Figure 2
From: Regulating heat conduction of complex networks by distributed nodes masses
Influence of the controlling parameter \(\alpha\) and network structure on the total flux J, with averaging over 50 realizations and randomly chosen source nodes. (a) J versus \(\alpha\) for \(N=300\), \(\langle k\rangle =4\) and different p, where the “squares”, “circles” and “triangles” represent the results for the networks with \(p=1, 0.5\) and 0, respectively. (b) Dependence of the maximum flux \(J_{max}\) on the parameter p for \(\alpha =1\). (c) J versus \(\alpha\) for \(N=300\), \(p=1\) for different \(\langle k\rangle\), where the “squares”, “circles” and “triangles’ represent the results for \(\langle k\rangle =4, 6\) and 8, respectively. (d) J versus \(\alpha\) for \(p=1\), \(\langle k\rangle =4\) for different N, where the “squares”, “circles” and “triangles” represent the results for \(N=100, 300\) and 600, respectively.
