Observe that the attractor has retained a semblance of the original function. It curves both upward and downward over its single valued domain. There appears to be no region of gain where the attractor is 0. The locations of the bifurcations are different from both the logistic and sinusoidal functions. The general outline of the region of chaos is distinct from the other two functions. Again though, the general appearance is similar to that of the others.