Mason's gain formula is a method for finding the transfer function of a linear signal-flow graph. The formula was derived by Samuel Jefferson Mason, whom it is also named after. MGF is an alternate method to finding the transfer function algebraically by labeling each signal, writing down the equation for how that signal depends on other signals, and then solving the multiple equations for the output signal in terms of the input signal. MGF provides a step by step method to obtain the transfer function from a SFG. Often, MGF can be determined by inspection of the SFG. The method can easily handle SFGs with many variables and loops including loops with inner loops. MGF comes up often in the context of control systems and digital filters because control systems and digital filters are often represented by SFGs.
Formula
The gain formula is as follows: where:
Δ = the determinant of the graph.
yin = input-node variable
yout = output-node variable
G = complete gain between yin and yout
N = total number of forward paths between yin and yout
Gk = path gain of the kth forward path between yin and yout
LiLj = product of the loop gains of any two non-touching loops
LiLjLk = product of the loop gains of any three pairwise nontouching loops
Δk = the cofactor value of Δ for the kth forward path, with the loops touching the kth forward path removed. *
Definitions
Path: a continuous set of branches traversed in the direction that they indicate.
Forward path: A path from an input node to an output node in which no node is touched more than once.
Loop: A path that originates and ends on the same node in which no node is touched more than once.
Path gain: the product of the gains of all the branches in the path.
Loop gain: the product of the gains of all the branches in the loop.
Procedure to find the solution
Make a list of all forward paths, and their gains, and label these Gk.
Make a list of all the loops and their gains, and label these Li. Make a list of all pairs of non-touching loops, and the products of their gains. Make a list of all pairwise non-touching loops taken three at a time, then four at a time, and so forth, until there are no more.
Compute the determinant Δ and cofactors Δk.
Apply the formula.
Examples
Circuit containing two-port
The transfer function from Vin to V2 is desired. There is only one forward path: There are three loops:
The signal flow graph has six loops. They are: There is one forward path: The forward path touches all the loops therefore the co-factor And the gain from input to output is
Mason's rule can be stated in a simple matrix form. Assume is the transient matrix of the graph where is the sum transmittance of branches from node m toward node n. Then, the gain from node m to node n of the graph is equal to, where and is the identity matrix. Mason's Rule is also particularly useful for deriving the z-domain transfer function of discrete networks that have inner feedback loops embedded within outer feedback loops. If the discrete network can be drawn as a signal flow graph, then the application of Mason's Rule will give that network's z-domain H transfer function.
Complexity and computational applications
Mason's Rule can grow factorially, because the enumeration of paths in a directed graph grows dramatically. To see this consider the complete directed graph on vertices, having an edge between every pair of vertices. There is a path form to for each of the permutations of the intermediate vertices. Thus Gaussian elimination is more efficient in the general case. Yet Mason's rule characterizes the transfer functions of interconnected systems in a way which is simultaneously algebraic and combinatorial, allowing for general statements and other computations in algebraic systems theory. While numerous inverses occur during Gaussian elimination, Mason's rule naturally collects these into a single quasi-inverse. General form is Where as described above, is a sum of cycle products, each of which typically falls into an ideal. Fractions of this form make a subring of the rational function field. This observation carries over to the noncommutative case, even though Mason's rule itself must then be replaced by Riegle's rule.
