, 1953)
• The block diagram reduction technique requires successive
application of fundamental relationships in order to arrive at the
system transfer function.
• On the other hand, Mason’s rule for reducing a signal-flow graph
to a single transfer function requires the application of one
formula.
• The formula was derived by S. J. Mason when he related the
signal-flow graph to the simultaneous equations that can be
written from the graph.
Mason’s Rule:
• The transfer function T, of a system represented by a signal-flow graph is;
Where,
n = number of forward paths.
Pi = the i th forward-path gain.
∆ = Determinant of the system
∆i = Determinant of the ith forward path
• ∆ is called the signal flow graph determinant or characteristic function. Since
∆=0 is the system characteristic equation.




 
n
i
iiP
sR
sC
T 1
)(
)(
Mason’s Rule:
∆ = 1- (sum of all individual loop transmittance) + (sum of the products of
loop transmittance of all possible pairs of Non Touching loops) – (sum of
the products of loop transmittance of Triple of Non Touching loop) + …
∆i = Calculate ∆ for ith path
=1- [loop transmittance of single Non Touching loops with forward path]
+ [loop transmittance of pair of Non Touching loops withforward path]




 
n
i
iiP
sR
sC
T 1
)(
)(
Systematic approach
1. Calculate forward path gain Pi for each forward
path i.
2. Calculate all loop transfer functions
3. Consider non-touching loops 2 at a time
4. Consider non-touching loops 3 at a time
5. etc
6. Calculate Δ from steps 2,3,4 and 5
7. Calculate Δi as portion of Δ not touching forward
path i
10


 2211
)(
)( PP
sR
sC
TTherefore,
24313242121411 HGGGLHGGGLHGGL  ,,
There are three feedback loops
Example#1:
Apply Mason’s Rule to calculate the transfer function of the system
represented by following Signal Flow Graph
∆ = 1- (sum of all individual loop gains)
There are no non-touching loops, therefore
 3211 LLL 
 243124211411 HGGGHGGGHGG 
Example#1:
Apply Mason’s Rule to calculate the transfer function of the system
represented by following Signal Flow Graph
∆1 = 1- (sum of all individual loop gains)+...
Eliminate forward path-1
∆1 = 1
∆2 = 1- (sum of all individual loop gains)+...
Eliminate forward path-2
∆2 = 1
Example#1:
Apply Mason’s Rule to calculate the transfer function of the system
represented by following Signal Flow Graph
Example#1: Continue
THANK YOU

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Signal flow graph

  • 1. Control System Engineering Kuntumal Sagar M. B.TECH (E.E) UID-U41000000484 Email: skuntmal@yahoo.com TOPIC Signal Flow Graphs
  • 2. Outline • Introduction to Signal Flow Graphs – Definitions – Terminologies – Example • Mason’s Gain Formula – Example
  • 3. Introduction 3 • A signal-flow graph consists of a network in which nodes are connected by directed branches. • It depicts the flow of signals from one point of a system to another and gives the relationships among the signals.
  • 4. Fundamentals of Signal Flow Graphs • Consider a simple equation below and draw its signal flow graph: • The signal flow graph of the equation is shown below; • Every variable in a signal flow graph is designed by a Node. • Every transmission function in a signal flow graph is designed by a Branch. • Branches are always unidirectional. • The arrow in the branch denotes the direction of the signal flow. axy  x ya
  • 5. Terminologies • An input node or source contain only the outgoing branches. i.e., X1 • An output node or sink contain only the incoming branches. i.e., X4 • A path is a continuous, unidirectional succession of branches along which no node is passed more than ones. i.e., • A forward path is a path from the input node to the output node. i.e., X1 to X2 to X3 to X4 , and X1 to X2 to X4 , are forward paths. • A feedback path or feedback loop is a path which originates and terminates on the same node. i.e.; X2 to X3 and back to X2 is a feedback path. X1 to X2 to X3 to X4 X1 to X2 to X4 X2 to X3 to X4
  • 6. Terminologies • A self-loop is a feedback loop consisting of a single branch. i.e.; A33 is a self loop. • The gain of a branch is the transmission function of that branch. • The path gain is the product of branch gains encountered in traversing a path. i.e. the gain of forwards path X1 to X2 to X3 to X4 is A21A32A43 • The loop gain is the product of the branch gains of the loop. i.e., the loop gain of the feedback loop from X2 to X3 and back to X2 is A32A23. • Two loops, paths, or loop and a path are said to be non-touching if they have no nodes in common.
  • 7. Mason’s Rule (Mason, 1953) • The block diagram reduction technique requires successive application of fundamental relationships in order to arrive at the system transfer function. • On the other hand, Mason’s rule for reducing a signal-flow graph to a single transfer function requires the application of one formula. • The formula was derived by S. J. Mason when he related the signal-flow graph to the simultaneous equations that can be written from the graph.
  • 8. Mason’s Rule: • The transfer function T, of a system represented by a signal-flow graph is; Where, n = number of forward paths. Pi = the i th forward-path gain. ∆ = Determinant of the system ∆i = Determinant of the ith forward path • ∆ is called the signal flow graph determinant or characteristic function. Since ∆=0 is the system characteristic equation.       n i iiP sR sC T 1 )( )(
  • 9. Mason’s Rule: ∆ = 1- (sum of all individual loop transmittance) + (sum of the products of loop transmittance of all possible pairs of Non Touching loops) – (sum of the products of loop transmittance of Triple of Non Touching loop) + … ∆i = Calculate ∆ for ith path =1- [loop transmittance of single Non Touching loops with forward path] + [loop transmittance of pair of Non Touching loops withforward path]       n i iiP sR sC T 1 )( )(
  • 10. Systematic approach 1. Calculate forward path gain Pi for each forward path i. 2. Calculate all loop transfer functions 3. Consider non-touching loops 2 at a time 4. Consider non-touching loops 3 at a time 5. etc 6. Calculate Δ from steps 2,3,4 and 5 7. Calculate Δi as portion of Δ not touching forward path i 10
  • 11.    2211 )( )( PP sR sC TTherefore, 24313242121411 HGGGLHGGGLHGGL  ,, There are three feedback loops Example#1: Apply Mason’s Rule to calculate the transfer function of the system represented by following Signal Flow Graph
  • 12. ∆ = 1- (sum of all individual loop gains) There are no non-touching loops, therefore  3211 LLL   243124211411 HGGGHGGGHGG  Example#1: Apply Mason’s Rule to calculate the transfer function of the system represented by following Signal Flow Graph
  • 13. ∆1 = 1- (sum of all individual loop gains)+... Eliminate forward path-1 ∆1 = 1 ∆2 = 1- (sum of all individual loop gains)+... Eliminate forward path-2 ∆2 = 1 Example#1: Apply Mason’s Rule to calculate the transfer function of the system represented by following Signal Flow Graph