Self Loop Rule

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3/13/2009
Self Loop Rule
1/4
Self-Loop Rule
Now consider the equation:
b1 = α a1 + β a2 + γ b1
A little dab of algebra allows us to determine the value of
node b1 :
b1 = α a1 + β a2 + γ b1
b1 − γ b1 = α a1 + β a2
(1 − γ ) b1 = α a1 + β a2
b1 =
α
1−γ
a1 +
β
1−γ
a2
The signal flow graph of the first equation is:
γ
b1 = α a1 + β a2 + γ b1
α
a1
Jim Stiles
a2
b1
β
The Univ. of Kansas
Dept. of EECS
3/13/2009
Self Loop Rule
2/4
While the signal flow graph of the second is:
b1 =
α
1−γ
a1 +
β
1−γ
a2
b1
α
1−γ
1−γ
a1
β
a2
These two signal flow graphs are equivalent!
Note the self-loop has been “removed” in the second graph.
Thus, we now have a method for removing self-loops. This
method is rule 3.
Rule 3 – Self-Loop Rule
A self-loop can be eliminate by multiplying all of the
branches “feeding” the self-loop node by 1 (1 − Ssl ) ,
where Ssl is the value of the self loop branch.
For example:
0. 6
0.2
b1 = 0.6 a1 + j 0.4a2 + 0.2b1
b1
a1
a2
j 0.4
Jim Stiles
The Univ. of Kansas
Dept. of EECS
3/13/2009
Self Loop Rule
3/4
can be simplified by eliminating the self-loop. We multiply
both of the two branches feeding the self-loop node by:
1
1
=
= 1.25
1 − Ssl 1 − 0.2
Therefore:
0.6 (1.25 )
b1
a2
a1
j 0.4 (1.25 )
And thus:
0.75
b1 = 0.75 a1 + j 0.5 a2
b1
a2
a1
j 0.5
Or another example:
a1 = 0.06 a1 − j b2
b1 = 0.3 a1
0.06
b1
a1
b2
Jim Stiles
−j
The Univ. of Kansas
0.3
Dept. of EECS
3/13/2009
Self Loop Rule
4/4
becomes after reduction using rule 3:
−j
a1 =
b2
0.94
b1 = 0.3 a1
b1
a1
b2
−j
0.94
0. 3
Q: Wait a minute! I think you forgot something. Shouldn’t
you also divide the 0.3 branch value by 1 − 0.06 = 0.94 ??
A: Nope! The 0.3 branch is exiting the self-loop node a1.
Only incoming branches (e.g., the –j branch) to the selfloop node are modified by the self-loop rule!
Jim Stiles
The Univ. of Kansas
Dept. of EECS
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