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µ = N$_{T}$ , i.e. a single module, so there is no possible combination of attractors. Case 4 has the lowest A of all five cases. The extreme case 5 has a minimum µ = 1 N$_{T}$ , i.e. N = 1, giving the highest A of all five cases. Notice that in case 5 A decreases for K$_{T}$ > 2. This is because even when κ is constant in theory, in practice κ decreases as K$_{T}$ increases, given the fact that if K > N is equivalent in practice to K = N because of fictitious inputs ( N = 1 in this case, see Table A.5 in Appendix A). 

## 4.1.2 Attractor Lengths 

<img src='content_image/318340.jpg'>

The effect of κ on Le seems to be minimal, as the average attractor lengths is very similar for cases 1, 2, and 3, exponentially increasing with K$_{T}$ , as it can be seen in Figure 7. 

The effect of µ on Le is seen in Figure 8. For K ≥ 3, classical RBNs ( µ = 1) have a higher Le 

